# Difference: HDBSPublicResults (1 vs. 3)

#### Revision 32019-08-14 - AndreasHoecker

Line: 1 to 1

 META TOPICPARENT name="WebHome"
<!--
Set ALLOWTOPICCHANGE   = GianlucaPicco, MaurizioColautti, atlas-phys-conveners, atlas-physics-coordinators, atlas-mgt-members, atlas-phys-office-developers

Line: 7 to 7

<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE FOLLOWING LINES                      -->
<!-- **************************************************************************** -->

<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE PREVIOUS LINES                      -->
<!-- **************************************************************************** -->
>
>

# Higgs and Diboson Searches

Changed:
<
<
>
>
Contact: ATLAS HDBS Working Group Conveners
Deleted:
<
<

This page gives access to the publicly-available studies and results from the ATLAS Higgs and Diboson Searches (HDBS) Working Group. Only this material is approved for showing in public by speakers from ATLAS or other collaborations.

#### Revision 22019-05-14 - GianlucaPicco

Line: 1 to 1

 META TOPICPARENT name="WebHome"
<!--
Set ALLOWTOPICCHANGE   = GianlucaPicco, MaurizioColautti, atlas-phys-conveners, atlas-physics-coordinators, atlas-mgt-members, atlas-phys-office-developers

-->

<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE FOLLOWING LINES                      -->
<!-- **************************************************************************** -->

Changed: <
<
<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE PREVIOUS LINES                      -->
<!-- **************************************************************************** -->
>
>
<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE PREVIOUS LINES                      -->
<!-- **************************************************************************** -->

Deleted:
<
<

## Higgs and Diboson Searches

Line: 34 to 29
Select the desired keywords to filter the results.
Selections within a section row are combined with a logical OR, while selections among different section rows are combined with a logical AND.
<!-- ***********************INCLUDE FILTER SECTION************************************* -->
Changed:
<
<
DiHiggs searches with the ATLAS detector','pubShortTitle':'HH generator simulation studies','refCode':'ATL-PHYS-PUB-2019-007','abstract':'','cdsLink':'https://cds.cern.ch/record/2665057','journal':'Preliminary','journalSub':'28-FEB-19','ecm':'13','luminosity':'','keywords':'','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2019-007@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2019-007@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'3444','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=3444','shortTitle':'HProspects HH and self-coupling for YR','fullTitle':'Measurement prospects of the pair production and self-coupling of the Higgs boson with the ATLAS experiment at the HL-LHC','pubShortTitle':'HH and self-coupling prospects for HL-LHC','refCode':'ATL-PHYS-PUB-2018-053','abstract':'','cdsLink':'https://cds.cern.ch/record/2652727','journal':'Preliminary','journalSub':'24-DEC-18','ecm':'14','luminosity':'','keywords':'14 TeV,HL-LHC,Higgs sector upgrade studies,Di-Higgs production,Higgs to tautau,Higgs to bb,Higgs to 2 photons,High luminosity upgrade studies,Statistical combination,Di-Higgs,Di-photon,b-jets,Photons,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-053@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-053@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'3643','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=3643','shortTitle':'HBSM h->aa summary plots','fullTitle':'h->aa summary plots','pubShortTitle':'h->aa summary plots','refCode':'ATL-PHYS-PUB-2018-045','abstract':'','cdsLink':'','journal':'Preliminary','journalSub':'10-DEC-18','ecm':'13','luminosity':'','keywords':'','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-045@linkEnd@Documents@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-045@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'3446','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=3446','shortTitle':'HProspects H/A->tautau for YR','fullTitle':'Prospects for the search for additional Higgs bosons in the ditau final state with the ATLAS detector at HL-LHC','pubShortTitle':'H/A->tautau prospects at HL-LHC','refCode':'ATL-PHYS-PUB-2018-050','abstract':'','cdsLink':'','journal':'Preliminary','journalSub':'19-DEC-18','ecm':'14','luminosity':'','keywords':'Taus,14 TeV,HL-LHC,Higgs sector upgrade studies,BSM Higgs searches,Higgs to tautau,High luminosity upgrade studies,BSM search','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-050@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-050@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'3543','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=3543','shortTitle':'Prospects of HH->4b Resonance Search','fullTitle':'Search prospects for resonant Higgs boson pair production in the $b\\bar{b}b\\bar{b}$ final state with large-radius jets from $pp$ collisions at the HL-LHC','pubShortTitle':'Prospects of HH->4b Resonance Search','refCode':'ATL-PHYS-PUB-2018-028','abstract':'','cdsLink':'https://cds.cern.ch/record/2646889','journal':'Preliminary','journalSub':'13-NOV-18','ecm':'14','luminosity':'','keywords':'14 TeV,HL-LHC,Exotic physics upgrade studies,Strong gravity,BSM resonance,High luminosity upgrade studies,BSM search,Di-Higgs,Boosted,b-jets,All hadronic','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-028@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-028@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'3283','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=3283','shortTitle':'Prospects of VV Search and Measurement','fullTitle':'HL-LHC prospects for Diboson resonance searches and electroweak WW/WZ production in association with a high-mass dijet system in the semileptonic final states','pubShortTitle':'Prospects of VV Search and Measurement','refCode':'ATL-PHYS-PUB-2018-022','abstract':'','cdsLink':'https://cds.cern.ch/record/2645269','journal':'Preliminary','journalSub':'30-OCT-18','ecm':'14','luminosity':'','keywords':'High luminosity upgrade studies,HL-LHC,Exotic physics upgrade studies','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-022@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2018-022@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'2325','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=2325','shortTitle':'HProspects HH to bbgamgam','fullTitle':'Study of the discovery potential of double Higgs production with the channel H(->bb)H(->gamgam) with the ATLAS experiment at HL-LHC','pubShortTitle':'HH to bb gamma gamma prospects HL-LHC','refCode':'ATL-PHYS-PUB-2017-001','abstract':'','cdsLink':'https://cds.cern.ch/record/2243387','journal':'Preliminary','journalSub':'27-JAN-17','ecm':'14','luminosity':'','keywords':'Photons,14 TeV,HL-LHC,Higgs sector upgrade studies,Di-Higgs production,Higgs to bb,Higgs to 2 photons,High luminosity upgrade studies,Di-Higgs,Higgs,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2017-001/@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2017-001/@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'683','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=683','shortTitle':'HP BSM Prospects','fullTitle':'Updated Sensitivity to New Phenomena via Higgs Couplings with the ATLAS Detector at a High-Luminosity LHC','pubShortTitle':'BSM h/A/H prospects HL-LHC','refCode':'ATL-PHYS-PUB-2014-017','abstract':'','cdsLink':'https://cds.cern.ch/record/1956711','journal':'Preliminary','journalSub':'20-OCT-14','ecm':'14','luminosity':'','keywords':'14 TeV,HL-LHC,Exotic physics upgrade studies,SUSY upgrade studies,Higgs sector upgrade studies,BSM Higgs searches,High luminosity upgrade studies,Statistical combination,Higgs','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2014-017@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2014-017@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'86','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=86','shortTitle':'HP - HSG6 2HDM interpretation','fullTitle':'Sensitivity to New Phenomena via Higgs Couplings with the ATLAS Detector at a High-Luminosity LHC','pubShortTitle':'Search BSM combination 2HDM prospects HL-LHC','refCode':'ATL-PHYS-PUB-2013-015','abstract':'','cdsLink':'https://cds.cern.ch/record/1611189','journal':'Preliminary','journalSub':'10-OCT-13','ecm':'14','luminosity':'','keywords':'14 TeV,HL-LHC,Exotic physics upgrade studies,Higgs sector upgrade studies,NMSSM,BSM Higgs searches,High luminosity upgrade studies,BSM reinterpretation,Statistical combination','links':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2013-015/@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2013-015/@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'152','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=152','shortTitle':'Higgs self-coupling measurements','fullTitle':'Studies of the ATLAS potential for Higgs self-coupling measurements at a High Luminosity LHC','pubShortTitle':'Higgs self couplings prospects HL-LHC','refCode':'ATL-PHYS-PUB-2013-001','abstract':'','cdsLink':'https://cds.cern.ch/record/1507263','journal':'Preliminary','journalSub':'18-JAN-13','ecm':'14','luminosity':'','keywords':'14 TeV,Di-Higgs production,High luminosity upgrade studies','links':'@linkBegin@http://cdsweb.cern.ch/record/1507263@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@http://cdsweb.cern.ch/record/1507263@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'217','internalLink':'https://glance.cern.ch/atlas/analysis/pubnotes/details.php?id=217','shortTitle':'Discovery Potential of A/H->tau tau->lh','fullTitle':'Discovery Potential of A/H->tau tau->lh in ATLAS','pubShortTitle':'Search BSM H/A -> tau tau prospects','refCode':'ATL-PHYS-PUB-2010-011','abstract':'','cdsLink':'','journal':'Preliminary','journalSub':'','ecm':'14','luminosity':'','keywords':'14 TeV,BSM Higgs searches,Higgs to tautau,High luminosity upgrade studies,Taus','links':'@linkBegin@http://cds.cern.ch/record/1279115@linkEnd@Documents@descriptionEnd@','run':'0','finalPubRef':'@linkBegin@http://cds.cern.ch/record/1279115@linkEnd@Figures@descriptionEnd@','publicationType':'PUB','pressStatement':''},{'publicationId':'11765','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=11765','shortTitle':'HComb combination 2015+2016/7','fullTitle':'Combined measurements of Higgs boson production and decay using up to $80$ fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=$ 13 TeV collected with the ATLAS experiment','pubShortTitle':'h(125) combination cross-sections, couplings','refCode':'HIGG-2018-57','abstract':'Combined measurements of Higgs boson production cross sections and branching fractions are presented. The combination is based on the analyses of the Higgs boson decay modes $H \\rightarrow \\gamma\\gamma$, $ZZ^\\ast$, $WW^\\ast$, $\\tau\\tau$, $b\\bar{b}$, $\\mu\\mu$, searches for decays into invisible final states, and on measurements of off-shell Higgs boson production. Up to $79.8$ fb$^{-1}$ of proton-proton collision data collected at $\\sqrt{s}=$ 13 TeV with the ATLAS detector are used. Results are presented for the gluon-gluon fusion and vector-boson fusion processes, and for associated production with vector bosons or top-quarks. The global signal strength is determined to be $\\mu = 1.11^{+0.09}_{-0.08}$. The combined measurement yields an observed (expected) significance for the vector-boson fusion production process of $6.5\\sigma$ ($5.3\\sigma$). Measurements in kinematic regions defined within the simplified template cross section framework are also shown. The results are interpreted in terms of modifiers applied to the Standard Model couplings of the Higgs boson to other particles, and are used to set exclusion limits on parameters in two-Higgs-doublet models and in the simplified Minimal Supersymmetric Standard Model. No significant deviations from Standard Model predictions are observed.','cdsLink':'','journal':'Phys. Rev. D','journalSub':'06-SEP-19','ecm':'13','luminosity':'80 fb-1','keywords':'13 TeV,kappa,Coupling measurements,H(125) measurements,Statistical combination','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2018-57@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1909.02845@linkEnd@1909.02845@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1752936@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'10587','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10587','shortTitle':'UEH - Displaced lepton jets','fullTitle':'Search for light long-lived neutral particles produced in $pp$ collisions at $\\sqrt{s } =$ 13 TeV and decaying into collimated leptons or light hadrons with the ATLAS detector','pubShortTitle':'Search for displaced lepton-jets','refCode':'EXOT-2017-28','abstract':'Several models of physics beyond the Standard Model predict the existence of dark photons, light neutral particles decaying into collimated leptons or light hadrons. This paper presents a search for long-lived dark photons produced from the decay of a Higgs boson or a heavy scalar boson and decaying into displaced collimated Standard Model fermions. The search uses data corresponding to an integrated luminosity of 36.1 fb$^{-1}$ collected in proton-proton collisions at $\\sqrt{s } =$ 13 TeV recorded in 2015-2016 with the ATLAS detector at the Large Hadron Collider. The observed number of events is consistent with the expected background, and limits on the production cross section times branching fraction as a function of the proper decay length of the dark photon are reported. A cross section times branching fraction above 4 pb is excluded for a Higgs boson decaying into two dark photons for dark-photon decay lengths between 1.5 mm and 307 mm.','cdsLink':'','journal':'EPJC','journalSub':'03-SEP-19','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Lepton-jets,Other new particle searches,BSM resonance,MVA / machine learning,Long-lived massive particles,Long-lived massive particle,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-28@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1909.01246@linkEnd@1909.01246@descriptionEnd@,@linkBegin@http://inspirehep.net/record/1752519@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/ins1752519?version=1@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'11946','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=11946','shortTitle':'HBSM hh to bbWW 2015-2018','fullTitle':'Search for non-resonant Higgs boson pair production in the $bb\\ell\\nu\\ell\\nu$ final state with the ATLAS detector in $pp$ collisions at $\\sqrt{s } = 13$ TeV','pubShortTitle':'HH->bb WW-> bblvlv','refCode':'HDBS-2018-33','abstract':'A search for non-resonant Higgs boson pair production, as predicted by the Standard Model, is presented, where one of the Higgs bosons decays via the $H\\rightarrow bb$ channel and the other via one of the $H \\rightarrow WW^*/ZZ^*/\\tau\\tau$ channels. The analysis selection requires events to have at least two $b$-tagged jets and exactly two leptons (electrons or muons) with opposite electric charge in the final state. Candidate events consistent with Higgs boson pair production are selected using a multi-class neural network discriminant. The analysis uses 139 fb$^{-1}$ of $pp$ collision data recorded at a centre-of-mass energy of 13 TeV, by the ATLAS detector at the Large Hadron Collider. An observed (expected) upper limit of 1.2 ($0.9^{+0.4}_{-0.3}$) pb is set on the non-resonant Higgs boson pair production cross-section at 95% confidence level, which is equivalent to 40 ($29^{+14}_{-9}$) times the value predicted in the Standard Model.','cdsLink':'','journal':'PLB','journalSub':'19-AUG-19','ecm':'13','luminosity':'139 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to bb,Higgs to WW,BSM search,Di-Higgs,WW,b-jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HDBS-2018-33@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1908.06765@linkEnd@1908.06765@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1750030@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'9823','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9823','shortTitle':'Hbb bH H to bb 2015+2016','fullTitle':'Search for heavy neutral Higgs bosons produced in association with $b$-quarks and decaying to $b$-quarks at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM bH H->bb','refCode':'HIGG-2016-32','abstract':'A search for heavy neutral Higgs bosons produced in association with one or two $b$-quarks and decaying to $b$-quark pairs is presented using 27.8 fb$^{-1}$ of $\\sqrt{s}=13$ TeV proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross-section times its branching ratio to $b\\bar{b}$ are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the Minimal Supersymmetric Standard Model.','cdsLink':'','journal':'PRD','journalSub':'05-JUL-19','ecm':'13','luminosity':'27.8 fb-1','keywords':'13 TeV,BSM Higgs searches,bH production,Higgs to bb,BSM search,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-32@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1907.02749@linkEnd@1907.02749@descriptionEnd@,@linkBegin@http://inspirehep.net/record/1742697@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'11745','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=11745','shortTitle':'DBL - VV all-hadronic search 2018','fullTitle':'Search for diboson resonances in hadronic final states in 139 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Diboson resonance search in the all-hadronic final state','refCode':'HDBS-2018-31','abstract':'Narrow resonances decaying into $WW$, $WZ$ or $ZZ$ boson pairs are searched for in 139 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of $\\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider from 2015 to 2018. The diboson system is reconstructed using pairs of high transverse momentum, large-radius jets. These jets are built from a combination of calorimeter- and tracker-inputs compatible with the hadronic decay of a boosted $W$ or $Z$ boson, using jet mass and substructure properties. The search is performed for diboson resonances with masses greater than 1.3 TeV. No significant deviations from the background expectations are observed. Exclusion limits at the 95% confidence level are set on the production cross-section times branching ratio into dibosons for resonances in a range of theories beyond the Standard Model, with the highest excluded mass of a new gauge boson at 3.8 TeV in the context of mass-degenerate resonances that couple predominantly to gauge bosons.','cdsLink':'','journal':'JHEP','journalSub':'20-JUN-19','ecm':'13','luminosity':'139 fb-1','keywords':'13 TeV,BSM resonance,BSM search,ZZ,WZ,WW,Boosted,All hadronic,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HDBS-2018-31@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1906.08589@linkEnd@1906.08589@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1740685@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'10573','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10573','shortTitle':'LPX - Excited Leptons','fullTitle':'Search for excited electrons singly produced in proton-proton collisions at $\\sqrt{s } = 13$ TeV with the ATLAS experiment at the LHC','pubShortTitle':'Search for excited electrons','refCode':'EXOT-2017-22','abstract':'A search for excited electrons produced in $pp$ collisions at $\\sqrt{s } = 13$ TeV via a contact interaction $q\\bar{q} \\to ee^*$ is presented. The search uses 36.1 fb$^{-1}$ of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron via a contact interaction into an electron and a pair of quarks ($eq\\bar{q}$) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a $W$ boson ($\\nu W$) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying $W$ boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the $pp \\to ee^* \\to eeq\\bar{q}$ and $pp \\to ee^* \\to e\\nu W$ production cross sections as a function of the excited electron mass $m_{e^*}$ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter $\\Lambda$ of the model as a function of $m_{e^*}$. For $m_{e^*} < 0.5$ TeV, the lower bound for $\\Lambda$ is 11 TeV. In the special case of $m_{e^* } = \\Lambda$, the values of $m_{e^*} < 4.8$ TeV are excluded. The presented limits on $\\Lambda$ are more stringent than those obtained in previous searches.','cdsLink':'','journal':'EPJC','journalSub':'07-JUN-19','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Compositeness,Contact interactions,BSM resonance,BSM search,2 jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-22@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1906.03204@linkEnd@1906.03204@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1738845@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/ins1738845?version=1@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'11825','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=11825','shortTitle':'HBSM hh combination 2015+2016','fullTitle':'Combination of searches for Higgs boson pairs in $pp$ collisions at  $\\sqrt{s } =$13 TeV with the ATLAS detector','pubShortTitle':'Combination h(125)h(125)','refCode':'HDBS-2018-58','abstract':'This letter presents a combination of searches for Higgs boson pair production using up to 36.1 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy $\\sqrt{s } = 13$ TeV recorded with the ATLAS detector at the LHC. The combination is performed using six analyses searching for Higgs boson pairs decaying into the $bbbb$, $bbWW$, $bb\\tau\\tau$, $WWWW$, $bb\\gamma \\gamma$ and $WW\\gamma\\gamma$ final states. Results are presented for non-resonant and resonant Higgs boson pair production modes. The combined observed limit at 95% confidence level on the non-resonant Higgs boson pair production cross-section is 6.9 times the predicted Standard Model cross-section. Limits are also set on the ratio ($\\kappa_{\\lambda}$) of the Higgs boson self-coupling to its Standard Model value. This ratio is constrained at 95% confidence level to $-5.0 < \\kappa_{\\lambda} <12.0$. In addition, limits are set on the production of narrow scalar resonances and spin-2 Kaluza-Klein Randall-Sundrum gravitons. Exclusion regions are also provided in the parameter space of the habemus Minimal Supersymmetric Standard Model and the Electroweak Singlet Model.','cdsLink':'','journal':'PLB','journalSub':'05-JUN-19','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Di-Higgs production,Higgs to tautau,Higgs to bb,Higgs to WW,Higgs to 2 photons,Statistical combination,Di-Higgs,Higgs','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HDBS-2018-58@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1906.02025@linkEnd@1906.02025@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1738524@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'','publicationType':'PAPER','pressStatement':''},{'publicationId':'11505','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=11505','shortTitle':'HComb H->inv combination 2011-2016','fullTitle':'Combination of searches for invisible Higgs boson decays with the ATLAS experiment','pubShortTitle':'H(125)->invisible combination','refCode':'HIGG-2018-54','abstract':'Dark matter particles, if sufficiently light, may be produced in decays of the Higgs boson. This Letter presents a statistical combination of searches for $H\\to\\textrm{invisible}$ decays where $H$ is produced according to the Standard Model via vector boson fusion, $Z(\\ell\\ell)H$, and $W\\!/\\!Z(\\textrm{had})H$, all performed with the ATLAS detector using 36.1 fb$^{-1}$ of $pp$ collisions at a center-of-mass energy of $\\sqrt s = 13$ TeV at the LHC. In combination with the results at $\\sqrt s = 7$ and 8 TeV, an exclusion limit on the $H\\to\\textrm{invisible}$ branching ratio of  $0.26 (0.17^{+0.07}_{-0.05})$ at 95% confidence level is observed (expected).','cdsLink':'','journal':'PRL','journalSub':'10-APR-19','ecm':'7, 8, 13','luminosity':'5 fb-1, 20 fb-1, 36 fb-1','keywords':'13 TeV,Exotic Higgs decays,Higgs to invisible,Statistical combination,MET','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2018-54@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1904.05105@linkEnd@1904.05105@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1729103@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1; 2','finalPubRef':'@linkBegin@https://link.aps.org/doi/10.1103/PhysRevLett.122.231801@linkEnd@DOI:10.1103/PhysRevLett.122.231801@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.122.231801@linkEnd@Phys.%20Rev.%20Lett.%20122%20(2019)%20231801@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8903','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8903','shortTitle':'HQT - Run 2 ttbar resonances hadronic','fullTitle':'Search for heavy particles decaying into a top-quark pair in the fully hadronic final state in $pp$ collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Search for top - anti-top resonances in the hadronic final state','refCode':'EXOT-2016-24','abstract':'A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of $\\sqrt{s } =$13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing $b$-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical $Z$ bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross-sections, the $Z$ boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1$-$3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 TeV to 0.9 TeV and from 2.0 TeV to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.','cdsLink':'','journal':'PRD','journalSub':'26-FEB-19','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM resonance,BSM search,Top pair,Boosted,All hadronic,>=3 jets,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-24@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1902.10077@linkEnd@1902.10077@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1722036@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevD.99.092004@linkEnd@DOI:10.1103/PhysRevD.99.092004@descriptionEnd@,@linkBegin@https://link.aps.org/doi/10.1103/PhysRevD.99.092004@linkEnd@Phys.%20Rev.%20D%2099%20(2019)%20092004@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10645','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10645','shortTitle':'LPX - leptoquarks 3rd Gen 2016','fullTitle':'Searches for third-generation scalar leptoquarks in $\\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector','pubShortTitle':'Searches for 3rd generation Leptoquarks','refCode':'EXOT-2017-30','abstract':'Limits are set on the pair production of scalar leptoquarks, where all possible decays of the leptoquark into a quark ($t$, $b$) and a lepton ($\\tau$, $\\nu$) of the third generation are considered. The limits are presented as a function of the leptoquark mass and the branching ratio into charged leptons for up-type ($\\mathrm{LQ}_{3}^{u}$ $\\rightarrow t \\nu / b \\tau$) and down-type ($\\mathrm{LQ}_{3}^{d}$ $\\rightarrow b \\nu / t \\tau$) leptoquarks. Many results are reinterpretations of previously published ATLAS searches. In all cases, LHC proton-proton collision data at a centre-of-mass energy of $\\sqrt{s}$ = 13 TeV recorded by the ATLAS detector in 2015 and 2016 are used, corresponding to an integrated luminosity of 36.1 fb$^{-1}$. Masses below 800 GeV are excluded for both $\\mathrm{LQ}_{3}^{u}$ and $\\mathrm{LQ}_{3}^{d}$ independently of the branching ratio, with masses below about 1 TeV being excluded for the limiting cases of branching ratios equal to zero or unity.','cdsLink':'','journal':'JHEP','journalSub':'21-FEB-19','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Leptoquarks,BSM resonance,BSM search,b-jets,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-30@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1902.08103@linkEnd@1902.08103@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1721072@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP06(2019)144@linkEnd@DOI:10.1007/JHEP06(2019)144@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP06(2019)144@linkEnd@JHEP%2006%20(2019)%20144@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10576','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10576','shortTitle':'UEH - Displaced jets CalRatio','fullTitle':'Search for long-lived neutral particles in $pp$ collisions at $\\sqrt{s}$ = 13 TeV that decay into displaced hadronic jets in the ATLAS calorimeter','pubShortTitle':'Search for displaced hadronic jets in the calorimeter','refCode':'EXOT-2017-25','abstract':'This paper describes a search for pairs of neutral, long-lived particles decaying in the ATLAS calorimeter. Long-lived particles occur in many extensions to the Standard Model and may elude searches for new promptly decaying particles. The analysis considers neutral, long-lived scalars with masses between 5 GeV and 400 GeV, produced from decays of heavy bosons with masses between 125 GeV and 1000 GeV, where the long-lived scalars decay into Standard Model fermions. The analysis uses either 10.8 fb$^{-1}$ or 33.0 fb$^{-1}$ of data (depending on the trigger) recorded in 2016 at the LHC with the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV. No significant excess is observed, and limits are reported on the production cross section times branching ratio as a function of the proper decay length of the long-lived particles.','cdsLink':'','journal':'EPJC','journalSub':'08-FEB-19','ecm':'13','luminosity':'33 fb-1','keywords':'13 TeV,Exotic Higgs decays,Other new particle searches,Dark sector,BSM resonance,MVA / machine learning,Long-lived massive particles,BSM search,Long-lived massive particle','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-25@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1902.03094@linkEnd@1902.03094@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1719200@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-019-6962-6@linkEnd@DOI:10.1140/epjc/s10052-019-6962-6@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-019-6962-6@linkEnd@Eur.%20Phys.%20J.%20C%2079%20(2019)%20481@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10865','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10865','shortTitle':'HLeptons bH H to mu mu','fullTitle':'Search for scalar resonances decaying into $\\mu^{+}\\mu^{-}$ in events with and without $b$-tagged jets produced in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM bH with H-> mu mu','refCode':'HIGG-2017-10','abstract':'A search for a narrow scalar resonance decaying into opposite-sign muon pair produced in events with and without b-tagged jets is presented in this paper. The A search for a narrow scalar resonance decaying into an opposite-sign muon pair produced in events with and without b-tagged jets is presented in this paper. The search uses 36.1 fb$^{-1}$ of $\\sqrt{s}=13$ TeV proton-proton collision data recorded by the ATLAS experiment at the LHC. No significant excess of events above the expected Standard Model background is observed in the investigated mass range of 0.2 to 1.0 TeV. The observed upper limits at 95% confidence level on the cross section times branching ratio for $b$-quark associated production and gluon-gluon fusion are between 1.9 and 41 fb and 1.6 and 44 fb respectively, which is consistent with expectations.','cdsLink':'','journal':'JHEP','journalSub':'23-JAN-19','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM Higgs searches,Higgs to 2 muons,BSM search,b-hadron,b-jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2017-10@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1901.08144@linkEnd@1901.08144@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1716572@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP07(2019)117@linkEnd@DOI:10.1007/JHEP07(2019)117@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007%252FJHEP07%25282019%2529117@linkEnd@JHEP%2007%20(2019)%20117@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9323','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9323','shortTitle':'HBSM HH to WW*WW*','fullTitle':'Search for Higgs boson pair production in the $WW^{( * )}WW^{( * )}$ decay channel using ATLAS data recorded at $\\sqrt{s}=13$ TeV','pubShortTitle':'Search BSM H->HH->4W and HH->4W','refCode':'HIGG-2016-24','abstract':'A search for a pair of neutral, scalar bosons with each decaying into two $W$ bosons is presented using 36.1 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider.  This search uses three production models: non-resonant and resonant Higgs boson pair production and resonant production of a pair of heavy scalar particles.  Three final states, classified by the number of leptons, are analysed: two same-sign leptons, three leptons, and four leptons. No significant excess over the expected Standard Model backgrounds is observed.  An observed (expected) 95% confidence-level upper limit of 160 (120) times the Standard Model prediction of non-resonant Higgs pair production cross-section is set from a combined analysis of the three final states.  Upper limits are set on the production cross-section times branching ratio of a heavy scalar $X$ decaying into a Higgs boson pair in the mass range of 260 GeV $\\le m_X \\le$ 500 GeV and the observed (expected) limits range from 9.3 (10) pb to 2.8 (2.6) pb. Upper limits are set on the production cross-section times branching ratio of a heavy scalar $X$ decaying into a pair of heavy scalars $S$ for mass ranges of 280 GeV $\\le m_X \\le$ 340 GeV and 135 GeV $\\le m_S \\le$ 165 GeV and the observed (expected) limits range from 2.5 (2.5) pb to 0.16 (0.17) pb.','cdsLink':'','journal':'JHEP','journalSub':'27-NOV-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to WW,BSM search,Di-Higgs,WW,>=3 leptons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-24@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1811.11028@linkEnd@1811.11028@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1705396@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP05(2019)124@linkEnd@DOI:10.1007/JHEP05(2019)124@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP05(2019)124@linkEnd@JHEP%2005%20(2019)%20124@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9463','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9463','shortTitle':'HBSM HH to bbWW 2015+2016','fullTitle':'Search for Higgs boson pair production in the $b\\bar{b}WW^{*}$ decay mode at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H->HH->bb WW and HH->bb WW','refCode':'HIGG-2016-27','abstract':'A search for Higgs boson pair production in the $b\\bar{b}WW^\\ast$ decay mode is performed in the $b\\bar{b}l\\nu qq$ final state using 36.1 fb$^{-1}$ of proton-proton collision data at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of events beyond the background expectation is found. Upper limits on the  non-resonant $pp\\to HH$  production cross section of 10 pb and on the resonant production  cross section  as a function of the $HH$ invariant mass are obtained. Resonant production limits are set for scalar and spin-2 graviton hypotheses in the mass range 500 to 3000 GeV.','cdsLink':'','journal':'JHEP','journalSub':'12-NOV-18','ecm':'13','luminosity':'37 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to bb,Higgs to WW,BSM search,Di-Higgs,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-27@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1811.04671@linkEnd@1811.04671@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1703139@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP04(2019)092@linkEnd@DOI:%2010.1007/JHEP04(2019)092@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP04(2019)092@linkEnd@JHEP%2004%20(2019)%20092@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10244','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10244','shortTitle':'HTop H+ to tb 2015+2016','fullTitle':'Search for charged Higgs bosons decaying into top and bottom quarks at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'Search BSM H+ -> tb','refCode':'HIGG-2017-04','abstract':'A search for charged Higgs bosons heavier than the top quark and decaying via $H^+ \\to tb$ is presented. The data analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s } = 13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \\to tb H^+$, is explored in the mass range from $m_H^+ =$ 200 to 2000 GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching fraction of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_H^+ =$ 200 GeV to 0.070 pb at $m_H^+ =$ 2000 GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.','cdsLink':'','journal':'JHEP','journalSub':'10-AUG-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM Higgs searches,BSM search,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2017-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1808.03599@linkEnd@1808.03599@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1686365@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP11(2018)085@linkEnd@DOI:10.1007/JHEP11(2018)085@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP11(2018)085@linkEnd@JHEP%2011%20(2018)%20085@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10667','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10667','shortTitle':'DBL - VV/VH and ll/lv Combination 2016','fullTitle':'Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'VV/VH and ll/lv heavy resonance search combination','refCode':'EXOT-2017-31','abstract':'Searches for new heavy resonances decaying into different pairings of $W$, $Z$, or Higgs bosons, as well as directly into leptons, are presented using a data sample corresponding to 36.1fb$^{-1}$ of $pp$ collisions at $\\sqrt{s } = 13$ TeV collected during 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting bosonic decay modes in the $qqqq$, $\\nu\\nu qq$, $\\ell\\nu qq$, $\\ell\\ell qq$, $\\ell\\nu\\ell\\nu$, $\\ell\\ell\\nu\\nu$, $\\ell\\nu\\ell\\ell$, $\\ell\\ell\\ell\\ell$, $qqbb$, $\\nu\\nu bb$, $\\ell\\nu bb$, and $\\ell\\ell bb$ final states are combined, searching for a narrow-width resonance. Likewise, analyses selecting the leptonic $\\ell\\nu$ and $\\ell\\ell$ final states are also combined. These two sets of analyses are then further combined. No significant deviation from the Standard Model predictions is observed. Three benchmark models are tested: a model predicting the existence of a new heavy scalar singlet, a simplified model predicting a heavy vector-boson triplet, and a bulk Randall-Sundrum model with a heavy spin-2 Kaluza-Klein excitation of the graviton. Cross-section limits are set at the 95% confidence level using an asymptotic approximation and are compared with predictions for the benchmark models. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The data exclude a heavy vector-boson triplet with mass below 5.5 TeV in a weakly coupled scenario and 4.5 TeV in a strongly coupled scenario, as well as a Kaluza-Klein graviton with mass below 2.3 TeV.','cdsLink':'','journal':'PRD','journalSub':'07-AUG-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Heavy vector triplets,BSM resonance,BSM reinterpretation,BSM search,Statistical combination,Di-Higgs,VH,Vphoton,ZZ,WZ,WW,Boosted,MET,b-jets,2 jets,1 jet,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-31@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1808.02380@linkEnd@1808.02380@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1685420@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://atlas.cern/updates/physics-briefing/stronger-together-combining-searches@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevD.98.052008@linkEnd@DOI:10.1103/PhysRevD.98.052008@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.98.052008@linkEnd@Phys.%20Rev.%20D%2098%20(2018)%20052008@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8583','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8583','shortTitle':'HBSM double charged H to WW','fullTitle':'Search for doubly charged scalar bosons decaying into same-sign $W$ boson pairs with the ATLAS detector','pubShortTitle':'Search BSM H++ -> W+W+','refCode':'HIGG-2016-09','abstract':'A search for doubly charged scalar bosons decaying into $W$ boson pairs is presented. It uses a data sample from proton-proton collisions corresponding to an integrated luminosity of  36.1 fb$^{-1}$ collected by the ATLAS detector at the LHC at a centre-of-mass energy of 13 TeV in 2015 and 2016. This search is guided by a model that includes an extension of the Higgs sector through a scalar triplet, leading to a rich phenomenology that includes doubly charged scalar bosons $H^{\\pm\\pm}$. Those bosons are produced in pairs in proton-proton collisions and decay predominantly into electroweak gauge bosons $H^{\\pm\\pm}\\to W^\\pm W^\\pm$. Experimental signatures with several leptons, missing transverse energy and jets are explored. No significant deviations from the Standard Model predictions are found. The parameter space of the benchmark model is excluded at 95% confidence level for $H^{\\pm\\pm}$ bosons with masses between 200 and 220 GeV.','cdsLink':'','journal':'EPJ C','journalSub':'05-AUG-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM Higgs searches,WW,W','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-09@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1808.01899@linkEnd@1808.01899@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1685418@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-018-6500-y@linkEnd@DOI:10.1140/epjc/s10052-018-6500-y@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-018-6500-y@linkEnd@Eur.%20Phys.%20J.%20C%2079%20(2019)%2058@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9104','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9104','shortTitle':'HBSM HH to bbtautau 2015+2016','fullTitle':'A search for resonant and non-resonant Higgs boson pair production in the ${b\\bar{b}\\tau^+\\tau^-}$ decay channel in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H->HH->bb tau tau and HH->bb tau tau','refCode':'HIGG-2016-16','abstract':'A search for resonant and non-resonant pair production of Higgs bosons in the $b\\bar{b}\\tau^+\\tau^-$ final state is presented. The search uses 36.1 fb$^{-1}$ of $pp$ collision data with $\\sqrt{s}= 13$ TeV recorded by the ATLAS experiment at the LHC in 2015 and 2016. The semileptonic and fully hadronic decays of the $\\tau$-lepton pair are considered. No significant excess above the expected background is observed in the data. The cross-section times branching ratio for non-resonant Higgs boson pair production is constrained to be less than 30.9 fb, 12.7 times the Standard Model expectation, at 95% confidence level. The data are also analyzed to probe resonant Higgs boson pair production, constraining a model with an extended Higgs sector based on two doublets and a Randall-Sundrum bulk graviton model. Upper limits are placed on the resonant Higgs boson pair production cross-section times branching ratio, excluding resonances $X$ in the mass range $305~{\\rm GeV} < m_X < 402~{\\rm GeV}$ in the simplified hMSSM minimal supersymmetric model for $\\tan\\beta= 2$ and excluding bulk Randall-Sundrum gravitons $G_{\\mathrm{KK}}$ in the mass range $325~{\\rm GeV} < m_{G_{\\mathrm{KK}}} < 885~{\\rm GeV}$ for $k/\\overline{M}_{\\mathrm{Pl} } = 1$.','cdsLink':'','journal':'PRL','journalSub':'01-AUG-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to tautau,Higgs to bb,BSM search,Di-Higgs,b-jets,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-16@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1808.00336@linkEnd@1808.00336@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1684645@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/ins1684645@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevLett.121.191801@linkEnd@DOI:10.1103/PhysRevLett.121.191801@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.121.191801@linkEnd@Phys.%20Rev.%20Lett.%20121%20(2018)%20191801@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9164','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9164','shortTitle':'HGam HBSM HH to WWyy 2015+2106','fullTitle':'Search for Higgs boson pair production in the $\\gamma\\gamma WW^{*}$ channel using $pp$ collision data recorded at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H->HH->WW gamma gamma and HH->WW gamma gamma','refCode':'HIGG-2016-20','abstract':'Searches for non-resonant and resonant Higgs boson pair production are performed in the $\\gamma\\gamma WW^{*}$ channel with the final state of $\\gamma\\gamma\\ell\\nu jj$ using 36.1 $\\mathrm{fb}^{-1}$ of proton-proton collision data recorded at a centre-of-mass energy of $\\sqrt{s } = 13$ TeV by the ATLAS detector at the Large Hadron Collider. No significant deviation from the Standard Model prediction is observed. A 95% confidence-level observed upper limit of 7.7 pb is set on the cross section for non-resonant production, while the expected limit is 5.4 pb. A search for a narrow-width resonance $X$ decaying to a pair of Standard Model Higgs bosons $HH$ is performed with the same set of data, and the observed upper limits on $\\sigma(pp \\rightarrow X) \\times B(X \\rightarrow HH)$ range between 40.0 pb and 6.1 pb for masses of the resonance between 260 GeV and 500 GeV, while the expected limits range between 17.6 pb and 4.4 pb. When deriving the limits above, the Standard Model branching ratios of the $H \\rightarrow \\gamma\\gamma$  and $H \\rightarrow WW^{*}$ are assumed.','cdsLink':'','journal':'EPJC','journalSub':'23-JUL-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to WW,Higgs to 2 photons,BSM search,Di-Higgs,Di-photon,WW,MET,Photons,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-20@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1807.08567@linkEnd@1807.08567@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1683431@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-018-6457-x@linkEnd@DOI:10.1140/epjc/s10052-018-6457-x@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-018-6457-x@linkEnd@Eur.%20Phys.%20J.%20C%2078%20(2018)%201007@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8743','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8743','shortTitle':'HBSM H+ to tau nu 2015+2016','fullTitle':'Search for charged Higgs bosons decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$ in the $\\tau$+jets and $\\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\\sqrt{s } = 13$ TeV with the ATLAS experiment','pubShortTitle':'Search BSM H+ -> tau nu','refCode':'HIGG-2016-11','abstract':'Charged Higgs bosons produced either in top-quark decays or in association with a top-quark, subsequently decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$, are searched for in 36.1 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=13$ TeV recorded with the ATLAS detector. Depending on whether the top-quark produced together with $H^{\\pm}$ decays hadronically or leptonically, the search targets $\\tau$+jets and $\\tau$+lepton final states, in both cases with a hadronically decaying $\\tau$-lepton. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\\mathrm{B}(H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau})$ in the range 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\\overline{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\\mathrm{B}(t\\to bH^{\\pm}) \\times \\mathrm{B}(H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau})$.','cdsLink':'','journal':'JHEP','journalSub':'20-JUL-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM Higgs searches,BSM search,MET,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-11@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1807.07915@linkEnd@1807.07915@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1683331@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/ins1683331@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP09(2018)139@linkEnd@DOI:10.1007/JHEP09(2018)139@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP09(2018)139@linkEnd@JHEP%2009%20(2018)%20139@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9103','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9103','shortTitle':'HGam HBSM HH to bbyy 2015+2016','fullTitle':'Search for Higgs boson pair production in the $\\gamma\\gamma b\\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment','pubShortTitle':'Search BSM H->HH->bb gamma gamma and HH->bb gamma gamma','refCode':'HIGG-2016-15','abstract':'A search is performed for resonant and non-resonant Higgs boson pair production in the $\\gamma\\gamma b\\bar{b}$ final state. The data set used corresponds to an integrated luminosity of 36.1 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of 13 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No significant excess relative to the Standard Model expectation is observed. The observed limit on the non-resonant Higgs boson pair cross-section is 0.73 pb at 95% confidence level. This observed limit is equivalent to 22 times the predicted Standard Model cross-section. The Higgs boson self-coupling ($\\kappa_\\lambda = \\lambda_{HHH} / \\lambda_{HHH}^{SM}$) is constrained at 95% confidence level to $-8.2 < \\kappa_\\lambda < 13.2$. For resonant Higgs boson pair production through X $\\rightarrow$ HH $\\rightarrow$ $\\gamma\\gamma b\\bar{b}$, the limit is presented, using the narrow-width approximation, as a function of $m_X$ in the range 260 GeV $< m_X <$ 1000 GeV. The observed limits range from 1.1 pb to 0.12 pb over this mass range.','cdsLink':'','journal':'JHEP','journalSub':'13-JUL-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM Higgs searches,Di-Higgs production,Higgs to bb,Higgs to 2 photons,BSM search,Di-Higgs,Di-photon,b-jets,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-15@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1807.04873@linkEnd@1807.04873@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1682345@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP11(2018)040@linkEnd@DOI:%20%0910.1007/JHEP11(2018)040@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP11(2018)040@linkEnd@JHEP%2011%20(2018)%20040@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9303','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9303','shortTitle':'HBSM H to J/psi gamma','fullTitle':'Searches for exclusive Higgs and $Z$ boson decays into $J/\\psi\\gamma$, $\\psi(2S)\\gamma$, and $\\Upsilon(nS)\\gamma$ at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search H(125)/Z->J/psi gamma and Upsilon(nS) gamma','refCode':'HIGG-2016-23','abstract':'Searches for the exclusive decays of the Higgs and $Z$ bosons into a $J/\\psi$, $\\psi(2S)$, or $\\Upsilon(nS)$ ($n=1,2,3$) meson and a photon are performed with a $pp$ collision data sample corresponding to an integrated luminosity of 36.1 $fb^{-1}$ collected at $\\sqrt{s}=13$ TeV with the ATLAS detector at the CERN Large Hadron Collider. No significant excess of events is observed above the expected backgrounds, and 95% confidence-level upper limits on the branching fractions of the Higgs boson decays to $J/\\psi\\gamma$, $\\psi(2S)\\gamma$, and $\\Upsilon(nS)\\gamma$ of $3.5\\times10^{-4}$, $2.0\\times10^{-3}$, and $(4.9,5.9,5.7)\\times10^{-4}$, respectively, are obtained assuming Standard Model production. The corresponding 95% confidence-level upper limits for the branching fractions of the $Z$ boson decays are $2.3\\times10^{-6}$, $4.5\\times10^{-6}$ and $(2.8,1.7,4.8)\\times10^{-6}$, respectively.','cdsLink':'','journal':'PLB','journalSub':'02-JUL-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Exotic Higgs decays,Higgs to meson+photon,Higgs to cc,Higgs to bb,Photons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-23@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1807.00802@linkEnd@1807.00802@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1680462@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.09.024@linkEnd@DOI:10.1016/j.physletb.2018.09.024@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S037026931830724X?via=ihub@linkEnd@Phys.%20Lett.%20B%20786%20(2018)%20134@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7922','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7922','shortTitle':'HBSM H to 2a to bb mumu','fullTitle':'Search for Higgs boson decays into a pair of light bosons in the $bb\\mu\\mu$ final state in $pp$ collision at $\\sqrt{s } =$13 TeV with the ATLAS detector','pubShortTitle':'Search BSM H(125)->2a->bb mu mu','refCode':'HIGG-2016-03','abstract':'A search for decays of the Higgs boson into a pair of new spin-zero particles, $H \\to aa$,  where the $a$-bosons decay into a $b$-quark pair and muon pair, is presented. The search uses 36.1 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s}=13$ TeV recorded by the ATLAS experiment at the LHC in 2015 and 2016.  No significant deviation from the Standard Model prediction is observed.  Upper limits at  95% confidence level are placed on the branching ratio $(\\sigma_H / \\sigma_{SM}) \\times B(H\\to aa\\to bb\\mu\\mu)$, ranging from $2\\times 10^{-4}$ to $10^{-3}$ in the $a$-boson mass range of $20-60$ GeV. Model-independent limits are set on the visible production cross-section times the branching ratio to the $bb\\mu\\mu$ final state for new physics, $\\sigma_{vis}(X) \\times B(X\\to bb\\mu\\mu)$, ranging from 0.1 fb to 0.73 fb for $m_{\\mu\\mu}$ between 18 and 62 GeV.','cdsLink':'','journal':'PLB','journalSub':'02-JUL-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,NMSSM,Exotic Higgs decays,b-jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-03@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1807.00539@linkEnd@1807.00539@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1680457@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.10.073@linkEnd@DOI:10.1016/j.physletb.2018.10.073@descriptionEnd@,@linkBegin@https://reader.elsevier.com/reader/sd/pii/S0370269318309717?token=DC8EA107DE771BCE01F7589B6F75A4A9CA3F230D34D076B44BAEABE9E913931A3BFD0970ECECCC480F64D953D256F21D@linkEnd@Phys.%20Lett.%20B%20790%20(2019)%201@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10263','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10263','shortTitle':'HTop H->2a->4b 2015+2016','fullTitle':'Search for the Higgs boson produced in association with a vector boson and decaying into two spin-zero particles in the $H \\rightarrow aa \\rightarrow 4b$ channel in $pp$ collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H(125)->2a->4b','refCode':'HIGG-2017-05','abstract':'A search for exotic decays of the Higgs boson into a pair of spin-zero particles, $H \\rightarrow aa$, where the $a$-boson decays into $b$-quarks promptly or with a mean proper lifetime $c\\tau_a$ up to 6 mm and has a mass in the range of $20-60$ GeV, is presented. The search is performed in events where the Higgs boson is produced in association with a $W$ or $Z$ boson, giving rise to a signature of one or two charged leptons (electrons or muons) and multiple jets from $b$-quark decays. The analysis is based on the dataset of proton-proton collisions at $\\sqrt{s } = 13$ TeV recorded in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider, corresponding to an integrated luminosity of $36.1$ fb$^{-1}$. No significant excess of events above the Standard Model background prediction is observed, and 95% confidence-level upper limits are derived for the production cross-sections for $pp \\rightarrow WH$, $ZH$ and their combination, times the branching ratio of the decay chain $H \\rightarrow aa \\rightarrow 4b$. For $a$-bosons which decay promptly, the upper limit on the combination of cross-sections for $WH$ and $ZH$ times the branching ratio of $H \\rightarrow aa \\rightarrow 4b$ ranges from 3.0 pb for $m_a= 20$ GeV to 1.3 pb for $m_a = 60$ GeV, assuming that the ratio of $WH$ to $ZH$ cross-sections follows the Standard Model prediction. For $a$-bosons with longer proper lifetimes, the most stringent limits are 1.8 pb and 0.6 pb, respectively, at $c\\tau_a \\sim 0.4$ mm.','cdsLink':'','journal':'JHEP','journalSub':'19-JUN-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,NMSSM,Exotic Higgs decays,BSM Higgs searches,Displaced vertex,Long-lived massive particles,Long-lived massive particle,b-jets,All hadronic,>=3 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2017-05@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1806.07355@linkEnd@1806.07355@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1678484@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP10(2018)031@linkEnd@DOI:10.1007/JHEP10(2018)031@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP10(2018)031@linkEnd@JHEP%2010%20(2018)%20031@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8763','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8763','shortTitle':'DBL - WZ->lvll resonance 2016','fullTitle':'Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Resonance search in the WZ to lvll final state','refCode':'EXOT-2016-11','abstract':'A search for a heavy resonance decaying into $WZ$ in the fully leptonic channel (electrons and muons) is performed. It is based on proton-proton collision data collected by the ATLAS experiment at the Large Hadron Collider at a centre-of-mass energy of 13 TeV, corresponding to  an integrated luminosity of 36.1 fb$^{-1}$. No significant excess is observed over the Standard Model predictions and limits are set on the production cross section times branching ratio of a heavy vector particle produced either in quark-antiquark fusion or through vector-boson fusion. Constraints are also obtained on the mass and couplings of a singly charged Higgs boson, in the Georgi-Machacek model, produced through vector-boson fusion.','cdsLink':'','journal':'PLB','journalSub':'05-JUN-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM Higgs searches,Other new particle searches,BSM resonance,BSM search,WZ,MET,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-11@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1806.01532@linkEnd@1806.01532@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1676472@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/82546@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.10.021@linkEnd@DOI:10.1016/j.physletb.2018.10.021@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269318307901?via=ihub@linkEnd@Phys.%20Lett.%20B%20787%20(2018)%2068@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8963','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8963','shortTitle':'DBL - Vgamma hadronic','fullTitle':'Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\\sqrt{s}=13$ $\\mathrm{!TeV}$ with the ATLAS detector','pubShortTitle':'Search for a resonance decaying to W/Z/H plus a photon in the hadronic final state','refCode':'EXOT-2016-30','abstract':'Many extensions of the Standard Model predict new resonances decaying to a $Z$, $W$, or Higgs boson and a photon. This paper presents a search for such resonances produced in $pp$ collisions at $\\sqrt{s } = 13$ TeV using a dataset with an integrated luminosity of 36.1 fb$^{-1}$ collected by the ATLAS detector at the Large Hadron Collider.  The $Z/W/H$ bosons are identified through their decays to hadrons. The data are found to be consistent with the Standard Model expectation in the entire investigated mass range. Upper limits are set on the production cross section times branching fraction for resonance decays to $Z/W+\\gamma$ in the mass range from 1.0 to 6.8 TeV, and for the first time into $H+\\gamma$ in the mass range from 1.0 to 3.0 TeV.','cdsLink':'','journal':'PRD','journalSub':'04-MAY-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Other new particle searches,Heavy vector triplets,BSM resonance,BSM search,Vphoton,Boosted,b-jets,1 jet','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-30@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1805.01908@linkEnd@1805.01908@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1672010@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/82605@linkEnd@HepData@descriptionEnd@@linkBegin@https://atlas.cern/updates/physics-briefing/searching-forces-beyond-standard-model@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevD.98.032015@linkEnd@DOI:10.1103/PhysRevD.98.032015@descriptionEnd@,@linkBegin@https://link.aps.org/doi/10.1103/PhysRevD.98.032015@linkEnd@Phys.%20Rev.%20D%2098%20(2018)%20%20032015@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'6644','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=6644','shortTitle':'HQT - Run 2 ttbar resonances semilept','fullTitle':'Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton--proton collisions at $\\sqrt{s } = 13$ TeV with the ATLAS  detector','pubShortTitle':'Search for top - anti-top resonances in the 1 lepton plus jets final state','refCode':'EXOT-2015-04','abstract':'A search for new heavy particles that decay into top-quark pairs is performed using data collected from proton--proton collisions at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. The integrated luminosity of the data sample is 36.1 fb$^{-1}$. Events consistent with top-quark pair production are selected by requiring a single isolated charged lepton, missing transverse momentum and jet activity compatible with a hadronic top-quark decay. Jets identified as likely to contain $b$-hadrons are required to reduce the background from other Standard Model processes. The invariant mass spectrum of the candidate top-quark pairs is examined for excesses above the background expectation. No significant deviations from the Standard Model predictions are found. Exclusion limits are set on the production cross-section times branching ratio for hypothetical $Z$ bosons, Kaluza--Kein gluons and Kaluza--Klein gravitons that decay into top-quark pairs.','cdsLink':'','journal':'EPJC','journalSub':'28-APR-18','ecm':'13','luminosity':'35 fb-1','keywords':'13 TeV,Strong gravity,BSM resonance,Other top properties,Top properties measurements,BSM search,Top pair,Boosted,MET,b-jets,>=3 jets,2 jets,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2015-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1804.10823@linkEnd@1804.10823@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1670803@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-018-5995-6@linkEnd@DOI:10.1140/epjc/s10052-018-5995-6@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-018-5995-6@linkEnd@Eur.%20Phys.%20J.%20C%2078%20(2018)%20565@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9063','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9063','shortTitle':'DBL - HH to 4b 2016','fullTitle':'Search for pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using proton-proton collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Search for HH to bbbb','refCode':'EXOT-2016-31','abstract':'A search for Higgs boson pair production in the $b\\bar{b}b\\bar{b}$ final state is carried out with up to 36.1 $\\mathrm{fb}^{-1}$ of LHC proton--proton collision data collected at $\\sqrt{s } = 13$ TeV with the ATLAS detector in 2015 and 2016. Three benchmark signals are studied: a spin-2 graviton decaying into a Higgs boson pair, a scalar resonance decaying into a Higgs boson pair, and Standard Model non-resonant Higgs boson pair production. Two analyses are carried out, each implementing a particular technique for the event reconstruction that targets Higgs bosons reconstructed as pairs of jets or single boosted jets. The resonance mass range covered is 260--3000 GeV. The analyses are statistically combined and upper limits on the production cross section of Higgs boson pairs times branching ratio to $b\\bar{b}b\\bar{b}$ are set in each model. No significant excess is observed; the largest deviation of data over prediction is found at a mass of 280 GeV, corresponding to 2.3 standard deviations globally. The observed 95% confidence level upper limit on the non-resonant production is 13 times the Standard Model prediction.','cdsLink':'','journal':'JHEP','journalSub':'17-APR-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,BSM resonance,Di-Higgs production,BSM search,Di-Higgs,Boosted,b-jets,All hadronic,>=3 jets,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-31@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1804.06174@linkEnd@1804.06174@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1668124@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/82599@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP01(2019)030@linkEnd@DOI:10.1007/JHEP01(2019)030@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP01(2019)030@linkEnd@JHEP%2001%20(2019)%20030@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9603','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9603','shortTitle':'DBL - A to Zh(not H125) leptonic','fullTitle':'Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\\ell\\ell bb$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'A to Zh search in the llbb final state with non-SM h ','refCode':'EXOT-2016-34','abstract':'A search for a heavy neutral Higgs boson, $A$, decaying into a $Z$ boson and another heavy Higgs boson, $H$, is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton--proton collisions at $\\sqrt{s } = 13$ TeV recorded in 2015 and 2016 by the ATLAS detector at the Large Hadron Collider. The search considers the $Z$ boson decaying to electrons or muons and the $H$ boson into a pair of $b$-quarks. No evidence for the production of an $A$ boson is found. Considering each production process separately, the 95% confidence-level upper limits on the $pp\\rightarrow A\\rightarrow ZH$ production cross-section times the branching ratio $H\\rightarrow bb$ are in the range of 14--830 fb for the gluon--gluon fusion process and 26--570 fb for the $b$-associated process for the mass ranges 130--700 GeV of the $H$ boson and process for the mass ranges 130--700 GeV of the $H$ boson and 230--800 GeV of the $A$ boson. The results are interpreted in the context of the two-Higgs-doublet model.','cdsLink':'','journal':'PLB','journalSub':'03-APR-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Exotic Higgs production,BSM Higgs searches,BSM resonance,Higgs to bb,BSM search,Z,b-jets,>=3 jets,2 jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-34@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1804.01126@linkEnd@1804.01126@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1665828@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/82527@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.07.006@linkEnd@DOI:10.1016/j.physletb.2018.07.006@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269318305446?via=ihub@linkEnd@Phys.%20Lett.%20B%20783%20(2018)%20392@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10523','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10523','shortTitle':'HBSM H to 2a to yy jj','fullTitle':'Search for Higgs boson decays into pairs of light (pseudo)scalar particles in the $\\gamma\\gamma jj$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM VBF H(125)->2a-> jet jet gamma gamma','refCode':'HIGG-2017-09','abstract':'This Letter presents a search for exotic decays of the Higgs boson to a pair of new (pseudo)scalar particles, $H\\to aa$, with a mass in the range 20--60 GeV, and where one of the $a$ bosons decays into a pair of photons and the other to a pair of gluons. The search is performed in event samples enhanced in vector-boson fusion Higgs boson production by requiring two jets with large invariant mass in addition to the Higgs boson candidate decay products. The analysis is based on the full dataset of $pp$ collisions at $\\sqrt{s}= 13$ TeV recorded in 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider, corresponding to an integrated luminosity of 36.7 fb$^{-1}$. The data are in agreement with the Standard Model predictions and an upper limit at the 95% confidence level is placed on the production cross section times the branching ratio for the decay $H\\to aa\\to \\gamma\\gamma gg$. This limit ranges from 3.1 pb to 9.0 pb depending on the mass of the $a$ boson.','cdsLink':'','journal':'PLB','journalSub':'29-MAR-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,NMSSM,Exotic Higgs decays,BSM search,VBF,Higgs,Di-photon,>=3 jets,2 jets,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2017-09@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1803.11145@linkEnd@1803.11145@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1665234@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.06.011@linkEnd@DOI:10.1016/j.physletb.2018.06.011@descriptionEnd@,@linkBegin@https://linkinghub.elsevier.com/retrieve/pii/S0370269318304593@linkEnd@Phys.%20Lett.%20B%20782%20(2018)%20750@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8884','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8884','shortTitle':'UEH - ZdarkZdark','fullTitle':'Search for Higgs boson decays to beyond-the-Standard-Model light bosons in four-lepton events with the ATLAS detector at $\\sqrt{s}=13$ TeV','pubShortTitle':'H to ZdarkZdark or ZZdark search in the llll final state','refCode':'EXOT-2016-22','abstract':'A search is conducted for a new beyond-the-Standard-Model boson using events where a Higgs boson with mass 125 GeV decays to four leptons ($\\ell =$ $e$ or $\\mu$). This decay is presumed to occur via an intermediate state which contains one or two on-shell, promptly decaying bosons: $H\\rightarrow ZX/XX \\rightarrow 4\\ell$, where $X$ is a new vector boson $Z_d$ or pseudoscalar $a$ with mass between 1 and 60 GeV. The search uses $pp$ collision data collected with the ATLAS detector at the LHC with an integrated luminosity of 36.1 fb$^{-1}$ at a centre-of-mass energy $\\sqrt{s}=13$ TeV. No significant excess of events above Standard Model background predictions is observed; therefore, upper limits at 95% confidence level are set on model-independent fiducial cross-sections, and on the Higgs boson decay branching ratios to vector and pseudoscalar bosons in two benchmark models.','cdsLink':'','journal':'JHEP','journalSub':'09-FEB-18','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Exotic Higgs decays,Dark sector,BSM search,Higgs,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-22@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1802.03388@linkEnd@1802.03388@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1654372@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP06(2018)166@linkEnd@DOI:10.1007/JHEP06(2018)166@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP06(2018)166@linkEnd@JHEP%2006%20(2018)%20166@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10285','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10285','shortTitle':'LPX - hadronic tau + MET search','fullTitle':'A search for high-mass resonances decaying to $\\tau\\nu$ in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'Search for a resonance in the hadronic tau + MET final state','refCode':'EXOT-2017-06','abstract':'A search for high-mass resonances decaying to $\\tau\\nu$ using proton-proton collisions at $\\sqrt{s}$ = 13 TeV produced by the Large Hadron Collider is presented. Only $\\tau$-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb$^{-1}$. No statistically significant excess above the Standard Model expectation is observed; model-independent upper limits are set on the visible $\\tau\\nu$ production cross section. Heavy $W^{\\prime}$ bosons with masses less than 3.7 TeV in the Sequential Standard Model and masses less than 2.2-3.8 TeV depending on the coupling in the non-universal G(221) model are excluded at the 95% credibility level.','cdsLink':'','journal':'PRL','journalSub':'22-JAN-18','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM resonance,BSM search,MET,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-06@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1801.06992@linkEnd@1801.06992@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1649273@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/80812@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevLett.120.161802@linkEnd@DOI:10.1103/PhysRevLett.120.161802@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.120.161802@linkEnd@Phys.%20Rev.%20Lett.%20120%20(2018)%20161802@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9163','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9163','shortTitle':'HZZ High mass search 2015+2016','fullTitle':'Search for heavy $ZZ$ resonances in the $\\ell^+\\ell^-\\ell^+\\ell^-$   and $\\ell^+\\ell^-\\nu\\bar\\nu$  final states using proton proton collisions  at $\\sqrt{s}= 13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H->ZZ->4l and llvv','refCode':'HIGG-2016-19','abstract':'A  search for heavy resonances decaying into a pair of $Z$ bosons leading to $\\ell^+\\ell^-\\ell^+\\ell^-$ and  $\\ell^+\\ell^-\\nu\\bar\\nu$ final states, where $\\ell$ stands for either an electron or a muon, is presented.  The search uses proton  proton collision data at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector during 2015 and 2016 at the Large Hadron Collider. Different mass ranges for the hypothetical resonances are considered, depending on the final state and model. The different ranges span between 200 GeV and 2000 GeV. The results are interpreted as  upper limits on the production cross section of a spin 0 or spin 2 resonance.  The  upper limits for the spin 0 resonance are translated to exclusion contours in the context of Type I and Type II two-Higgs-doublet models, while those for the spin 2 resonance are used to constrain the Randall Sundrum model with an extra dimension giving rise to spin 2 graviton excitations.','cdsLink':'','journal':'EPJC','journalSub':'18-DEC-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM Higgs searches,Higgs to ZZ,Higgs to 4 lepton,MET,>=3 leptons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-19@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1712.06386@linkEnd@1712.06386@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1643838@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-018-5686-3@linkEnd@DOI:10.1140/epjc/s10052-018-5686-3@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-018-5686-3@linkEnd@Eur.%20Phys.%20J.%20C%2078%20(2018)%20293@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8703','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8703','shortTitle':'DBL - VH semileptonic 2016','fullTitle':'Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs   boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector','pubShortTitle':'Resonance search in the VH to ll/lv/vv plus bb final state','refCode':'EXOT-2016-10','abstract':'A search is conducted for new resonances decaying into a $W$ or $Z$ boson and a 125 GeV Higgs boson in the $\\nu\\bar{\\nu}b\\bar{b}$, $\\ell^{\\pm}{\\nu}b\\bar{b}$, and $\\ell^+\\ell^-b\\bar{b}$ final states, where $\\ell ^{\\pm}= e^{\\pm}$ or $\\mu^{\\pm}$, in $pp$ collisions at $\\sqrt s = 13$ TeV. The data used correspond to a total integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector at the Large Hadron Collider during the 2015 and 2016 data-taking periods. The search is conducted by examining the reconstructed invariant or transverse mass distributions of $Wh$ and $Zh$ candidates for evidence of a localised excess in the mass range of 220 GeV up to 5 TeV. No significant excess is observed and the results are interpreted in terms of constraints on the production cross-section times branching fraction of heavy $W^\\prime$ and $Z^\\prime$ resonances in heavy-vector-triplet models and the CP-odd scalar boson $A$ in two-Higgs-doublet models. Upper limits are placed at the 95 % confidence level and range between $9.0\\times 10^{-4}$ pb and $8.1\\times 10^{-1}$ pb depending on the model and mass of the resonance.','cdsLink':'','journal':'JHEP','journalSub':'17-DEC-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM Higgs searches,Heavy vector triplets,BSM resonance,BSM search,VH,Boosted,MET,b-jets,>=3 jets,2 jets,1 jet,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-10@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1712.06518@linkEnd@1712.06518@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1643843@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/79797@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP03(2018)174@linkEnd@DOI:%2010.1007/JHEP03(2018)174@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP03(2018)174@linkEnd@JHEP%2003%20(2018)%20174@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9023','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9023','shortTitle':'HBSM H to phi gamma 2015+2016','fullTitle':'Search for exclusive Higgs and $Z$ boson decays to $\\phi\\gamma$ and $\\rho\\gamma$ with the ATLAS detector','pubShortTitle':'Search H(125)/Z->phi gamma and rho gamma','refCode':'HIGG-2016-13','abstract':'A search for the exclusive decays of the Higgs and $Z$ bosons to a $\\phi$ or $\\rho$ meson and a photon is performed with a $pp$ collision data sample corresponding to an integrated luminosity of up to 35.6 $fb^{-1}$ collected at $\\sqrt{s}=13$ TeV with the ATLAS detector at the CERN Large Hadron Collider.  These decays have been suggested as a probe of the Higgs boson couplings to light quarks.  No significant excess of events is observed above the background, as expected from the Standard Model. Upper limits at 95% confidence level were obtained on the branching fractions of the Higgs boson decays to $\\phi\\gamma$ and $\\rho\\gamma$ of $4.8\\times10^{-4}$ and $8.8\\times10^{-4}$, respectively.  The corresponding 95% confidence level upper limits for the $Z$ boson decays are $0.9\\times10^{-6}$ and $25\\times10^{-6}$ for $\\phi\\gamma$ and $\\rho\\gamma$, respectively. ','cdsLink':'','journal':'JHEP','journalSub':'07-DEC-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Exotic Higgs decays,Higgs to meson+photon,Photons,Charged tracks','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-13@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1712.02758@linkEnd@1712.02758@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1641767@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP07(2018)127@linkEnd@DOI:10.1007/JHEP07(2018)127@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP07(2018)127@linkEnd@JHEP%2007%20(2018)%20127@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8926','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8926','shortTitle':'DBL - VV to lvqq 2016','fullTitle':'Search for $WW/WZ$ resonance production in $\\ell \\nu qq$ final states in $pp$ collisions at $\\sqrt{s } =$ 13 TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV to lvqq final state','refCode':'EXOT-2016-28','abstract':'A search is conducted for new resonances decaying into a $WW$ or $WZ$ boson pair, where one $W$ boson decays leptonically and the other $W$ or $Z$ boson decays hadronically. It is based on proton--proton collision data with an integrated luminosity of 36.1 fb$^{-1}$ collected with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of $\\sqrt{s}$ =  13 TeV in 2015 and 2016. The search is sensitive to diboson resonance production via vector--boson fusion as well as quark--antiquark annihilation and gluon--gluon fusion mechanisms. No significant excess of events is observed with respect to the Standard Model backgrounds. Several benchmark models are used to interpret the results. Limits on the production cross section are set for a new narrow scalar resonance, a new heavy vector-boson and a spin-2 Kaluza--Klein graviton.','cdsLink':'','journal':'JHEP','journalSub':'19-OCT-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Heavy vector triplets,BSM resonance,BSM search,VBF,WZ,WW,Boosted,MET,b-jets,2 jets,1 jet,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-28@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1710.07235@linkEnd@1710.07235@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1631642@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/79779@linkEnd@HepData@descriptionEnd@@linkBegin@http://atlas.cern/updates/physics-briefing/probing-heavy-vector-bosons@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP03(2018)042@linkEnd@DOI:10.1007/JHEP03(2018)042@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP03(2018)042@linkEnd@JHEP%2003%20(2018)%20042@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9763','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9763','shortTitle':'HWW high mass lnulnu','fullTitle':'Search for heavy resonances decaying into $WW$ in the $e\\nu\\mu\\nu$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H->WW->lvlv','refCode':'HIGG-2016-31','abstract':'A search for neutral heavy resonances is performed in the $WW\\to e\\nu\\mu\\nu$ decay channel using $pp$ collision data corresponding to an integrated luminosity of 36.1 fb$^{-1}$, collected at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. No evidence of such heavy resonances is found. In the search for production via the quark--antiquark annihilation or gluon--gluon fusion process, upper limits on $\\sigma_X\\times B(X \\to WW)$ as a function of the resonance mass are obtained in the mass range between 200 GeV and up to 5 TeV for various benchmark models: a Higgs-like scalar in different width scenarios, a two-Higgs-doublet model, a heavy vector triplet model, and a warped extra dimensions model. In the vector-boson fusion process, constraints are also obtained on these resonances, as well as on a Higgs boson in the Georgi--Machacek model and a heavy tensor particle coupling only to gauge bosons.','cdsLink':'','journal':'EPJC','journalSub':'03-OCT-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,BSM Higgs searches,BSM resonance,Higgs to WW,BSM search,WW,MET,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-31@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1710.01123@linkEnd@1710.01123@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1628411@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-017-5491-4@linkEnd@DOI:10.1140/epjc/s10052-017-5491-4@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-017-5491-4@linkEnd@Eur.%20Phys.%20J.%20C%2078%20(2018)%2024@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8783','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8783','shortTitle':'HBSM A to tau tau search 2015+2016','fullTitle':'Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'Search BSM A/H/Z->tautau','refCode':'HIGG-2016-12','abstract':'A search for heavy neutral Higgs bosons and $Z^{\\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016. The heavy resonance is assumed to decay to $\\tau^+\\tau^-$ with at least one tau lepton decaying to final states with hadrons and a neutrino. The search is performed in the mass range of 0.2-2.25 TeV for Higgs bosons and 0.2-4.0 TeV for $Z^{\\prime}$ bosons.  The data are in good agreement with the background predicted by the Standard Model.  The results are interpreted in benchmark scenarios.  In the context of the hMSSM scenario, the data exclude $\\tan\\beta > 1.0$ for $m_A$ = 0.25 TeV and $\\tan\\beta > 42$ for $m_A$ = 1.5 TeV at the 95% confidence level.  For the Sequential Standard Model, $Z^{\\prime}_\\mathrm{SSM}$ with $m_{Z^{\\prime}} < 2.42$ TeV is excluded at 95% confidence level, while $Z^{\\prime}_\\mathrm{NU}$ with $m_{Z^{\\prime}} < 2.25$ TeV is excluded for the non-universal $G(221)$ model that exhibits enhanced couplings to third-generation fermions.','cdsLink':'','journal':'JHEP','journalSub':'21-SEP-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,BSM resonance,Higgs to tautau,BSM search,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-12@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1709.07242@linkEnd@1709.07242@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1624690@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP01(2018)055@linkEnd@DOI:10.1007/JHEP01(2018)055@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP01(2018)055@linkEnd@JHEP%2001%20(2018)%20055@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'10183','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=10183','shortTitle':'DBL - W to XH','fullTitle':'A search for resonances decaying into a Higgs boson and a new particle $X$ in the $XH \\to qqbb$ final state with the ATLAS detector','pubShortTitle':'Search for a resonance in the XH to qqbb final state where X is a new particle','refCode':'EXOT-2017-04','abstract':'A search for heavy resonances decaying into a Higgs boson ($H$) and a new particle ($X$) is reported, utilizing 36.1 fb$^{-1}$ of proton--proton collision data at $\\sqrt{s } =$ 13 TeV collected during 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. The particle $X$ is assumed to decay to a pair of light quarks, and the fully hadronic final state $XH \\rightarrow q\\bar qb\\bar b$ is analysed. The search considers the regime of high $XH$ resonance masses, where the $X$ and $H$ bosons are both highly Lorentz-boosted and are each reconstructed using a single jet with large radius parameter. A two-dimensional phase space of $XH$ mass versus $X$ mass is scanned for evidence of a signal, over a range of $XH$ resonance mass values between 1 TeV and 4 TeV, and for $X$ particles with masses from 50 GeV to 1000 GeV. All search results are consistent with the expectations for the background due to Standard Model processes, and 95% CL upper limits are set, as a function of $XH$ and $X$ masses, on the production cross-section of the $XH$ resonance.','cdsLink':'','journal':'PLB','journalSub':'20-SEP-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM resonance,BSM search,Higgs,b-hadron,Boosted,b-jets,All hadronic,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2017-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1709.06783@linkEnd@1709.06783@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1624549@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/78568@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2018.01.042@linkEnd@DOI:10.1016/j.physletb.2018.01.042@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269318300509@linkEnd@Phys.%20Lett.%20B%20779%20(2018)%2024@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8927','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8927','shortTitle':'DBL - VV to llqq,vvqq','fullTitle':'Searches for heavy $ZZ$ and $ZW$ resonances in the $\\ell\\ell qq$ and $\\nu\\nu qq$ final states in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV to ll/vv plus qq final state','refCode':'EXOT-2016-29','abstract':'This paper reports searches for heavy resonances decaying into $ZZ$ or $ZW$ using data from proton--proton collisions at a centre-of-mass energy of $\\sqrt{s}=13$ TeV. The data, corresponding to an integrated luminosity of 36.1 fb$^{-1}$, were recorded with the ATLAS detector in 2015 and 2016 at the Large Hadron Collider. The searches are performed in final states in which one $Z$ boson decays into either a pair of light charged leptons (electrons and muons) or a pair of neutrinos, and the associated $W$ boson or the other $Z$ boson decays hadronically. No evidence of the production of heavy resonances is observed. Upper bounds on the production cross sections of heavy resonances times their decay branching ratios to $ZZ$ or $ZW$ are derived in the mass range 300--5000 GeV within the context of Standard Model extensions with additional Higgs bosons, a heavy vector triplet or warped extra dimensions. Production through gluon--gluon fusion, Drell--Yan or vector-boson fusion are considered, depending on the assumed model.','cdsLink':'','journal':'JHEP','journalSub':'31-AUG-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,BSM Higgs searches,Heavy vector triplets,BSM resonance,BSM search,VBF,ZZ,WZ,Boosted,MET,b-jets,2 jets,1 jet,2 leptons,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-29@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1708.09638@linkEnd@1708.09638@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1620910@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/78550@linkEnd@HepData@descriptionEnd@@linkBegin@http://atlas.cern/updates/physics-briefing/probing-heavy-vector-bosons@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP03(2018)009@linkEnd@DOI:10.1007/JHEP03(2018)009@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP03(2018)009@linkEnd@JHEP%2003%20(2018)%20009@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9503','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9503','shortTitle':'HZZ ZH to ll+MET 2015+2016','fullTitle':'Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson in $pp$ collisions at $\\sqrt{s } =$ 13 TeV with the ATLAS detector','pubShortTitle':'Search ZH(125), H(125)->invisible and Z+MET','refCode':'HIGG-2016-28','abstract':'A search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a leptonically decaying $Z$ boson in proton--proton collisions at $\\sqrt{s } =$ 13 TeVis presented. This search uses 36.1 fb$^{-1}$ of data collected by the ATLAS experiment at the Large Hadron Collider. No significant deviation from the background expectation is observed. Assuming the Standard Model $ZH$ production cross-section, an observed (expected) upper limit of 67% (39%) at the 95% confidence level is set on the branching ratio of invisible decays of the Higgs boson with mass $m_H =$ 125 GeV. The corresponding limits on the production cross-section of the $ZH$ process with the invisible Higgs boson decays are also presented. Furthermore, exclusion limits on the dark matter candidate and mediator masses are reported in the framework of simplified dark matter models.','cdsLink':'','journal':'PLB','journalSub':'31-AUG-17','ecm':'13','luminosity':'36 fb-1','keywords':'13 TeV,Simplified DM model,Exotic Higgs decays,Higgs to invisible,Dark matter,Z,MET,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-28@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1708.09624@linkEnd@1708.09624@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1620909@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2017.11.049@linkEnd@DOI:10.1016/j.physletb.2017.11.049@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269317309413@linkEnd@PLB%20%20776%20(2017)%20318@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8843','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8843','shortTitle':'DBL - VV full-hadronic search','fullTitle':'Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV hadronic final state','refCode':'EXOT-2016-19','abstract':'Narrow resonances decaying into $WW$, $WZ$ or $ZZ$ boson pairs are searched for in 36.7 fb $^{-1}$ of proton--proton collision data at a centre-of-mass energy of $\\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 and 2016. The diboson system is reconstructed using pairs of large-radius jets with high transverse momentum and tagged as compatible with the hadronic decay of high-momentum $W$ or $Z$ bosons, using jet mass and substructure properties. The search is sensitive to diboson resonances with masses in the range 1.2-5.0 TeV. No significant excess is observed in any signal region. Exclusion limits are set at the 95% confidence level on the production cross section times branching ratio to dibosons for a range of theories beyond the Standard Model. Lower limits on the mass of new gauge bosons up to 3.5 TeV are set, depending on the assumed model.','cdsLink':'','journal':'PLB','journalSub':'15-AUG-17','ecm':'13','luminosity':'37 fb-1','keywords':'13 TeV,BSM resonance,BSM search,ZZ,WZ,WW,Boosted,All hadronic,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-19@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1708.04445@linkEnd@1708.04445@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1616092@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/79162@linkEnd@HepData@descriptionEnd@@linkBegin@http://atlas.cern/updates/physics-briefing/probing-heavy-vector-bosons@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2017.12.011@linkEnd@DOI:10.1016/j.physletb.2017.12.011@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269317309887@linkEnd@Phys.%20Lett.%20B%20777%20(2017)%2091@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9083','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9083','shortTitle':'HSG1 Higgs to Zgamma 2015+2016','fullTitle':'Searches for the $Z\\gamma$ decay mode of the Higgs boson and for new high-mass resonances in pp collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'H(125)->Zgam and search BSM H->Zgam','refCode':'HIGG-2016-14','abstract':'This article presents searches for the $Z\\gamma$ decay of the Higgs boson and for narrow high-mass resonances decaying to $Z\\gamma$, exploiting $Z$ boson decays to pairs of electrons or muons. The data analysis uses 36.1 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s } = 13$ TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. The data are found to be consistent with the expected Standard Model background. The observed (expected -- assuming Standard Model $pp\\to H\\to Z\\gamma$ production and decay) upper limit on the production cross section times the branching ratio for $pp\\to H\\to Z\\gamma$ is  6.6 (5.2) times the Standard Model prediction at the 95% confidence level for a Higgs boson mass of 125.09 GeV. In addition, upper limits are set on the production cross section times the branching ratio as a function of the mass of a narrow resonance between  250 GeV and 2.4 TeV, assuming spin-0 resonances produced via gluon--gluon fusion, and spin-2 resonances produced via gluon--gluon or quark--antiquark initial states. For high-mass spin-0 resonances, the observed (expected) limits vary between 88 fb (61 fb) and 2.8 fb (2.7 fb) for the mass range from 250 GeV to 2.4 TeV at the 95% confidence level.','cdsLink':'','journal':'JHEP','journalSub':'01-AUG-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Exotic Higgs decays,Higgs to Z+photon,H(125) measurements,Higgs,Vphoton,Z,Photons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-14@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1708.00212@linkEnd@1708.00212@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1613896@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://atlas.cern/updates/physics-briefing/exploring-rare-decays-higgs-boson@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP10(2017)112@linkEnd@DOI:10.1007/JHEP10(2017)112@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP10(2017)112@linkEnd@JHEP%2010%20(2017)%20112@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8803','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8803','shortTitle':'DBL - VH full-hadronic search','fullTitle':'Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\\bar{q}^{(\\prime)}b\\bar{b}$ final state in $pp$ collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VH hadronic final state','refCode':'EXOT-2016-12','abstract':'A search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\\bar{q}^{(\\prime)}b\\bar{b}$ final state is described.  The search uses 36.1 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s } =$ 13 TeV collected by the ATLAS detector at the CERN Large Hadron Collider in 2015 and 2016.  The data are in agreement with the Standard Model expectations, with the largest excess found at a resonance mass of 3.0 TeV with a local (global) significance of 3.3 (2.1)~$\\sigma$. The results are presented in terms of constraints on a simplified model with a heavy vector triplet.  Upper limits are set on the production cross-section times branching ratio for resonances decaying to a $W$ ($Z$) boson and a Higgs boson, itself decaying to $b\\bar{b}$,   in the mass range between 1.1 and 3.8~\\tev; the limits range between 83 and 1.6~fb (77 and 1.1~fb) at 95\\% confidence level.','cdsLink':'','journal':'PLB','journalSub':'20-JUL-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Heavy vector triplets,BSM resonance,BSM search,VH,Boosted,b-jets,All hadronic,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-12@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1707.06958@linkEnd@1707.06958@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1611039@linkEnd@Inspire@descriptionEnd@ @linkBegin@https://www.hepdata.net/record/77272@linkEnd@HepData@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2017.09.066@linkEnd@DOI:10.1016/j.physletb.2017.09.066@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269317307785@linkEnd@Phys.%20Lett.%20B%20774%20(2017)%20494@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8603','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8603','shortTitle':'HQT - H to ttbar 8 TeV','fullTitle':'Search for heavy Higgs bosons $A/H$ decaying to a top quark pair in $pp$ collisions at $\\sqrt{s } = 8$ TeV with the ATLAS detector','pubShortTitle':'Search for A/H to top - anti-top including interference','refCode':'EXOT-2016-04','abstract':'A search for heavy pseudoscalar ($A$) and scalar ($H$) Higgs bosons decaying into a top quark pair ($t\\bar{t}$) has been performed with 20.3 fb$^{-1}$ of proton--proton collision data collected by the ATLAS experiment at the Large Hadron Collider at a center-of-mass energy of $\\sqrt{s } = 8$ TeV. Interference effects between the signal process and Standard Model $t\\bar{t}$ production, which are expected to distort the signal shape from a single peak to a peak--dip structure, are taken into account. No significant deviation from the Standard Model prediction is observed in the $t\\bar{t}$ invariant mass spectrum in final states with an electron or muon, large missing transverse momentum, and at least four jets. The results are interpreted within the context of a type-II two-Higgs-doublet model. Exclusion limits on the signal strength are derived as a function of the mass $m_{A/H}$ and the ratio of the vacuum expectation values of the two Higgs fields, $\\tan\\beta$, for $m_{A/H} > 500$ GeV. ','cdsLink':'','journal':'PRL','journalSub':'19-JUL-17','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM Higgs searches,BSM resonance,BSM search,Gluon fusion,Top pair,MET,b-jets,>=3 jets,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1707.06025@linkEnd@1707.06025@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1610625@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevLett.119.191803@linkEnd@DOI:10.1103/PhysRevLett.119.191803@descriptionEnd@,@linkBegin@https://link.aps.org/doi/10.1103/PhysRevLett.119.191803@linkEnd@Phys.%20Rev.%20Lett.%20119%20(2017)%20191803@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9123','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9123','shortTitle':'HGam high mass diphoton 2015+2016','fullTitle':'Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H/X->gammagamma','refCode':'HIGG-2016-17','abstract':'Searches for new phenomena in high-mass diphoton final states with the ATLAS experiment at the LHC are presented. The analysis is based on $pp$ collision data corresponding to an integrated luminosity of 36.7 fb$^{-1}$ at a centre-of-mass energy $\\sqrt{s}=13$ TeV recorded in 2015 and 2016. Searches are performed for resonances with spin 0, as predicted by theories with an extended Higgs sector, and for resonances with spin 2, using a warped extra-dimension model as a benchmark model, as well as for non-resonant signals, assuming a large extra-dimension scenario. No significant deviation from the Standard Model is observed. Upper limits are placed on the production cross section times branching ratio to two photons as a function of hypothesized signal mass for the two resonance models. In addition, lower limits are set on the ultraviolet cutoff scale in the large extra-dimensions model, depending on the number of extra dimensions and the theoretical formalism used.','cdsLink':'','journal':'PLB','journalSub':'13-JUL-17','ecm':'13','luminosity':'37 fb-1','keywords':'13 TeV,BSM Higgs searches,Strong gravity,BSM resonance,Higgs to 2 photons,Di-photon,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-17@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1707.04147@linkEnd@1707.04147@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1609773@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1016/j.physletb.2017.10.039@linkEnd@DOI:10.1016/j.physletb.2017.10.039@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269317308511@linkEnd@Phys.%20Lett.%20B%20775%20(2017)%20105@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9404','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9404','shortTitle':'HGam FCNC t->qH, H->gaga','fullTitle':'Search for top quark decays $t \\rightarrow qH$, with $H\\to\\gamma\\gamma$, in $\\sqrt{s } = 13$ TeV $pp$ collisions using the ATLAS detector','pubShortTitle':'Search FCNC t->H(125) q, H(125)->gammagamma','refCode':'HIGG-2016-26','abstract':'This article presents a search for flavour-changing neutral currents in the decay of a top quark into an up-type ($q = c, u$) quark and a Higgs boson, where the Higgs boson decays into two photons. The proton--proton collision data set analysed amounts to 36.1 fb$^{-1}$ at $\\sqrt{s } = 13$ TeV collected by the ATLAS experiment at the LHC. Top quark pair events are searched for, where one top quark decays into $qH$ and the other decays into $bW$. Both the hadronic and leptonic decay modes of the $W$ boson are used. No significant excess is observed and an upper limit is set on the $t \\rightarrow cH$ branching ratio of $2.2\\times 10^{-3}$ at the 95% confidence level, while the expected limit in the absence of signal is $1.6 \\times 10^{-3}$. The corresponding limit on the $tcH$ coupling is 0.090 at the 95% confidence level. The observed upper limit on the $t \\rightarrow uH$ branching ratio is $2.4 \\times 10^{-3}$.','cdsLink':'','journal':'JHEP','journalSub':'05-JUL-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Exotic Higgs production,Higgs to 2 photons,Top properties measurements,ttbar rare decays,BSM search,Higgs,Di-photon,W,b-hadron,b-jets,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-26@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1707.01404@linkEnd@1707.01404@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1608777@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1007/JHEP10(2017)129@linkEnd@DOI:10.1007/JHEP10(2017)129@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP10(2017)129@linkEnd@JHEP%2010%20(2017)%20129@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'9124','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=9124','shortTitle':'HGam H to diphoton + MET 2015+2016','fullTitle':'Search for dark matter in association with a Higgs boson decaying to two photons at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'Search H(125)->gamgam + Missing-ET','refCode':'HIGG-2016-18','abstract':'A search for dark matter in association with a Higgs boson decaying to two photons is presented. This study is based on data collected with the ATLAS detector, corresponding to an integrated luminosity of $36.1~\\mathrm{fb}^{-1}$ of proton--proton collisions at the LHC at a center-of-mass energy of 13 TeV in 2015 and 2016. No significant excess over the expected background is observed. Upper limits at 95% confidence level are set on the visible cross section for beyond the Standard Model physics processes, and the production cross section times branching fraction of the Standard Model Higgs boson decaying into two photons in association with missing transverse momentum in three different benchmark models. Limits at 95% confidence level are also set on the observed signal in two-dimensional mass planes. Additionally, the results are interpreted in terms of 90% confidence-level limits on the dark-matter--nucleon scattering cross section, as a function of the dark-matter particle mass, for a spin-independent scenario.','cdsLink':'','journal':'PRD','journalSub':'13-JUN-17','ecm':'13','luminosity':'36.1 fb-1','keywords':'13 TeV,Simplified DM model,Exotic Higgs production,Higgs to 2 photons,BSM search,Dark matter,Higgs,Di-photon,MET,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-18@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1706.03948@linkEnd@1706.03948@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1604888@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevD.96.112004@linkEnd@DOI:10.1103/PhysRevD.96.112004@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.96.112004@linkEnd@Phys.%20Rev.%20D%2096%20(2017)%20112004@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7142','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7142','shortTitle':'HLeptons HBSM A to tau tau search 2015','fullTitle':'Search for Minimal Supersymmetric Standard Model Higgs bosons $H/A$ and for a $Z^{\\prime}$ boson in the $\\tau \\tau$ final state produced in $pp$ collisions at $\\sqrt{s}=13$~!TeV with the ATLAS Detector','pubShortTitle':'Search BSM A/H/Z->tautau','refCode':'HIGG-2015-08','abstract':'A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) and for a heavy neutral $Z^{\\prime}$ boson is performed using a data sample corresponding to an integrated luminosity of 3.2~fb$^{-1}$ from proton--proton collisions at $\\sqrt{s } = 13$~TeV recorded by the ATLAS detector at the LHC.  The heavy resonance is assumed to decay to a $\\tau^+ \\tau^-$ pair with at least one $\\tau$ lepton decaying to final states with hadrons and a neutrino. The search is performed in the mass range of 0.2--1.2~TeV for the MSSM neutral Higgs bosons and 0.5--2.5~TeV for the heavy neutral $Z^{\\prime}$ boson.  The data are in good agreement with the background predicted by the Standard Model and hence results are given as upper limits on the production cross section times branching fraction of the boson decay to $\\tau^+\\tau^-$ as a function of the boson mass.  The results are interpreted in  MSSM and $Z^{\\prime}$ benchmark scenarios.  The most stringent MSSM parameter space constraints for the Higgs boson search exclude at 95\\% confidence level (CL) $\\tan\\beta > 7.6$ for $m_A = 200$~GeV in the $m_{h}^{\\textrm{mod+}}$ MSSM scenario.   This analysis extends the MSSM limits from previous searches for the mass range $m_A > 500$~GeV. For the Sequential Standard Model, a $Z^{\\prime}_\\mathrm{SSM}$ mass up to 1.90~TeV is excluded at 95\\% CL and masses up to 1.82--2.17~TeV are excluded for a $Z^{\\prime}_{\\mathrm{SFM}}$ of the Strong Flavour Model.','cdsLink':'','journal':'EPJC','journalSub':'02-AUG-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,BSM Higgs searches,BSM resonance,Higgs to tautau,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2015-08/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1608.00890@linkEnd@1608.00890@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1478983@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://doi.org/10.1140/epjc/s10052-016-4400-6@linkEnd@DOI:10.1140/epjc/s10052-016-4400-6@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-016-4400-6@linkEnd@Eur.%20Phys.%20J.%20C%2076%20(2016)%20585@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8122','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8122','shortTitle':'DBL - Run 2 V-gamma resonances','fullTitle':'Search for heavy resonances decaying to a $Z$ boson and a photon in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search for a resonance decaying to Z plus a photon','refCode':'EXOT-2016-02','abstract':'This Letter presents a search for new resonances with mass larger than 250 GeV, decaying to a $Z$ boson and a photon. The dataset consists of an integrated luminosity of 3.2 fb$^{-1}$ of $pp$ collisions collected at $\\sqrt{s } = 13$ TeV with the ATLAS detector at the Large Hadron Collider. The $Z$ bosons are identified through their decays either to charged,  light, lepton pairs ($e^+e^-$, $\\mu^+\\mu^-$) or to hadrons. The data are found to be consistent with the expected background in the whole mass range investigated and upper limits are set on the production cross section times decay branching ratio to $Z\\gamma$ of a narrow scalar boson with mass between 250 GeV and 2.75 TeV.','cdsLink':'','journal':'PLB','journalSub':'21-JUL-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,Higgs to Z+photon,Other new particle searches,Heavy vector triplets,BSM resonance,BSM search,Vphoton,Photon,Z,Boosted,2 jets,1 jet,Photons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-02/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1607.06363@linkEnd@1607.06363@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1477403@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2016.11.005@linkEnd@DOI:10.1016/j.physletb.2016.11.005@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269316306669@linkEnd@Phys.%20Lett.%20B%20764%20(2017)%2011@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'6658','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=6658','shortTitle':'DBL - Run 2 VH search','fullTitle':'Search for new resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $\\ell^+ \\ell^- b\\bar b$, $\\ell \\nu b\\bar b$, and $\\nu\\bar{\\nu} b\\bar b$ channels with $pp$ collisions at $\\sqrt s = 13$ TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VH to ll/lv/vv plus bb final state','refCode':'EXOT-2015-18','abstract':'A search is presented for new resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $\\ell^+ \\ell^- b\\bar b$, $\\ell\\nu b\\bar b$, and $\\nu\\bar{\\nu} b\\bar b$ channels in $pp$ collisions at $\\sqrt s = 13$ TeV with the ATLAS detector at the Large Hadron Collider using a total integrated luminosity of 3.2 fb$^{-1}$. The search is conducted by looking for a localized excess in the $WH$/$ZH$ invariant or transverse mass distribution. No significant excess is observed, and the results are interpreted in terms of constraints on a simplified model based on a phenomenological Lagrangian of heavy vector triplets.','cdsLink':'','journal':'PLB','journalSub':'19-JUL-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,Heavy vector triplets,BSM resonance,BSM search,VH,Boosted,MET,b-jets,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2015-18/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1607.05621@linkEnd@1607.05621@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1477027@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2016.11.045@linkEnd@DOI:10.1016/j.physletb.2016.11.045@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269316307080@linkEnd@Physics%20Letters%20B%20765(2017)%2032-52@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7926','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7926','shortTitle':'HBSM H to phi gamma','fullTitle':'Search for Higgs and $Z$ Boson Decays to $\\phi\\,\\gamma$ with the ATLAS Detector','pubShortTitle':'Search H(125)/Z->phi gamma','refCode':'HIGG-2016-05','abstract':'A search for the decays of the Higgs and $Z$ bosons to a $\\phi$ meson and a photon is performed with a $pp$ collision data sample corresponding to an integrated luminosity of $2.7\\,\\mathrm{fb}^{-1}$ collected at $\\sqrt{s}=13\\mathrm{TeV}$ with the ATLAS detector at the LHC. No significant excess of events is observed above the background, and 95% confidence level upper limits on the branching fractions of the Higgs and $Z$ boson decays to $\\phi\\,\\gamma$ of $1.4\\times10^{-3}$ and $8.3\\times10^{-6}$, respectively, are obtained.','cdsLink':'','journal':'PRL','journalSub':'12-JUL-16','ecm':'13','luminosity':'2.5 fb-1','keywords':'13 TeV,Exotic Higgs decays,Higgs to meson+photon,Photons,Charged tracks','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-05/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1607.03400@linkEnd@1607.03400@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1475286@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.117.111802@linkEnd@DOI:10.1103/PhysRevLett.117.111802@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.117.111802@linkEnd@Phys.%20Rev.%20Lett.%20117%2C%20111802@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7702','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7702','shortTitle':'HBSM H to 2a to 4b','fullTitle':'Search for the Higgs boson produced in association with a $W$ boson and decaying to four $b$-quarks via two spin-zero particles in $pp$ collisions at 13 TeV with the ATLAS detector','pubShortTitle':'Search BSM H->2a->4b','refCode':'HIGG-2016-01','abstract':'This paper presents a dedicated search for exotic decays of the Higgs boson to a pair of new spin-zero particles, $H \\rightarrow aa$, where the particle $a$ decays to $b$-quarks and has a mass in the range of 20-60 GeV. The search is performed in events where the Higgs boson is produced in association with a $W$ boson, giving rise to a signature of a lepton (electron or muon), missing transverse momentum, and multiple jets from $b$-quark decays. The analysis is based on the full dataset of $pp$ collisions at $\\sqrt{s } = 13$ TeV recorded in 2015 by the ATLAS detector at the CERN Large Hadron Collider, corresponding to an integrated luminosity of 3.2 fb$^{-1}$. No significant excess of events above the Standard Model prediction is observed, and a $95\\%$ confidence-level upper limit is derived for the product of the production cross section for $pp \\rightarrow WH$ times the branching ratio for the decay $H \\rightarrow aa \\rightarrow 4b$. The upper limit ranges from 6.2 pb for an $a$-boson mass $m_a = 20$ GeV to 1.5 pb for $m_a = 60$ GeV.','cdsLink':'','journal':'EPJC','journalSub':'27-JUN-16','ecm':'13','luminosity':'3.3 fb-1','keywords':'13 TeV,NMSSM,Exotic Higgs decays,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-01/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1606.08391@linkEnd@1606.08391@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1472323@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-016-44@linkEnd@DOI:10.1140/epjc/s10052-016-4418-9@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-016-4418-9@linkEnd@Eur.%20Phys.%20J.%20C%2076%20(2016)%20605@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7944','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7944','shortTitle':'DBL - Run 2 VV resonances','fullTitle':'Searches for heavy diboson resonances in pp collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'VV heavy resonance search combination','refCode':'EXOT-2016-01','abstract':'Searches for new heavy resonances decaying to $WW$, $WZ$, and $ZZ$ bosons are presented, using a data sample corresponding to 3.2 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=13$ TeV collected with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting $\\nu\\nu qq$, $\\ell\\nu qq$, $\\ell\\ell qq$ and $qqqq$ final states are combined, searching for a narrow-width resonance with mass between 500 and 3000 GeV. The discriminating variable is either an invariant mass or a transverse mass. No significant deviations from the Standard Model predictions are observed. Three benchmark models are tested: a model predicting the existence of a new heavy scalar singlet, a simplified model predicting a heavy vector-boson triplet, and a bulk Randall-Sundrum model with a heavy spin-2 graviton. Cross-section limits are set at the 95% confidence level and are compared to theoretical cross-section predictions for a variety of models. The data exclude a scalar singlet with mass below 2650 GeV, a heavy vector-boson triplet with mass below 2600 GeV, and a graviton with mass below 1100 GeV. These results significantly extend the previous limits set using $pp$ collisions at $\\sqrt{s}=8$ TeV.','cdsLink':'','journal':'JHEP','journalSub':'15-JUN-16','ecm':'13','luminosity':'3.2 pb-1','keywords':'13 TeV,Other new particle searches,Heavy vector triplets,BSM resonance,BSM search,Statistical combination,ZZ,WZ,WW,Boosted,All hadronic,2 jets,1 jet,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2016-01/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1606.04833@linkEnd@1606.04833@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1469453@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP09(2016)173@linkEnd@DOI:10.1007/JHEP09(2016)173@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP09(2016)173@linkEnd@JHEP%2009%20(2016%20)173@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'6651','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=6651','shortTitle':'JDM - Run 2 HH->4b search','fullTitle':'Search for pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using proton - proton collisions at $\\sqrt{s } = 13$ TeV with the ATLAS detector','pubShortTitle':'Search for HH to bbbb','refCode':'EXOT-2015-11','abstract':'A search for Higgs-boson pair production in the $b\\bar{b}b\\bar{b}$ final state  is carried out with 3.2~fb$^{-1}$ of proton--proton collision data collected at  $\\sqrt{s } = 13$ TeV with the ATLAS detector. The data are consistent with the estimated background and are used to set upper limits on the production cross section of Higgs-boson pairs times  branching ratio to $b\\bar{b}b\\bar{b}$ for both nonresonant and resonant production. In the case of resonant production of Kaluza--Klein gravitons within the Randall--Sundrum model, upper limits in the 24 to 91 fb range are  obtained for masses between 600 and 3000 GeV, at the 95% confidence level. The production cross section times branching ratio for nonresonant Higgs-boson pairs  is also constrained to be less than 1.22 pb, at the 95% confidence level.','cdsLink':'','journal':'PRD','journalSub':'15-JUN-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,Strong gravity,Di-Higgs production,BSM search,Di-Higgs,Boosted,b-jets,>=3 jets,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2015-11/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1606.04782@linkEnd@1606.04782@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1469452@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.94.052002@linkEnd@DOI:10.1103/PhysRevD.94.052002@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.94.052002@linkEnd@Phys.%20Rev.%20D%2094%20(2016)%20052002@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'8003','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=8003','shortTitle':'HGam LPX high mass diphoton 2015','fullTitle':'Search for resonances in diphoton events at $\\sqrt{s}$=13 TeV with the ATLAS detector','pubShortTitle':'Search BSM H/X->gammagamma','refCode':'HIGG-2016-08','abstract':'Searches for new resonances decaying into two photons in the ATLAS experiment at the CERN Large Hadron Collider are described. The analysis is based on proton--proton collision data corresponding to an integrated luminosity of 3.2 fb$^{-1}$ at $\\sqrt{s } = 13$ TeV recorded in 2015. Two searches are performed, one targeted at a spin-2 particle of mass larger than 500 GeV, using Randall--Sundrum graviton states as a benchmark model, and one optimized for a spin-0 particle of mass larger than 200 GeV. Varying both the mass and the decay width, the most significant deviation from the background-only hypothesis is observed at a diphoton invariant mass around 750 GeV with local significances of 3.8 and 3.9 standard deviations in the searches optimized for a spin-2 and spin-0 particle, respectively. The global significances are estimated to be 2.1 standard deviations for both analyses. The consistency between the data collected at 13 TeV and 8 TeV is also evaluated. Limits on the production cross section times branching ratio to two photons for the two  resonance types are reported.','cdsLink':'','journal':'JHEP','journalSub':'13-JUN-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,BSM Higgs searches,Strong gravity,BSM resonance,Higgs to 2 photons,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2016-08/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1606.03833@linkEnd@1606.03833@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1469066@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP09(2016)001@linkEnd@DOI:10.1007/JHEP09(2016)001@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP09(2016)001@linkEnd@JHEP%2009%20(2016)%20001@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7222','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7222','shortTitle':'LFV H tau lep combined and Z tau mu','fullTitle':'Search for lepton-flavour-violating decays of the Higgs and $Z$ bosons with the ATLAS detector','pubShortTitle':'Search BSM H(125)->tau l (l=e,mu)  flavor violating decay','refCode':'HIGG-2015-09','abstract':'Direct searches for lepton flavour violation in decays of the Higgs and $Z$ bosons with the ATLAS detector at the LHC are presented. The following three decays are considered: $H\\to e\\tau$, $H\\to\\mu\\tau$, and $Z\\to\\mu\\tau$. The searches are based on the data sample of proton--proton collisions collected by the ATLAS detector corresponding to an integrated luminosity of 20.3 fb$^{-1}$ at a centre-of-mass energy of $\\sqrt{s } = 8$ TeV. No significant excess is observed, and upper limits on the lepton-flavour-violating branching ratios are set at the 95% confidence level: Br$(H\\to e\\tau) <$ 1.04%, Br$(H\\to\\mu\\tau) <$ 1.43%, and Br$(Z\\to\\mu\\tau) <$ 1.69 $\\times$ 10$^{-5}$.','cdsLink':'','journal':'EPJC','journalSub':'26-APR-16','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Exotic Higgs decays,LFV,Taus,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2015-09/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1604.07730@linkEnd@1604.07730@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1452557@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-017-4624-0@linkEnd@DOI:10.1140/epjc/s10052-017-4624-0@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-017-4624-0@linkEnd@Eur.%20Phys.%20J.%20C%2077%20(2017)%2070@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'7302','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=7302','shortTitle':'HBSM charged Higgs to tau nu','fullTitle':'Search for charged Higgs bosons produced in association with a top quark and decaying via $H^{\\pm} \\rightarrow \\tau\\nu$ using $pp$ collision data recorded at $\\sqrt{s } = 13$ TeV by the ATLAS detector','pubShortTitle':'Search BSM H+ -> tau nu','refCode':'HIGG-2015-11','abstract':'Charged Higgs bosons produced in association with a single top quark and decaying via $H^{\\pm} \\rightarrow \\tau\\nu$ are searched for with the ATLAS experiment at the LHC, using proton--proton collision data at $\\sqrt{s } = 13$ TeV corresponding to an integrated luminosity of 3.2 $\\mathrm{fb}^{-1}$. The final state is characterised by the presence of a hadronic $\\tau$ decay and missing transverse momentum, as well as a hadronically decaying top quark, resulting in the absence of high-transverse-momentum electrons and muons. The data are found to be consistent with the expected background from Standard Model processes. A statistical analysis leads to 95% confidence-level upper limits on the production cross section times branching fraction, $\\sigma(pp \\rightarrow [b]t H^{\\pm}) \\times \\mbox{BR}(H^{\\pm} \\rightarrow \\tau\\nu)$, between 1.9 pb and 15 fb, for charged Higgs boson masses ranging from 200 to 2000 GeV. The exclusion limits for this search surpass those obtained with the proton--proton collision data recorded at $\\sqrt{s } = 8$ TeV.','cdsLink':'','journal':'PLB','journalSub':'30-MAR-16','ecm':'13','luminosity':'3.2 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM Higgs searches,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2015-11/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1603.09203@linkEnd@1603.09203@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1436496@linkEnd@Inspire@descriptionEnd@ ','run':'2','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2016.06.017@linkEnd@DOI:10.1016/j.physletb.2016.06.017@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269316302702@linkEnd@Phys.%20Lett.%20B%20759%20(2016)%20555-574@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5862','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5862','shortTitle':'DBL - diboson combination','fullTitle':'Combination of searches for $WW$, $WZ$, and $ZZ$ resonances in $pp$ collisions at $\\sqrt{s } = 8$ TeV with the ATLAS detector','pubShortTitle':'VV heavy resonance search combination','refCode':'EXOT-2014-18','abstract':'The ATLAS experiment at the CERN Large Hadron Collider has performed searches for new, heavy bosons decaying to $WW$, $WZ$ and $ZZ$ final states in multiple decay channels using 20.3 fb^{-1} of $pp$ collision data at $\\sqrt{s } = 8$ TeV. In the current study, the results of these searches are combined to provide a more stringent test of models predicting heavy resonances with couplings to vector bosons. Direct searches for a charged diboson resonance decaying to WZ in the $\\ell\\nu\\ell\\ell$ ($\\ell = \\mu, e$) , $\\ell\\ell q \\bar{q}$, $\\ell \\nu q \\bar{q}$ and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the $WZ$ bosons are compared with predictions of an extended gauge model with a heavy $W$ boson. In addition, direct searches for a neutral diboson resonance decaying to $WW$ and $ZZ$ in the $\\ell \\ell q \\bar{q}$, $\\ell \\nu q \\bar{q}$, and fully hadronic final states are combined and upper limits on the rate of production times branching ratio to the $WW$ and $ZZ$ bosons are compared with predictions for a heavy, spin-2 graviton in an extended Randall--Sundrum model where the Standard Model fields are allowed to propagate in the bulk of the extra dimension.','cdsLink':'','journal':'PLB','journalSub':'16-DEC-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,Strong gravity,BSM resonance,BSM reinterpretation,BSM search,Statistical combination,ZZ,WZ,WW,Boosted,MET,>=3 jets,2 jets,1 jet,0 jets,>=3 leptons,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2014-18/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1512.05099@linkEnd@1512.05099@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1409918@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2016.02.015@linkEnd@DOI:10.1016/j.physletb.2016.02.015@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269316001118@linkEnd@Phys.%20Lett.%20B%20755%20(2016)%20285-305@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4705','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4705','shortTitle':'HSG8 Heavy charged Higgs tb','fullTitle':'Search for charged Higgs bosons in the $H^{\\pm} \\rightarrow tb$ decay channel in $pp$ collisions at $\\sqrt{s } = 8$ TeV using the ATLAS detector','pubShortTitle':'Search BSM H+ -> tb','refCode':'HIGG-2013-28','abstract':'Charged Higgs bosons heavier than the top quark and decaying via $H^{\\pm} \\rightarrow tb$ are searched for in proton--proton collisions measured with the ATLAS experiment at $\\sqrt{s}=8$ TeV corresponding to an integrated luminosity of 20.3 fb$^{-1}$. The production of a charged Higgs boson in association with a top quark, $gb \\rightarrow tH^{\\pm}$, is explored in the mass range 200 to 600 GeV using multi-jet final states with one electron or muon. In order to separate the signal from the Standard Model background, analysis techniques combining several kinematic variables are employed. An excess of events above the background-only hypothesis is observed across a wide mass range, amounting to up to 2.4 standard deviations. Upper limits are set on the $gb\\rightarrow tH^{\\pm}$ production cross section times the branching fraction $\\mathrm{BR}(H^{\\pm} \\rightarrow tb)$. Additionally, the complementary $s$-channel production, $qq \\rightarrow H^{\\pm}$, is investigated through a reinterpretation of $W \\rightarrow tb$ searches in ATLAS. Final states with one electron or muon are relevant for $H^{\\pm}$ masses from 0.4 to 2.0 TeV, whereas the all-hadronic final state covers the range 1.5 to 3.0 TeV. In these search channels, no significant excesses from the predictions of the Standard Model are observed, and upper limits are placed on the $qq \\rightarrow H^{\\pm}$ production cross section times the branching fraction BR$(H^{\\pm} \\rightarrow tb)$.','cdsLink':'','journal':'JHEP','journalSub':'11-DEC-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Charged Higgs searches,BSM Higgs searches,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-28/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1512.03704@linkEnd@1512.03704@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1409300@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP03(2016)127@linkEnd@DOI:10.1007/JHEP03(2016)127@descriptionEnd@,@linkBegin@https://dx.doi.org/10.1007/JHEP03(2016)127@linkEnd@JHEP%2003%20(2016)%20127@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4742','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4742','shortTitle':'LPX - Multiphoton search 8 TeV','fullTitle':'Search for new phenomena in events with at least three photons collected in $pp$ collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector','pubShortTitle':'Search for new phenomena with at least three photons','refCode':'EXOT-2013-24','abstract':'Results of a search for new phenomena in events with at least three photons are reported. Data from proton--proton collisions at a centre-of-mass energy of 8 TeV, corresponding to an integrated luminosity of 20.3 fb$^{-1}$, were collected with the ATLAS detector at the LHC. The observed data are well described by the Standard Model. Limits at the 95% confidence level on new phenomena are presented based on the rate of events in an inclusive signal region and a restricted signal region targeting the rare decay $Z\\to 3\\gamma$, as well as di-photon and tri-photon resonance searches. For a Standard Model Higgs boson decaying to four photons via a pair of intermediate pseudoscalar particles ($a$), limits are found to be $\\sigma \\times {\\text {BR}}(h \\rightarrow aa) \\times {\\text {BR}}(a \\rightarrow \\gamma \\gamma)^{2} < 10^{-3} \\sigma_{\\text{SM}}$ for 10 GeV $< m_{a} <$ 62 GeV. Limits are also presented for Higgs boson-like scalars ($H$) for $m_{H} >$ 125 GeV, and for a $Z$ decaying to three photons via $Z \\rightarrow a+\\gamma \\rightarrow 3\\gamma$. Additionally, the observed limit on the branching ratio of the $Z$ boson decay to three photons is found to be BR$(Z \\rightarrow 3\\gamma) < 2.2 \\times 10^{-6}$, a result five times stronger than the previous result from LEP.','cdsLink':'','journal':'EPJC','journalSub':'16-SEP-15','ecm':'8','luminosity':'20.3 fb-1','keywords':'8 TeV,Exotic Higgs decays,BSM Higgs searches,BSM resonance,Rare decays,BSM search,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-24/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1509.05051@linkEnd@1509.05051@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1393757@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-016-4034-8@linkEnd@DOI:10.1140/epjc/s10052-016-4034-8@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-016-4034-8@linkEnd@Eur.%20Phys.%20J.%20C%2076%20(2016)%20210@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4783','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4783','shortTitle':'HSG6 Higgs to HH Channels','fullTitle':'Searches for Higgs boson pair production in the $HH\\to bb\\tau\\tau, \\gamma\\gamma WW*, \\gamma\\gamma bb, bbbb$ channels with the ATLAS detector','pubShortTitle':'Search BSM HH->bb gamma gamma, bb bb, bb tautau, gamma gamma WW','refCode':'HIGG-2013-33','abstract':'Searches for both resonant and non-resonant Higgs boson pair production are performed in the $hh\\to bb\\tau\\tau, \\gamma\\gamma WW^*$ final states using 20.3 fb$^{-1}$ of $pp$ collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. No evidence of their production is observed and 95% confidence level upper limits on the production cross sections are set. These results are then combined with the published results of the $hh\\to \\gamma\\gamma bb, bbbb$ analyses. An upper limit of 0.69 (0.47) pb on the non-resonant Standard Model like $hh$ production is observed (expected), corresponding to 70 (48) times of the SM $gg\\to hh$ cross section. For production via narrow resonances, cross section limits of $hh$ production from a heavy Higgs boson decay are set as a function of the heavy Higgs boson mass. The observed (expected) limits range from 2.1 (1.1) pb at 260 GeV to 0.011 (0.018) pb at 1000 GeV. These results are interpreted in the context of two simplified scenarios of the Minimal Supersymmetric Standard Model.','cdsLink':'','journal':'PRD','journalSub':'15-SEP-15','ecm':'7, 8','luminosity':'25 fb-1','keywords':'7 TeV,BSM Higgs searches,Di-Higgs production,Statistical combination,Di-Higgs,Di-photon,WW,b-jets,Photons,Taus,1 lepton,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-33/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1509.04670@linkEnd@1509.04670@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1393493@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.92.092004@linkEnd@DOI:10.1103/PhysRevD.92.092004@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.92.092004@linkEnd@Phys.%20Rev.%20D%2092%2C%20092004%20(2015)@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'6244','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=6244','shortTitle':'HSG6 HSG7 BSM coupling interpretation','fullTitle':'Constraints on new phenomena via Higgs boson couplings and invisible decays with the ATLAS detector','pubShortTitle':'Search HBSM H/A constraints from combined H(125) measurements and invisible decays','refCode':'HIGG-2015-03','abstract':'The ATLAS experiment at the LHC has measured the Higgs boson couplings and mass, and searched for invisible Higgs boson decays, using multiple production and decay channels with up to 4.7 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}= 7$ TeV and 20.3 fb$^{-1}$ at $\\sqrt{s}=8$ TeV. In the current study, the measured production and decay rates of the observed Higgs boson in the $\\gamma\\gamma$, $ZZ$, $WW$, $Z\\gamma$, $bb$, $\\tau\\tau$, and $\\mu\\mu$ decay channels, along with results from the associated production of a Higgs boson with a top-quark pair, are used to probe the scaling of the couplings with mass. Limits are set on parameters in extensions of the Standard Model including a composite Higgs boson, an additional electroweak singlet, and two-Higgs-doublet models. Together with the measured mass of the scalar Higgs boson in the $\\gamma\\gamma$ and $ZZ$ decay modes, a lower limit is set on the pseudoscalar Higgs boson mass of $m_{A}>370$ GeV in the hMSSM simplified Minimal Supersymmetric Standard Model. Results from direct searches for heavy Higgs bosons are also interpreted in the hMSSM. Direct searches for invisible Higgs boson decays in the vector-boson fusion and associated production of a Higgs boson with $W/Z$ ($Z\\to ll$, $W/Z \\to jj$) modes are statistically combined to set an upper limit on the Higgs boson invisible branching ratio of 0.25. The use of the measured visible decay rates in a more general coupling fit improves the upper limit to 0.23, constraining a Higgs portal model of dark matter.','cdsLink':'','journal':'JHEP','journalSub':'02-SEP-15','ecm':'7, 8','luminosity':'4.7 fb-1, 20.3 fb-1','keywords':'7 TeV,Exotic Higgs decays,BSM Higgs searches,Higgs to invisible,BSM reinterpretation,Statistical combination,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2015-03/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1509.00672@linkEnd@1509.00672@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1391509@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP11%282015%29206@linkEnd@DOI:10.1007/JHEP11(2015)206@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP11%282015%29206@linkEnd@JHEP11(2015)206@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4628','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4628','shortTitle':'HSG3 HSG6 Heavy Higgs Search','fullTitle':'Search for a high-mass Higgs boson decaying to a $W$ boson pair in $pp$ collisions at $\\sqrt{s } = 8$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H/X-> W W','refCode':'HIGG-2013-19','abstract':'A search for a high-mass Higgs boson $H$ is performed in the $H\\to WW\\to\\ell\\nu\\ell\\nu$ and $H\\to WW\\to \\ell\\nu{qq}$ decay channels using $pp$ collision data corresponding to an integrated luminosity of 20.3 fb$^{-1}$ collected at $\\sqrt{s}=$ 8 TeV by the ATLAS detector at the Large Hadron Collider. No evidence of a high-mass Higgs boson is found. Limits on $\\sigma_H\\times \\mathrm{BR}(H\\to WW)$ as a function of the Higgs boson mass $m_H$ are determined in three different scenarios: one in which the heavy Higgs boson has a narrow width compared to the experimental resolution, one for a width increasing with the boson mass and modeled by the complex-pole scheme following the same behavior as in the Standard Model, and one for intermediate widths. The upper range of the search is $m_H=1500$ GeV for the narrow-width scenario and $m_H=1000$ GeV for the other two scenarios. The lower edge of the search range is $200$--$300$ GeV and depends on the analysis channel and search scenario. For each signal interpretation, individual and combined limits from the two $WW$ decay channels are presented. At $m_{H } = 1500$ GeV, the highest-mass point tested, $\\sigma_H\\times\\mathrm{BR}(H\\rightarrow WW)$ for a narrow-width Higgs boson is constrained to be less than 21 fb and 6.0 fb at 95% CL for the gluon fusion and vector-boson fusion production modes, respectively.','cdsLink':'','journal':'JHEP','journalSub':'01-SEP-15','ecm':'7, 8','luminosity':'25 fb-1','keywords':'7 TeV,BSM Higgs searches,Higgs to WW,WW,2 jets,2 leptons,1 lepton,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-19/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1509.00389@linkEnd@1509.00389@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1391323@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP01%282016%29032@linkEnd@DOI@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP01%282016%29032@linkEnd@JHEP%2001%20(2016)%20032@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4629','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4629','shortTitle':'HSG2 High Mass Search','fullTitle':'Search for an additional, heavy Higgs boson in the $H\\rightarrow ZZ$ decay channel at $\\sqrt{s}$ = 8 TeV in $pp$ collision data with the ATLAS detector','pubShortTitle':'Search BSM H -> ZZ','refCode':'HIGG-2013-20','abstract':'A search is presented for a high-mass Higgs boson in the $H\\rightarrow\\ell\\ell\\ell\\ell$, $H\\rightarrow\\ell\\ell\\nu\\nu$, $H\\rightarrow\\ell\\ell qq$, and $H\\rightarrow\\nu\\nu qq$ decay modes using the ATLAS detector at the CERN Large Hadron Collider. The search uses proton-proton collision data at a centre-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20.3 fb$^{-1}$. The results of the search are interpreted in the scenario of a heavy Higgs boson with a width that is small compared with the experimental mass resolution. The Higgs boson mass range considered extends up to 1 TeV for all four decay modes and down to as low as 140 GeV, depending on the decay mode. No significant excess of events over the Standard Model prediction is found. A simultaneous fit to the four decay modes yields upper limits on the production cross-section of a heavy Higgs boson times the branching ratio to Z boson pairs. 95% confidence level upper limits range from 0.53 pb at $m_H=195$ GeV to 0.008 pb at $m_H=950$ GeV for the gluon-fusion production mode and from 0.31 pb at $m_H=195$ GeV to 0.009 pb at $m_H=950$ GeV for the vector-boson-fusion production mode. The results are also interpreted in the context of Type-I and Type-II two-Higgs-doublet models.','cdsLink':'','journal':'EPJC','journalSub':'21-JUL-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM Higgs searches,VBF production,Gluon fusion production,Higgs to ZZ,Higgs to 4 lepton,BSM search,VBF,Gluon fusion,Higgs,ZZ,MET,2 jets,>=3 leptons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-20/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1507.05930@linkEnd@1507.05930@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1384120@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-015-3820-z@linkEnd@DOI:10.1140/epjc/s10052-015-3820-z@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3820-z@linkEnd@Eur.%20Phys.%20J.%20C76%20(2016)%2045@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5363','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5363','shortTitle':'HSG1 HSG6 DM and Higgs diphoton MET','fullTitle':'Search for Dark Matter in Events with Missing Transverse Momentum and a Higgs Boson Decaying to Two Photons in $pp$ Collisions at $\\sqrt{s}=8$ TeV with the ATLAS Detector','pubShortTitle':'Search BSM H(125)->gamma gamma + missing-ET','refCode':'HIGG-2014-05','abstract':'Results of a search for new phenomena in events with large missing transverse momentum and a Higgs boson decaying to two photons are reported. Data from proton--proton collisions at a center-of-mass energy of 8 TeV and corresponding to an integrated luminosity of 20.3 fb$^{-1}$ have been collected with the ATLAS detector at the LHC. The observed data are well described by the expected Standard Model backgrounds. Upper limits on the cross section of events with large missing transverse momentum and a Higgs boson candidate are also placed. Exclusion limits are presented for models of physics beyond the Standard Model featuring dark-matter candidates.','cdsLink':'','journal':'PRL','journalSub':'02-JUN-15','ecm':'8','luminosity':'20.3 fb-1','keywords':'7 TeV,Simplified DM model,BSM Higgs searches,Higgs to 2 photons,Dark matter,Di-photon,MET,Photons,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-05/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1506.01081@linkEnd@1506.01081@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1374488@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.115.131801@linkEnd@DOI:10.1103/PhysRevLett.115.131801@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.131801@linkEnd@Phys.%20Rev.%20Lett.%20115%20(2015)%20131801@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3924','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3924','shortTitle':'DBL - W to WZ in 2 J','fullTitle':'Search for high-mass diboson resonances with boson-tagged jets in proton--proton collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV hadronic final state','refCode':'EXOT-2013-08','abstract':'A search is performed for narrow resonances decaying into $WW$, $WZ$, or $ZZ$ boson pairs using 20.3 fb$^{-1}$ of proton--proton collision data at a centre-of-mass energy of $\\sqrt{s}$ = 8 TeV recorded with the ATLAS detector at the Large Hadron Collider. Diboson resonances with masses in the range from 1.3 to 3.0 TeV are sought after using the invariant mass distribution of dijets where both jets are tagged as a boson jet, compatible with a highly boosted $W$ or $Z$ boson decaying to quarks, using jet mass and substructure properties. The largest deviation from a smoothly falling background in the observed dijet invariant mass distribution occurs around 2 TeV in the $WZ$ channel, with a global significance of 2.5 standard deviations. Exclusion limits at the 95% confidence level are set on the production cross section times branching ratio for the $WZ$ final state of a new heavy gauge boson, $W$, and for the $WW$ and $ZZ$ final states of Kaluza--Klein excitations of the graviton in a bulk Randall--Sundrum model, as a function of the resonance mass. $W$ bosons with couplings predicted by the extended gauge model in the mass range from 1.3 to 1.5 TeV are excluded at 95% confidence level.','cdsLink':'','journal':'JHEP','journalSub':'02-JUN-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,Strong gravity,BSM resonance,BSM search,ZZ,WZ,WW,Boosted,All hadronic,2 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-08/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1506.00962@linkEnd@1506.00962@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1374218@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP12%282015%29055@linkEnd@DOI@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP12%282015%29055@linkEnd@JHEP%2012%20(2015)%2055@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5562','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5562','shortTitle':'JTX - Diboson to 4b','fullTitle':'Search for Higgs boson pair production in the $b\\bar{b} b\\bar{b}$ final state from $pp$ collisions at $\\sqrt{s } = 8$ TeV with the ATLAS detector','pubShortTitle':'Search for HH to bbbb','refCode':'EXOT-2014-11','abstract':'A search for Higgs boson pair production $pp \\to hh$ is performed with 19.5 fb$^{-1}$ of proton--proton collision data at $\\sqrt{s}=$ 8 TeV, which were recorded by the ATLAS detector at the Large Hadron Collider in 2012. The decay products of each Higgs boson are reconstructed as a high-momentum $b\\bar{b}$ system with either a pair of small-radius jets or a single large-radius jet, the latter exploiting jet substructure techniques and associated $b$-tagged track-jets. No evidence for resonant or non-resonant Higgs boson pair production is observed. The data are interpreted in the context of the Randall--Sundrum model with a warped extra dimension as well as the two-Higgs-doublet model. An upper limit on the cross-section for $pp \\to G^{*}_{\\mathrm{KK}} \\to hh \\to b\\bar{b} b\\bar{b}$ of 3.2 (2.3) fb is set for a Kaluza--Klein graviton $G^{*}_{\\mathrm{KK}}$ mass of 1.0 (1.5) TeV, at the 95\\% confidence level. The search for non-resonant Standard Model $hh$ production sets an observed 95\\% confidence level upper limit on the production cross-section $\\sigma(pp \\to hh \\to b\\bar{b}b\\bar{b})$ of 202 fb, compared to a SM prediction of $\\sigma(pp \\to hh \\to b\\bar{b}b\\bar{b}) = 3.6 \\pm 0.5$ fb.','cdsLink':'','journal':'EPJC','journalSub':'31-MAY-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Exotic Higgs production,Strong gravity,Di-Higgs production,BSM search,Di-Higgs,Boosted,b-jets,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2014-11/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1506.00285@linkEnd@1506.00285@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1373912@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-015-3628-x@linkEnd@DOI:10.1140/epjc/s10052-015-3628-x@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3628-x@linkEnd@Eur.%20Phys.%20J.%20C%20%20(2015)%2075:412@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4342','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4342','shortTitle':'DBL - H to ZZd/ZdZd to 4 lepton','fullTitle':'Search for new light gauge bosons in Higgs boson decays to four-lepton final states in $pp$ collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector at the LHC','pubShortTitle':'H to ZdarkZdark or ZZdark search in the llll final state','refCode':'EXOT-2013-15','abstract':'This paper presents a search for Higgs bosons decaying to four leptons, either electrons or muons, via one or two light exotic gauge bosons $Z_d$, $H\\to Z Z_d \\to 4\\ell$ or $H\\to Z_d Z_d \\to 4\\ell$. The search was performed using $pp$ collision data corresponding to an integrated luminosity of about 20 fb$^{-1}$ at the center-of-mass energy of $\\sqrt{s}=8$TeV recorded with the ATLAS detector at the Large Hadron Collider. The observed data are well described by the Standard Model prediction. Upper bounds on the branching ratio of $H\\to Z Z_d \\to 4\\ell$ and on the kinetic mixing parameter between the $Z_d$ and the Standard Model hypercharge gauge boson are set in the range $(1$--$9)\\times10^{-5}$ and $(4$--$17)\\times10^{-2}$ respectively, at 95% confidence level assuming the Standard Model branching ratio of $H\\to Z Z^* \\to 4\\ell$, for $Z_d$ masses between 15 and 55 GeV. Upper bounds on the effective mass mixing parameter between the $Z$ and the $Z_d$ are also set using the branching ratio limits in the $H \\to ZZ_d\\to 4\\ell$ search, and are in the range $(1.5$--$8.7)\\times 10^{-4}$ for $15<m_{Z_d} < 35$ GeV. Upper bounds on the branching ratio of $H\\rightarrow Z_dZ_d \\to 4\\ell$ and on Higgs portal coupling parameter, controlling the strength of the coupling of the Higgs boson to dark vector bosons, are set in the range $(2$--$3)\\times10^{-5}$ and $(1$--$10)\\times 10^{-4}$ respectively, at 95 % confidence level assuming the Standard Model Higgs boson production cross sections, for $Z_d$ masses between 15 and 60 GeV.','cdsLink':'','journal':'PRD','journalSub':'28-MAY-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Exotic Higgs decays,Dark sector,BSM search,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-15/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1505.07645@linkEnd@1505.07645@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1373520@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.92.092001@linkEnd@DOI@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.92.092001@linkEnd@Phys.%20Rev.%20D%2092%20(2015)%20092001@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5182','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5182','shortTitle':'HSG6 h to 2a to tautau mumu','fullTitle':'Search for Higgs bosons decaying to aa in the mumutautau final-state in pp collisions  at sqrt(s) = 8 TeV with the ATLAS experiment','pubShortTitle':'Search BSM H->2a->tau tau mu mu','refCode':'HIGG-2014-02','abstract':'A search for the decay to a pair of new particles of either the 125 GeV Higgs boson ($h$) or a second CP-even Higgs boson ($H$) is presented. The dataset correspods to an integrated luminosity of 20.3 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=$ 8 TeV recorded by the ATLAS experiment at the LHC in 2012. The search was done in the context of the next-to-minimal supersymmetric standard model, in which the new particles are the lightest neutral pseudoscalar Higgs bosons ($a$). One of the two $a$ bosons is required to decay to two muons while the other is required to decay to two $\\tau$-leptons. No significant excess is observed above the expected backgrounds in the dimuon invariant mass range from 3.7 GeV to 50 GeV. Upper limits are placed on the production of $h\\rightarrow{aa}$ relative to the Standard Model $gg\\rightarrow{h}$ production, assuming no coupling of the $a$ boson to quarks. The most stringent limit is placed at 3.5% for $m_a =$ 3.75 GeV. Upper limits are also placed on the production cross section of $H\\rightarrow{aa}$ from 2.33 pb to 0.72 pb, for fixed $m_a$ = 5 GeV with $m_H$ ranging from 100 GeV to 500 GeV.','cdsLink':'','journal':'PRD','journalSub':'07-MAY-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,NMSSM,Exotic Higgs decays,Taus,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-02/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1505.01609@linkEnd@1505.01609@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1367302@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.92.052002@linkEnd@DOI:10.1103/PhysRevD.92.052002@descriptionEnd@,@linkBegin@https://journals.aps.org/prd/abstract/10.1103/PhysRevD.92.052002@linkEnd@Phys.%20Rev.%20D92%20(2015)%20052002@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3142','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3142','shortTitle':'LPX - Diphoton search 8 TeV','fullTitle':'Search for high-mass diphoton resonances in $pp$ collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector','pubShortTitle':'Search for high-mass diphoton resonances','refCode':'EXOT-2012-19','abstract':'This article describes a search for high-mass resonances decaying to a pair of photons using a sample of $20.3$ fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}=8$ TeV recorded with the ATLAS detector at the Large Hadron Collider. The data are found to be in agreement with the Standard Model prediction, and limits are reported in the framework of the Randall-Sundrum model. This theory leads to the prediction of graviton states, the lightest of which could be observed at the Large Hadron Collider. A lower limit of $2.66$ ($1.41$) TeV at 95% confidence level is set on the mass of the lightest graviton for couplings of $k/\\overline{M}_{\\mathrm{Pl} } = 0.1$ ($0.01$).','cdsLink':'','journal':'PRD','journalSub':'21-APR-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Strong gravity,BSM resonance,BSM search,Di-photon,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-19/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1504.05511@linkEnd@1504.05511@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1362490@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.92.032004@linkEnd@DOI:10.1103/PhysRevD.92.032004@descriptionEnd@,@linkBegin@https://link.aps.org/abstract/PRD/v92/e032004@linkEnd@Phys.%20Rev.%20D%2092%20(2015)%20032004%20@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4564','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4564','shortTitle':'HQT - SS dilepton/3-leptons with b-tags','fullTitle':'Analysis of events with $b$-jets and a pair of leptons of the same charge in $pp$ collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector','pubShortTitle':'Same-sign dilepton plus b-jet search','refCode':'EXOT-2013-16','abstract':'An analysis is presented of events containing jets including at least one $b$-tagged jet, sizeable missing transverse momentum, and at least two leptons including a pair of the same electric charge, with the scalar sum of the jet and lepton transverse momenta being large. A data sample with an integrated luminosity of 20.3 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s } = 8$ TeV recorded by the ATLAS detector at the Large Hadron Collider is used. Standard Model processes rarely produce these final states, but there are several models of physics beyond the Standard Model that predict an enhanced rate of production of such events; the ones considered here are production of vector-like quarks, enhanced four-top-quark production, pair production of chiral $b^\\prime$-quarks, and production of two positively charged top quarks. Eleven signal regions are defined; subsets of these regions are combined when searching for each class of models. In the three signal regions primarily sensitive to positively charged top quark pair production, the data yield is consistent with the background expectation. There are more data events than expected from background in the set of eight signal regions defined for searching for vector-like quarks and chiral $b^\\prime$-quarks, but the significance of the discrepancy is less than two standard deviations. The discrepancy reaches 2.5 standard deviations in the set of five signal regions defined for searching for four-top-quark production. The results are used to set 95% CL limits on various models.','cdsLink':'','journal':'JHEP','journalSub':'17-APR-15','ecm':'8','luminosity':'20.3 fb-1','keywords':'8 TeV,Compositeness,Heavy vector triplets,Vector-like quarks,Contact interactions,BSM resonance,Other top properties,Top properties measurements,BSM search,b-jets,>=3 jets,>=3 leptons,2 leptons (same charge)','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-16/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1504.04605@linkEnd@1504.04605@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1361912@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP10%282015%29150@linkEnd@DOI@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP10%282015%29150@linkEnd@JHEP%2010%20(2015)%20150@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5442','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5442','shortTitle':'HSG6 VH H invisible V to jj','fullTitle':'Search for invisible decays of the Higgs boson produced in association with a hadronically decaying vector boson in $pp$ collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector','pubShortTitle':'Search BSM VH(125)->invisible and V-> jet jet','refCode':'HIGG-2014-07','abstract':'A search for Higgs boson decays to invisible particles is performed using 20.3 fb$^{-1}$ of $pp$ collision data at a centre-of-mass energy of 8 TeV recorded by the ATLAS detector at the Large Hadron Collider. The process considered is Higgs boson production in association with a vector boson ($V$ = $W$ or $Z$) that decays hadronically, resulting in events with two or more jets and large missing transverse momentum. No excess of candidates is observed in the data over the background expectation. The results are used to constrain $VH$ production followed by $H$ decaying to invisible particles for the Higgs mass range $115<m_H<300$~GeV. The 95% confidence-level observed upper limit on $\\sigma_{VH} \\times \\text{BR}(H\\rightarrow \\text{inv.})$ varies from 1.6 pb at 115 GeV to 0.13 pb at 300 GeV. Assuming Standard Model production and including the $gg\\rightarrow H$ contribution as signal, the results also lead to an observed upper limit of 78% at 95% confidence level on the branching ratio of Higgs bosons decays to invisible particles at a mass of 125 GeV.','cdsLink':'','journal':'EPJC','journalSub':'16-APR-15','ecm':'7, 8','luminosity':'25 fb-1','keywords':'7 TeV,Exotic Higgs decays,Higgs to invisible,Dark matter,VH,Z,W,MET,All hadronic,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-07/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1504.04324@linkEnd@1504.04324@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1360288@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1','finalPubRef':'@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3551-1@linkEnd@DOI:%20%20%20%2010.1140/epjc/s10052-015-3551-1@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3551-1@linkEnd@Eur.%20Phys.%20J.%20C%20(2015)%2075:337@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4724','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4724','shortTitle':'DBL - VH->lv/vv/ll+bb','fullTitle':'Search for a new resonance decaying to a $W$ or $Z$ boson and a Higgs boson in the $\\ell \\ell/ \\ell \\nu/ \\nu \\nu + b \\bar{b}$ final states with the ATLAS Detector','pubShortTitle':'Resonance search in the VH to ll/lv/vv plus bb final state','refCode':'EXOT-2013-23','abstract':'A search for a new resonance decaying to a $W$ or $Z$ boson and a Higgs boson in the $\\ell \\ell/ \\ell \\nu/ \\nu \\nu + b \\bar{b}$ final states is performed using 20.3 fb$^{-1}$ of $pp$ collision data recorded at $\\sqrt{s}=$ 8 TeV with the ATLAS detector at the Large Hadron Collider. The search is conducted by examining the $WH/ZH$ invariant mass distribution for a localized excess. No significant deviation from the Standard Model background prediction is observed. The results are interpreted in terms of constraints on the Minimal Walking Technicolor model and on a simplified approach based on a phenomenological Lagrangian of Heavy Vector Triplets.','cdsLink':'','journal':'EPJC','journalSub':'27-MAR-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,BSM resonance,BSM search,VH,MET,b-jets,2 jets,2 leptons,1 lepton,0 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-23@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1503.08089@linkEnd@1503.08089@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1356730@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-015-3474-x@linkEnd@DOI:10.1140/epjc/s10052-015-3474-x@descriptionEnd@,@linkBegin@https://epjc.epj.org/articles/epjc/abs/2015/06/10052_2015_Article_3474/10052_2015_Article_3474.html@linkEnd@Eur.%20Phys.%20J.%20C%20(2015)%2075:%20263@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3642','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3642','shortTitle':'DBL - Diboson lvjj resonance 8 TeV','fullTitle':'Search for production of $WW/WZ$ resonances decaying to a lepton, neutrino and jets in $pp$ collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV to lvqq final state','refCode':'EXOT-2013-01','abstract':'A search is presented for a narrow diboson resonances decaying to $WW$ or $WZ$ in the final state where one $W$ boson decays leptonically (to an electron or a muon plus a neutrino) and the other $W/Z$ boson decays hadronically. The analysis is performed using an integrated luminosity of 20.3 fb$^{-1}$ of $pp$ collisions at $\\sqrt{s}$ = 8 TeV collected by the ATLAS detector at the LHC. No evidence for resonant diboson production is observed, and resonance masses below 700 GeV and 1490 GeV are excluded at 95% confidence level for the spin-2 Randall-Sundrum bulk graviton $G^*$ with coupling constant of 1.0 and the extended gauge model $W$ boson respectively.','cdsLink':'','journal':'EPJC','journalSub':'16-MAR-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,Strong gravity,BSM resonance,BSM search,WZ,WW,Boosted,MET,2 jets,1 jet,1 lepton','links':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-01/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1503.04677@linkEnd@1503.04677@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1352826@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-015-3425-6@linkEnd@DOI:10.1140/epjc/s10052-015-3425-6@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3425-6@linkEnd@Eur.%20Phys.%20J.%20C%20%2075%20(2015)%20209@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5962','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5962','shortTitle':'HSG6  Charged Higgs to WZ','fullTitle':'Search for a Charged Higgs Boson Produced in the Vector-boson Fusion Mode with Decay $H^\\pm \\to W^\\pm Z$ using $pp$ Collisions at $\\sqrt{s}=8$ TeV with the ATLAS Experiment','pubShortTitle':'Search BSM H+ -> WZ','refCode':'HIGG-2014-13','abstract':'A search for a charged Higgs boson, $H^\\pm$, decaying to a $W^\\pm$ boson and a $Z$ boson is presented. The search is based on 20.3 fb$^{-1}$ of proton-proton collision data at a center-of-mass energy of 8 TeV recorded with the ATLAS detector at the LHC. The $H^\\pm$ boson is assumed to be produced via vector-boson fusion and the decays $W^\\pm \\to q\\bar{q^\\prime}$ and $Z\\rightarrow e^+e^-/\\mu^+\\mu^-$ are considered. The search is performed in a range of charged Higgs boson masses from 200 to 1000 GeV. No evidence for the production of an $H^\\pm$ boson is observed. Upper limits of 31--1020 fb at 95\\% CL are placed on the cross section for vector-boson fusion production of an $H^\\pm$ boson times its branching fraction to $W^\\pm Z$. The limits are compared with predictions from the Georgi-Machacek Higgs Triplet Model.','cdsLink':'','journal':'PRL','journalSub':'13-MAR-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Charged Higgs searches,BSM Higgs searches,WZ','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-13@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1503.04233@linkEnd@1503.04233@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1352819@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://10.1103/PhysRevLett.114.231801@linkEnd@DOI@descriptionEnd@,@linkBegin@https://link.aps.org/abstract/PRL/v114/e231801@linkEnd@Phys.%20Rev.%20Lett.%20114%2C%20231801%20(2015)@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4502','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4502','shortTitle':'HSG6 Heavy Higgs to Zh','fullTitle':'Search for a CP-odd Higgs boson decaying to $Zh$ in $pp$ collisions at $\\sqrt{s } = 8$ TeV with the ATLAS detector','pubShortTitle':'Serach BSM A -> ZH(125)','refCode':'HIGG-2013-06','abstract':'A search for a heavy, CP-odd Higgs boson, $A$, decaying into a $Z$ boson and a 125 GeV Higgs boson, $h$, with the ATLAS detector at the LHC is presented. The search uses proton--proton collision data at a centre-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20.3 fb$^{-1}$. Decays of CP-even $h$ bosons to $\\tau\\tau$ or $bb$ pairs with the $Z$ boson decaying to electron or muon pairs are considered, as well as $h \\rightarrow bb$ decays with the $Z$ boson decaying to neutrinos. No evidence for the production of an $A$ boson in these channels is found and the 95% confidence level upper limits derived for $\\sigma (gg\\rightarrow A) \\times \\mbox{BR}(A\\rightarrow Zh) \\times \\mbox{BR}(h\\rightarrow f\\bar{f})$ are 0.098--0.013 pb for $f=\\tau$ and 0.57--0.014 pb for $f=b$ in a range of $m_A =$ 220--1000 GeV. The results are combined and interpreted in the context of two-Higgs-doublet models.','cdsLink':'','journal':'PLB','journalSub':'16-FEB-15','ecm':'7, 8','luminosity':'25 fb-1','keywords':'7 TeV,BSM Higgs searches,Z,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-06/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1502.04478@linkEnd@1502.04478@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1345028@linkEnd@Inspire@descriptionEnd@ ','run':'1; 1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2015.03.054@linkEnd@DOI:10.1016/j.physletb.2015.03.054@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269315002257@linkEnd@Physics%20Letters%20B%20744%20(2015)%20163-183@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5183','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5183','shortTitle':'HSG6 H JPsi gamma','fullTitle':'Search for Higgs and Z Boson Decays to J/psi gamma and Upsilon(nS) gamma with the ATLAS Detector','pubShortTitle':'Search H(125)/Z->J/psi gamma and Upsilon(nS) gamma','refCode':'HIGG-2014-03','abstract':'A search for the decays of the Higgs and $Z$ bosons to $J/\\psi\\gamma$ and $\\Upsilon(nS)\\gamma$ ($n=1,2,3$) is performed with $pp$ collision data samples corresponding to integrated luminosities of up to $20.3\\mathrm{fb}^{-1}$ collected at $\\sqrt{s}=8\\mathrm{TeV}$ with the ATLAS detector at the CERN Large Hadron Collider. No significant excess of events is observed above expected backgrounds and 95\\% CL upper limits are placed on the branching fractions. In the $J/\\psi\\gamma$ final state the limits are $1.5\\times10^{-3}$ and $2.6\\times10^{-6}$ for the Higgs and $Z$ bosons, respectively, while in the $\\Upsilon(1S,2S,3S)\\,\\gamma$ final states the limits are $(1.3,1.9,1.3)\\times10^{-3}$ and $(3.4,6.5,5.4)\\times10^{-6}$, respectively.','cdsLink':'','journal':'PRL','journalSub':'14-JAN-15','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Exotic Higgs decays,Higgs to meson+photon,Higgs to cc,Higgs to bb,Photons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-03/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1501.03276@linkEnd@1501.03276@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1339252@linkEnd@Inspire@descriptionEnd@ ','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.114.121801@linkEnd@DOI:10.1103/PhysRevLett.114.121801@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.114.121801@linkEnd@Phys.%20Rev.%20Lett.%20114%20(2015)%20121801@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4762','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4762','shortTitle':'HSG6 Charged to tau nu','fullTitle':'Search for charged Higgs bosons decaying via H+- -->
tau +- nu in fully hadronic final states using pp collision data at sqrt(s) = 8 TeV with the ATLAS detector','pubShortTitle':'Search BSM H+ -> tau nu','refCode':'HIGG-2013-30','abstract':'The results of a search for charged Higgs bosons decaying to a $\\tau$ lepton and a neutrino, $H^{\\pm} \\rightarrow \\tau^{\\pm} \\nu$, are presented. The analysis is based on 19.5 fb$^{-1}$ of proton--proton collision data at $\\sqrt{s}=8$ TeV collected by the ATLAS experiment at the Large Hadron Collider. Charged Higgs bosons are searched for in events consistent with top-quark pair production or in associated production with a top quark. The final state is characterised by the presence of a hadronic $\\tau$ decay, missing transverse momentum, $b$-tagged jets, a hadronically decaying $W$ boson, and the absence of any isolated electrons or muons with high transverse momenta. The data are consistent with the expected background from Standard Model processes. A statistical analysis leads to 95% confidence-level upper limits on the product of branching ratios ${\\cal B}(t\\rightarrow bH^\\pm) \\times {\\cal B}(H^\\pm\\rightarrow \\tau^{\\pm}\\nu)$, between 0.23% and 1.3% for charged Higgs boson masses in the range 80--160 GeV. It also leads to 95% confidence-level upper limits on the production cross section times branching ratio, $\\sigma(pp \\rightarrow tH^{\\pm} + X) \\times {\\cal B}(H^{\\pm} \\rightarrow \\tau^{\\pm} \\nu)$, between 0.76 pb and 4.5 fb, for charged Higgs boson masses ranging from 180 GeV to 1000 GeV. In the context of different scenarios of the Minimal Supersymmetric Standard Model, these results exclude nearly all values of $\\tan\\beta$ above one for charged Higgs boson masses between 80 GeV and 160 GeV, and exclude a region of parameter space with high $\\tan\\beta$ for $H^{\\pm}$ masses between 200 GeV and 250 GeV.','cdsLink':'','journal':'JHEP','journalSub':'20-DEC-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Charged Higgs searches,BSM Higgs searches,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-30/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1412.6663@linkEnd@1412.6663@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1335266@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP03%282015%29088@linkEnd@DOI:10.1007/JHEP03(2015)088@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP03%282015%29088@linkEnd@JHEP03%20(2015)%20088@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3922','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3922','shortTitle':'DBL - VV lljj llJ resonance at 8 TeV','fullTitle':'Search for resonant diboson production in the llqq final state in pp collisions at sqrt(s) = 8!TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV to llqq final state','refCode':'EXOT-2013-06','abstract':'This paper reports on a search for narrow resonances in diboson production in the $\\ell\\ell q\\bar{q}$ final state using pp collision data corresponding to an integrated luminosity of $20 fb^{-1}$ collected at $\\sqrt{s}=8$ TeV with the ATLAS detector at the Large Hadron Collider. No significant excess of data events over the Standard Model expectation is observed. Upper limits at the 95% confidence level are set on the production cross section times branching ratio for Kaluza--Klein gravitons predicted by the Randall--Sundrum model and for Extended Gauge Model W bosons. These results lead to the exclusion of mass values below 740 GeV and 1590 GeV for the graviton and W boson respectively.','cdsLink':'','journal':'EPJC','journalSub':'22-SEP-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,Strong gravity,BSM resonance,BSM search,ZZ,WZ,Boosted,2 jets,1 jet,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-06@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1409.6190@linkEnd@1409.6190@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1318483@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-015-3261-8@linkEnd@DOI:10.1140/epjc/s10052-015-3261-8%20@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-015-3261-8@linkEnd@Eur.%20Phys.%20J.%20C%20(2015)%2075:69%20@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4763','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4763','shortTitle':'HSG6 MSSM to tautau','fullTitle':'Search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector','pubShortTitle':'Search BSM H/A -> tau tau','refCode':'HIGG-2013-31','abstract':'A search for the neutral Higgs bosons predicted by the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is performed on data from proton--proton collisions at a centre-of-mass energy of $8 TeV$ collected with the ATLAS detector at the Large Hadron Collider. The samples used for this search were collected in 2012 and correspond to integrated luminosities in the range 19.5 - 20.3 fb$^{-1}$. The MSSM Higgs bosons are searched for in the $\\tau\\tau$ final state. No significant excess over the expected background is observed, and exclusion limits are derived for the production cross section times branching fraction of a scalar particle as a function of its mass. The results are also interpreted in the MSSM parameter space for various benchmark scenarios.','cdsLink':'','journal':'JHEP','journalSub':'21-SEP-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM Higgs searches,BSM search,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-31@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1409.6064@linkEnd@1409.6064@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1318481@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP11%282014%29056@linkEnd@DOI:10.1007/JHEP11(2014)056@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP11%282014%29056@linkEnd@JHEP11(2014)056@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3925','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3925','shortTitle':'DBL - Diboson Vgamma resonance 8 TeV','fullTitle':'Search for new resonances in the Wgamma and Zgamma final states in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector','pubShortTitle':'Search for a resonance decaying to W/Z plus a photon','refCode':'EXOT-2013-09','abstract':'This letter presents a search for new resonances decaying to final states with a vector boson produced in association with a high transverse momentum photon, $V\\gamma$, with $V= W(\\rightarrow \\ell \\nu)$ or $Z(\\rightarrow \\ell^{+} \\ell^{-})$, where $\\ell = e$ or $\\mu$. The measurements use $20.3$~fb$^{-1}$ of proton--proton collision data at a center--of--mass energy of $\\sqrt{s}=8\\,\\mathrm{TeV}$ recorded with the ATLAS detector. No deviations from the Standard Model expectations are found, and production cross section limits are set at 95\\% confidence level. Masses of the hypothetical $a_{\\mathrm{T}}$ and $\\omega_{\\mathrm{T}}$ states of a benchmark Low Scale Technicolor model are excluded in the ranges $[275,960]\\,\\mathrm{GeV}$ and $[200,700]\\cup[750,890]\\,\\mathrm{GeV}$, respectively. Limits at 95% confidence level on the production cross section of a singlet scalar resonance decaying to $Z\\gamma$ final states have also been obtained for masses below $1180\\,\\mathrm{GeV}$.','cdsLink':'','journal':'PLB','journalSub':'30-JUL-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM resonance,BSM search,Vphoton,Photon,Z,W,MET,Photons,2 leptons,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-09@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1407.8150@linkEnd@1407.8150@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1308923@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2014.10.002@linkEnd@DOI:10.1016/j.physletb.2014.10.002@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269314007254@linkEnd@PLB%20738%20(2014)%20428-447@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'5282','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=5282','shortTitle':'HSG1 low and high mass search','fullTitle':'Search for Scalar Diphoton Resonances in the Mass Range 65-600 Gev with the ATLAS Detector in pp Collision Data at sqrt(s) = 8 TeV','pubShortTitle':'Search BSM H-> gamma gamma','refCode':'HIGG-2014-04','abstract':'A search for scalar particles decaying via narrow resonances into two photons in the mass range $65-600$ GeV is performed using 20.3 fb$^{-1}$ of $\\sqrt{s}$ = 8 TeV $pp$ collision data collected with the ATLAS detector at the Large Hadron Collider. The recently discovered Higgs boson is treated as a background. No significant evidence for an additional signal is observed. The results are presented as limits at the 95 % confidence level on the production cross-section of a scalar boson times branching ratio into two photons, in a fiducial volume where the reconstruction efficiency is approximately independent of the event topology. The upper limits set extend over a considerably wider mass range than previous searches.','cdsLink':'','journal':'PRL','journalSub':'24-JUL-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM Higgs searches,Higgs to 2 photons,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1407.6583@linkEnd@1407.6583@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1307756@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.113.171801@linkEnd@DOI:10.1103/PhysRevLett.113.171801@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.171801@linkEnd@Phys.%20Rev.%20Lett.%20113%2C%20171801@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4723','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4723','shortTitle':'HSG1 HSG6 HH to bbgg','fullTitle':'Search for double Higgs production in the H->gamgam and H->bb decay channels','pubShortTitle':'Search BSM H->H(125)H(125)->bb gamma gamma and H(125)H(125)->bb gamma gamma','refCode':'HIGG-2013-29','abstract':'Searches are performed for resonant and non-resonant Higgs boson pair production in the $hh \\rightarrow \\gamma\\gamma b \\overline b$ final state using 20 fb$^{-1}$ of proton--proton collisions at a center-of-mass energy of 8TeV recorded with the ATLAS detector at the CERN Large Hadron Collider. A 95% confidence level upper limit on the cross section times branching ratio of non--resonant production is set at 2.2 pb, while the expected limit is 1.0 pb. The corresponding limit observed for a narrow resonance ranges between 0.8 and 3.5 pb as a function of its mass.','cdsLink':'','journal':'PRL','journalSub':'19-JUN-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,BSM Higgs searches,Di-Higgs production,Higgs to bb,Higgs to 2 photons,BSM search,Di-Higgs,Di-photon,b-jets,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-29@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1406.5053@linkEnd@1406.5053@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1301558@linkEnd@Inspire@descriptionEnd@
@linkBegin@http://hepdata.cedar.ac.uk/view/ins1301558@linkEnd@HepData@descriptionEnd@','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.114.081802@linkEnd@DOI@descriptionEnd@,@linkBegin@https://link.aps.org/abstract/PRL/v114/e081802@linkEnd@Phys.%20Rev.%20Lett.%20114%2C%20081802%20(2015)@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3923','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3923','shortTitle':'DBL - Diboson lvll resonance 8 TeV','fullTitle':'Search for WZ resonances in the fully leptonic channel using pp collisions at sqrt{s } = 8 TeV with the ATLAS detector','pubShortTitle':'Resonance search in the VV to lvll final state','refCode':'EXOT-2013-07','abstract':'A search for resonant $WZ$ production in the $\\ell\\nu\\ell\\ell$ ($\\ell, \\ell = e,\\mu$) decay channel using 20.3 fb$^{-1}$ of $\\sqrt{s}$ = 8 TeV $pp$ collision data collected by the ATLAS experiment at LHC is presented. No significant deviation from the Standard Model prediction is observed and upper limits on the production cross sections of $WZ$ resonances from an extended gauge model $W^{\\prime}$ and from a simplified model of heavy vector triplets are derived. A corresponding observed (expected) lower mass limit of 1.52 (1.49) TeV is derived for the $W^{\\prime}$ at the 95% confidence level.','cdsLink':'','journal':'PLB','journalSub':'17-JUN-14','ecm':'8','luminosity':'20 fb-1','keywords':'8 TeV,Heavy vector triplets,BSM resonance,BSM search,WZ,MET,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2013-07@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1406.4456@linkEnd@1406.4456@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1300821@linkEnd@Inspire@descriptionEnd@
@linkBegin@http://hepdata.cedar.ac.uk/view/ins1300821@linkEnd@HepData@descriptionEnd@','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2014.08.039@linkEnd@DOI:10.1016/j.physletb.2014.08.039@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269314006066@linkEnd@Phys.%20Lett.%20B%20737%20%20(2014)%20223@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4583','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4583','shortTitle':'HSG1 FCNC top to Hc to diphoton charm','fullTitle':'Search for top quark decays t\\rightarrow qH with H\\to\\gamma\\gamma using the ATLAS detector','pubShortTitle':'Search FCNC t->H(125) q, H(125)->gammagamma','refCode':'HIGG-2013-09','abstract':'A search is performed for flavour-changing neutral currents in the decay of a top quark to an up-type ($c, u$) quark and a Higgs boson, where the Higgs boson decays to two photons. The proton-proton collision data set used corresponds to 4.7 fb$^{-1}$ at $\\sqrt{s}$ = 7 TeV and 20.3 fb$^{-1}$ at $\\sqrt{s}$ = 8 TeV collected by the ATLAS experiment at the LHC. Top quark pair events are searched for in which one top quark decays to $qH$ and the other decays to $bW$. Both the hadronic and the leptonic decay modes of the $W$ boson are used. No significant signal is observed and an upper limit is set on the $t\\rightarrow qH$ branching ratio of 0.79% at the 95% confidence level. The corresponding limit on the $tqH$ coupling combination $\\sqrt{\\lambda_{tcH}^{2} + \\lambda_{tuH}^{2}}$ is 0.17.','cdsLink':'','journal':'JHEP','journalSub':'26-MAR-14','ecm':'7, 8','luminosity':'25 fb-1','keywords':'7 TeV,BSM Higgs searches,Higgs to 2 photons,FCNC,Di-photon,b-jets,Photons,8 TeV','links':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-09@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1403.6293@linkEnd@1403.6293@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1287055@linkEnd@Inspire@descriptionEnd@
','run':'1; 1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP06%282014%29008@linkEnd@DOI:10.1007/JHEP06(2014)008@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP06%282014%29008@linkEnd@JHEP06(2014)008@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'3982','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=3982','shortTitle':'HSG2 ZH H Invisible for Winter 2013','fullTitle':'Search for Invisible Decays of a Higgs Boson Produced \\\\ in Association with a $\\boldsymbol{Z}$ Boson in ATLAS','pubShortTitle':'Serach BSM Z H/H(125) -> invisible','refCode':'HIGG-2013-03','abstract':'A search for evidence of invisible-particle decay modes of a Higgs boson produced in association with a Z boson at the Large Hadron Collider is presented. No deviation from the Standard Model expectation is observed in 4.5 fb$^{−1}$ (20.3 fb$^{−1}$) of 7 (8) TeV pp collision data collected by the ATLAS experiment. Assuming the Standard Model rate for ZH production, an upper limit of 75%, at the 95% confidence level is set on the branching ratio to invisible-particle decay modes of the Higgs boson at a mass of 125.5 GeV. The limit on the branching ratio is also interpreted in terms of an upper limit on the allowed dark matter–nucleon scattering cross section within a Higgs-portal dark matter scenario. Limits are also set on an additional neutral Higgs boson, in the mass range 110 < $m_H$ < 400 GeV, produced in association with a Z boson and decaying to invisible particles.','cdsLink':'','journal':'PRL','journalSub':'13-FEB-14','ecm':'7, 8','luminosity':'24 fb-1','keywords':'7 TeV,Exotic Higgs decays,BSM Higgs searches,Higgs to invisible,Dark matter,Z,MET,2 leptons,8 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-03@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1402.3244@linkEnd@1402.3244@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1281236@linkEnd@Inspire@descriptionEnd@
','run':'1; 1','finalPubRef':'@linkBegin@https://doi.org/10.1103/PhysRevLett.112.201802@linkEnd@DOI:10.1103/PhysRevLett.112.201802@descriptionEnd@,@linkBegin@https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.112.201802@linkEnd@Phys.%20Rev.%20Lett.%20112%20%20(2014)%20201802@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'4004','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=4004','shortTitle':'HSG6 2HDM Higgs cascade','fullTitle':'Search for a Multi-Higgs Boson Cascade in W+W- bbar events with the ATLAS detector in pp collisions at sqrt(s) = 8 TeV','pubShortTitle':'Search BSM H0 -> W H+ -> WH(125)','refCode':'HIGG-2013-04','abstract':'A search is presented for new particles in an extension to the Standard Model that includes a heavy Higgs boson ($H^0$), an intermediate charged Higgs boson (H±), and a light Higgs boson ($h^0$). The analysis searches for events involving the production of a single heavy neutral Higgs boson which decays to the charged Higgs boson and a W boson, where the charged Higgs boson subsequently decays into a W boson and the lightest neutral Higgs boson decaying to a bottom-antibottom-quark pair. Such a cascade results in a W-boson pair and a bottom–antibottom-quark pair in the final state. Events with exactly one lepton, missing transverse momentum, and at least four jets are selected from a data sample corresponding to an integrated luminosity of 20.3 fb$^{-1}$, collected by the ATLAS detector in proton-proton collisions at √s = 8 TeV at the LHC. The data are found to be consistent with Standard Model predictions, and 95% confidence level upper limits are set on the product of cross-section and branching ratio. These limits range from 0.065 pb to 43 pb as a function of $H^0$ and H± masses, with $m_{h0}$ fixed at 125 GeV.','cdsLink':'','journal':'PRD','journalSub':'06-DEC-13','ecm':'8','luminosity':'20.7 fb-1','keywords':'8 TeV,BSM Higgs searches,W','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2013-04@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1312.1956@linkEnd@1312.1956@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1268153@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.89.032002@linkEnd@DOI:10.1103/PhysRevD.89.032002@descriptionEnd@,@linkBegin@https://prd.aps.org/abstract/PRD/v89/i3/e032002@linkEnd@Phys.%20Rev.%20D%2089%2C%20032002%20(2014)@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'2121','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=2121','shortTitle':'DBL - Diboson lvjj resonance search','fullTitle':'Search for heavy resonance decaying to WW or WZ in the lvjj and lvJ (boosted) final states.','pubShortTitle':'Diboson resonance search in lnuqq','refCode':'EXOT-2012-08','abstract':'A search for resonant diboson production using a data sample corresponding to 4.7 fb$^{-1}$ of integrated luminosity collected by the ATLAS experiment at the Large Hadron Collider in pp collisions at $\\sqrt{s}$ = 7 TeV is presented. The search for a narrow resonance in the WW or WZ mass distribution is conducted in a final state with an electron or a muon, missing transverse energy and at least two jets. No significant excess is observed and limits are set using three benchmark models: WW resonance masses below 940 and 710 GeV are excluded at 95% confidence level for spin-2 Randall-Sundrum and Bulk Randall-Sundrum gravitons, respectively; WZ resonance masses below 950 GeV are excluded at 95% confidence level for a spin-1 Extended Gauge Model W boson.','cdsLink':'','journal':'PRD','journalSub':'01-MAY-13','ecm':'7','luminosity':'5 fb-1','keywords':'7 TeV,Heavy vector triplets,Strong gravity,BSM search,WZ,WW,MET,2 jets,1 lepton','links':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-08/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1305.0125@linkEnd@1305.0125@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1231616@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://link.aps.org/doi/10.1103/PhysRevD.87.112006@linkEnd@DOI:10.1103/PhysRevD.87.112006@descriptionEnd@,@linkBegin@https://prd.aps.org/abstract/PRD/v87/i11/e112006@linkEnd@Phys.%20Rev.%20D%2087%2C%20112006%20(2013)@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'2004','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=2004','shortTitle':'LPX diphoton resonance search','fullTitle':'Search for extra dimensions in diphoton events using proton-proton collisions recorded at sqrt(s) = 7 TeV with the ATLAS detector at the LHC','pubShortTitle':'Search for diphoton resonances','refCode':'EXOT-2012-06','abstract':'The large difference between the Planck scale and the electroweak scale, known as the hierarchy problem, is addressed in certain models through the postulate of extra spatial dimensions. A search for evidence of extra spatial dimensions in the diphoton channel has been performed using the full set of proton-proton collisions at $\\sqrt{s}$ = 7 TeV recorded in 2011 with the ATLAS detector at the CERN Large Hadron Collider. This dataset corresponds to an integrated luminosity of 4.9 /fb. The diphoton invariant mass spectrum is observed to be in good agreement with the expected Standard Model background. 95% confidence level lower limits of between 2.52 TeV and 3.92 TeV are set on the Ms scale in the context of the model proposed by Arkani-Hamed, Dimopoulos and Dvali, depending on the number of extra dimensions and the theoretical formalism used. In the context of the Randall--Sundrum model, a lower limit of 1.00 (2.06) TeV at 95% confidence level is set on the mass of the lightest graviton for couplings of k/Mpl = 0.01 (0.1). Combining with the ATLAS dilepton searches based on the 2011 data, the 95% confidence level limit on the Randall--Sundrum graviton mass is further tightened to 1.03 (2.23) TeV for k/Mpl = 0.01 (0.1).','cdsLink':'','journal':'NJP','journalSub':'21-FEB-13','ecm':'7','luminosity':'4.9 fb-1','keywords':'7 TeV,Strong gravity,BSM resonance,BSM search,Di-photon,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-06/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1210.8389@linkEnd@1210.8389@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1197323@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1088/1367-2630/15/4/043007@linkEnd@DOI:10.1088/1367-2630/15/4/043007@descriptionEnd@,@linkBegin@https://stacks.iop.org/1367-2630/15/043007@linkEnd@New%20J.%20Phys.%2015%20(2013)%20043007@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'1762','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=1762','shortTitle':'Charged Higgs to csbar Moriond 2012','fullTitle':'Search for a light charged Higgs boson in the decay channel H+ -> csbar in ttbar events using pp collisions at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Search BSM H+ -> c sbar','refCode':'HIGG-2012-10','abstract':'A search for a charged Higgs boson ($H^+$) in $t\\bar{t}$ decays is presented, where one of the top quarks decays via $t \\to H^+b$, followed by $H^+ \\to$ two jets ($c\\bar{s}$). The other top quark decays to Wb, where the W boson then decays into a lepton ($e/\\mu$) and a neutrino. The data were recorded in pp collisions at $\\sqrt{s}$ = 7 TeV by the ATLAS detector at the LHC in 2011, and correspond to an integrated luminosity of 4.7 fb-1. With no observation of a signal, 95% confidence level (CL) upper limits are set on the decay branching ratio of top quarks to charged Higgs bosons varying between 5% and 1% for $H^+$ masses between 90 GeV and 150 GeV, assuming $B(H^+ \\to c\\bar{s})$=100%.','cdsLink':'','journal':'EPJC','journalSub':'15-FEB-13','ecm':'7','luminosity':'4.7 fb-1','keywords':'7 TeV,Charged Higgs searches,BSM Higgs searches,c-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2012-10/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1302.3694@linkEnd@1302.3694@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1219797@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-013-2465-z@linkEnd@DOI:10.1140/epjc/s10052-013-2465-z@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1140/epjc/s10052-013-2465-z@linkEnd@Eur.%20Phys.%20J.%20C%2C%2073%206%20(2013)%202465@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'2608','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=2608','shortTitle':'Search for charged Higgs via lfv','fullTitle':'Search for charged Higgs bosons through the violation of lepton universality in ttbar events using pp collision data at sqrt(s) = 7 TeV with the ATLAS experiment','pubShortTitle':'Search BSM FCNC t->H+b','refCode':'HIGG-2012-22','abstract':'In several extensions of the Standard Model, the top quark can decay into a bottom quark and a light charged Higgs boson $H^+, t \\to bH^+$, in addition to the Standard Model decay $t \\to bW$. Since W bosons decay to the three lepton generations equally, while $H^+$ may predominantly decay into $\\tau\\nu$, charged Higgs bosons can be searched for using the violation of lepton universality in top quark decays. The analysis in this paper is based on 4.6/fb of proton-proton collision data at $\\sqrt{s}$ = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider. Signatures containing leptons (e or $\\mu$) and/or a hadronically decaying $\\tau (\\tau_{had})$ are used. Event yield ratios between $e+\\tau_{had}$ and $e+\\mu$, as well as between $\\mu+\\tau_{had}$ and $\\mu+e$, final states are measured in the data and compared to predictions from simulations. This ratio-based method reduces the impact of systematic uncertainties in the analysis. No significant deviation from the Standard Model predictions is observed. With the assumption that the branching fraction $B(H^+ \\to \\tau\\nu)$ is 100%, upper limits in the range 3.2%-4.4% can be placed on the branching fraction $B(t \\to bH^+)$ for charged Higgs boson masses $m_{H+}$ in the range 90-140 GeV. After combination with results from a search for charged Higgs bosons in ttbar decays using the $\\tau_{had}$+jets final state, upper limits on $B(t \\to bH^+)$ can be set in the range 0.8%-3.4%, for $m_{H+}$ in the range 90-160 GeV.','cdsLink':'','journal':'JHEP','journalSub':'14-DEC-12','ecm':'7','luminosity':'4.6 fb-1','keywords':'7 TeV,Charged Higgs searches,BSM Higgs searches,Top pair,b-jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2012-22/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1212.3572@linkEnd@1212.3572@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1207451%3Fln%3Den@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP03%282013%29076@linkEnd@DOI:10.1007/JHEP03(2013)076@descriptionEnd@,@linkBegin@https://link.springer.com/article/10.1007/JHEP03%282013%29076@linkEnd@JHEP03(2013)076@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'1923','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=1923','shortTitle':'LPX - Search for Z to tau tau','fullTitle':'A search for high-mass resonances decaying to tau+tau- in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Search for di-tau resonances','refCode':'EXOT-2012-03','abstract':'This Letter presents a search for high-mass resonances decaying into $\\tau^+ \\tau^-$ final states using proton-proton collisions at $\\sqrt{s}$ = 7 TeV produced by the Large Hadron Collider. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 4.6 inverse femtobarns. No statistically significant excess above the Standard Model expectation is observed; 95% credibility upper limits are set on the cross section times branching fraction of Z resonances decaying into $\\tau^+ \\tau^-$ pairs as a function of the resonance mass. As a result, Z bosons of the Sequential Standard Model with masses less than 1.40 TeV are excluded at 95% credibility.','cdsLink':'','journal':'PLB','journalSub':'24-OCT-12','ecm':'7','luminosity':'4.6 fb-1','keywords':'7 TeV,BSM resonance,BSM search,Taus,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-03/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1210.6604@linkEnd@1210.6604@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1193050@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2013.01.040@linkEnd@DOI:10.1016/j.physletb.2013.01.040@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269313000816@linkEnd@Phys.%20Lett.%20B%20719%20(2013)%20242-260@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'2982','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=2982','shortTitle':'DBL -Doubly charged Higgs like sign L','fullTitle':'Search for doubly-charged Higgs bosons in like-sign dilepton final states at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Doubly charged Higgs search in same-sign dilepton','refCode':'EXOT-2012-18','abstract':'A search for doubly-charged Higgs bosons decaying to pairs of electrons and/or muons is presented. The search is performed using a data sample corresponding to an integrated luminosity of 4.7 fb-1 of pp collisions at $\\sqrt{s}$ = 7 TeV collected by the ATLAS detector at the LHC. Pairs of prompt, isolated, high-pT leptons with the same electric charge (ee, emu, mumu) are selected, and their invariant mass distribution is searched for a narrow resonance. No significant excess over Standard Model background expectations is observed, and limits are placed on the cross section times branching ratio for pair production of doubly-charged Higgs bosons. The masses of doubly-charged Higgs bosons are constrained depending on the branching ratio into these leptonic final states. Assuming pair production, coupling to left-handed fermions, and a branching ratio of 100% for each final state, masses below 409 GeV, 375 GeV, and 398 GeV are excluded for ee, emu, mumu, respectively.','cdsLink':'','journal':'EPJC','journalSub':'18-OCT-12','ecm':'7','luminosity':'4.7 fb-1','keywords':'7 TeV,Charged Higgs searches,BSM search,2 leptons (same charge)','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-18@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1210.5070@linkEnd@1210.5070@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1191430@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://link.aps.org/doi/10.1103/PhysRevD.86.091103@linkEnd@DOI:10.1103/PhysRevD.86.091103@descriptionEnd@,@linkBegin@https://prd.aps.org/abstract/PRD/v86/i9/e091103@linkEnd@Phys.%20Rev.%20D86%20(2012)%20091103@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'2423','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=2423','shortTitle':'DBL - Diboson lvlv resonance search','fullTitle':'Search for new phenomena in the WW to l nu l nu final state in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Diboson resonance search in lnulnu','refCode':'EXOT-2012-11','abstract':'This Letter reports a search for a heavy particle that decays to WW using events produced in pp collisions at $\\sqrt{s}$ = 7 TeV. The data were recorded in 2011 by the ATLAS detector and correspond to an integrated luminosity of 4.7 fb$^{-1}$. $WW \\to l\\nu l\\nu(l, l = e$ or $\\mu)$ final states are considered and the distribution of the transverse mass of the WW candidates is found to be consistent with Standard Model expectations. Upper limits on the production cross section times branching ratio into W boson pairs are set for Randall-Sundrum and bulk Randall-Sundrum gravitons, which result in observed 95% CL lower limits on the masses of the two particles of 1.23 TeV and 0.84 TeV, respectively.','cdsLink':'','journal':'PLB','journalSub':'14-AUG-12','ecm':'7','luminosity':'5 fb-1','keywords':'7 TeV,Strong gravity,BSM resonance,BSM search,WW,MET,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2012-11@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1208.2880@linkEnd@1208.2880@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1127504@linkEnd@Inspire@descriptionEnd@
@linkBegin@http://hepdata.cedar.ac.uk/View/9718621@linkEnd@HepData@descriptionEnd@','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2012.11.040@linkEnd@DOI:10.1016/j.physletb.2012.11.040@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269312012051@linkEnd@Phys.%20Lett.%20B%20718%20(2013)%20860-878@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'1481','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=1481','shortTitle':'Search for W production in single top','fullTitle':'Search for tb resonances in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Search for tb resonances at 7 TeV','refCode':'TOPQ-2011-20','abstract':'This Letter presents a search for tb resonances in 1.04/fb$^{-1}$ of LHC proton-proton collision data collected by the ATLAS detector at a center-of-mass energy of 7 TeV. Events with a lepton, missing transverse momentum, and two jets are selected and the invariant mass of the corresponding final state is reconstructed. The search exploits the shape of the tb invariant mass distribution compared to the expected Standard Model backgrounds. The model of a right-handed W$_R$ with Standard Model-like couplings is chosen as the benchmark model for this search. No statistically significant excess of events is observed in data, and upper limits on the cross section times the branching ratio of W$_R$ resonances at 95% CL lie in the range 6.1-1.0 pb for W$_R$ masses ranging from 0.5 to 2.0 TeV. These limits are translated into a lower bound on the allowed right-handed W$_R$ mass, giving $m_{W_R}$ > 1.13 TeV at 95% CL.','cdsLink':'','journal':'PRL','journalSub':'04-MAY-12','ecm':'7','luminosity':'1.04 fb-1','keywords':'1 lepton,BSM resonance,Single top measurements','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2011-20@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1205.1016@linkEnd@1205.1016@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1113597@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1140/epjc/s10052-012-2157-0@linkEnd@DOI:10.1140/epjc/s10052-012-2157-0@descriptionEnd@,@linkBegin@https://www.springerlink.com/content/26106q400g15263k/@linkEnd@Eur.%20Phys.%20J.%20C%20(2012)%2072:2157@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'1761','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=1761','shortTitle':'Charged Higgs to taunu Moriond 2012','fullTitle':'Search for charged Higgs bosons decaying via H+ -> tau+nu in ttbar events using 4.6 fb-1 of pp collision data at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Search BSM H+ -> tau nu','refCode':'HIGG-2012-09','abstract':'The results of a search for charged Higgs bosons are presented. The analysis is based on 4.6/fb of proton-proton collision data at $\\sqrt{s}$ = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider, using top quark pair events with a tau lepton in the final state. The data are consistent with the expected background from Standard Model processes. Assuming that the branching ratio of the charged Higgs boson to a tau lepton and a neutrino is 100%, this leads to upper limits on the branching ratio of top quark decays to a b quark and a charged Higgs boson between 5% and 1% for charged Higgs boson masses ranging from 90 GeV to 160 GeV, respectively. In the context of the mh-max scenario of the MSSM, tan(beta) above 12-26, as well as between 1 and 2-6, can be excluded for charged Higgs boson masses between 90 GeV and 150 GeV.','cdsLink':'','journal':'JHEP','journalSub':'12-APR-12','ecm':'7','luminosity':'4.6 fb-1','keywords':'7 TeV,Charged Higgs searches,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2012-09@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1204.2760@linkEnd@1204.2760@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1110689@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1007/JHEP06%282012%29039@linkEnd@DOI:10.1007/JHEP06(2012)039@descriptionEnd@,@linkBegin@https://www.springerlink.com/content/4876m2k082hm4l06/@linkEnd@JHEP%201206%20(2012)%20039@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'1161','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=1161','shortTitle':'DBL - WZ to lvll resonance search','fullTitle':'Search for resonant WZ production in the WZ to lnull channel in sqrt(s) = 7 TeV pp collisions with the ATLAS detector','pubShortTitle':'WZ resonance search in lnull','refCode':'EXOT-2011-24','abstract':'A generic search is presented for a heavy particle decaying to $WZ \\to l\\nu ll (l, l = e, \\mu)$ final states. The data were recorded by the ATLAS detector in $\\sqrt{s}$ = 7 TeV pp collisions at the Large Hadron Collider and correspond to an integrated luminosity of 1.02 fb-1. The transverse mass distribution of the selected WZ candidates is found to be consistent with the Standard Model expectation. Upper limits on the production cross section times branching ratio are derived using two benchmark models predicting a heavy particle decaying to a WZ pair.','cdsLink':'','journal':'PRD','journalSub':'07-APR-12','ecm':'7','luminosity':'1.02 fb-1','keywords':'7 TeV,Other new particle searches,Heavy vector triplets,BSM resonance,BSM search,WZ,MET,>=3 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2011-24@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1204.1648@linkEnd@1204.1648@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1107731@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevD.85.112012@linkEnd@DOI:10.1103/PhysRevD.85.112012@descriptionEnd@,@linkBegin@https://prd.aps.org/abstract/PRD/v85/i11/e112012@linkEnd@Phys.Rev.%20D85%20(2012)%20112012@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'623','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=623','shortTitle':'DBL - resonances in ZZ to 4l and 2l2j','fullTitle':'Search for new particles decaying to ZZ using final states with leptons and jets with the ATLAS detector in sqrt(s) = 7 TeV proton-proton collisions','pubShortTitle':'ZZ resonance search in 4l and lljj','refCode':'EXOT-2011-16','abstract':'A search is presented for a narrow resonance decaying to a pair of Z bosons using data corresponding to 1.02/fb$^{-1}$ of integrated luminosity collected by the ATLAS experiment from pp collisions at $\\sqrt{s}$ = 7 TeV. Events containing either four charged leptons ($llll$) or two charged leptons and two jets ($lljj$) are analyzed and found to be consistent with the Standard Model background expectation. Lower limits on a resonance mass are set using the Randall-Sundrum (RS1) graviton model as a benchmark. Using both $llll$ and $lljj$ events, an RS1 graviton with $k/\\overline{m}_{pl}$ = 0.1 and mass between 325 and 845 GeV is excluded at 95% confidence level. In addition, the $llll$ events are used to set a fiducial cross section limit of $\\sigma_{fiducial}$(pp -> X -> ZZ < 0.92 pb at 95% confidence level for any new sources of ZZ production with $m_{ZZ}$ greater than 300 GeV.','cdsLink':'','journal':'PLB','journalSub':'04-MAR-12','ecm':'7','luminosity':'1 fb-1','keywords':'7 TeV,Strong gravity,BSM resonance,BSM search,ZZ,2 jets,>=3 leptons,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2011-16/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1203.0718@linkEnd@1203.0718@descriptionEnd@,@linkBegin@https://inspirehep.net/record/1092728@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1016/j.physletb.2012.03.022@linkEnd@DOI:10.1016/j.physletb.2012.03.022@descriptionEnd@,@linkBegin@https://www.sciencedirect.com/science/article/pii/S0370269312002869@linkEnd@Phys.Lett.%20B710%20(2012)%20538-556@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'584','internalLink':'https://glance.cern.ch/atlas/analysis/papers/details.php?id=584','shortTitle':'Dilepton (Z and RS graviton) - 2011data','fullTitle':'Search for dilepton resonances in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector','pubShortTitle':'Dilepton resonance search','refCode':'EXOT-2011-06','abstract':'This Letter reports on a search for narrow high-mass resonances decaying into dilepton final states. The data were recorded by the ATLAS experiment in pp collisions at $\\sqrt{s}$ = 7 TeV at the LHC and correspond to a total integrated luminosity of 1.08/fb (1.21/fb) in the ee (mumu) channel. No statistically significant excess above the Standard Model expectation is observed and upper limits are set at the 95% C.L. on the cross section times branching ratio of Z resonances and Randall-Sundrum gravitons decaying into dileptons as a function of the resonance mass. A lower mass limit of 1.83 TeV on the Sequential Standard Model Z boson is set. A Randall-Sundrum graviton with coupling $k/\\overline{M}_{Pl}$=0.1 is excluded at 95% C.L. for masses below 1.63 TeV.','cdsLink':'','journal':'PRL','journalSub':'08-AUG-11','ecm':'7','luminosity':'1 fb-1','keywords':'7 TeV,Strong gravity,BSM resonance,BSM search,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/EXOT-2011-06/@linkEnd@Documents@descriptionEnd@,@linkBegin@https://arxiv.org/abs/1108.1582@linkEnd@1108.1582@descriptionEnd@,@linkBegin@https://inspirehep.net/record/922410@linkEnd@Inspire@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://dx.doi.org/10.1103/PhysRevLett.106.121803@linkEnd@DOI:10.1103/PhysRevLett.106.121803@descriptionEnd@,@linkBegin@https://prl.aps.org/abstract/PRL/v106/i12/e121803@linkEnd@Phys.Rev.Lett.%20106%20(2011)%20121803@descriptionEnd@','publicationType':'PAPER','pressStatement':''},{'publicationId':'11909','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=11909','shortTitle':'HZZ H->emu LFV + H->ee 2015-2018','fullTitle':'Search for the decays of the Higgs boson $H\\to ee$ and $H\\to e\\mu$ in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector','pubShortTitle':'Search BSM H(125)->emu lepton flavor violating decay and H(125)->ee','refCode':'ATLAS-CONF-2019-037','abstract':'Searches for the decay of the Higgs boson $H \\to ee$ and $H \\to e \\mu$ are performed using data corresponding to an integrated luminosity of 139 bf$^{-1}$ collected with the ATLAS detector in $pp$ collisions at $\\sqrt{s}=$13 TeV at the LHC. No significant signals are observed, in agreement with the Standard Model expectation. For a Higgs boson mass of 125 GeV the observed (expected) upper limit at the 95% confidence level on the branching fraction of $H \\to ee$ is $3.6 \\times 10^{-4}$ ($3.5 \\times 10^{-4}$) and on $H \\to e\\mu$ is $6.1\\times 10^{-5}$ ($5.8\\times 10^{-5}$). These results represent an improvement of a factor of about 5 and 6 on the previous best limits on the branching fractions of $H \\to ee$ and $H \\to e \\mu$, respectively.','cdsLink':'https://cds.cern.ch/record/2685338','journal':'Preliminary','journalSub':'05-AUG-19','ecm':'13','luminosity':'139 fb-1','keywords':'2 leptons,13 TeV,Exotic Higgs decays,LFV,BSM search','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-037@linkEnd@Documents@descriptionEnd@
@linkBegin@https://atlas.cern/updates/physics-briefing/higgs-interaction-lightest-charged-lepton@linkEnd@Briefing@descriptionEnd@','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-037@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'11907','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=11907','shortTitle':'HBSM dimuon mass +b jets 8 TeV +13 TeV','fullTitle':'Search for a new resonance in the $bj\\mu\\mu$ final state at a dimuon invariant mass around 28 Gev with ATLAS $pp$ data collected at $\\sqrt{s } =$ 8 and 13 TeV','pubShortTitle':'Dimuon search + b-jet at 8 and 13 TeV','refCode':'ATLAS-CONF-2019-036','abstract':'A search for a resonance decaying to two muons in the dimuon invariant mass range between 26-30 GeV and produced in association with a $b$-jet and an additional jet, is presented. The analysis uses proton-proton collision datasets recorded by the ATLAS detector at the centre-of-mass energies of 8 and 13 TeV, corresponding to integrated luminosities of 20~$\\text{fb}^{-1}$ and 139~$\\text{fb}^{-1}$, respectively. The events are categorised into two mutually exclusive search regions - the first one with exactly one central jet and at least one forward jet, and the second with at least two central jets and no forward jets. No significant excess above the Standard Model predictions is observed.','cdsLink':'https://cds.cern.ch/record/2684853','journal':'Preliminary','journalSub':'31-JUL-19','ecm':'13','luminosity':'139 fb-1','keywords':'8 TeV,BSM resonance,BSM search,b-jets,1 jet,2 leptons,13 TeV','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-036@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-036@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'11830','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=11830','shortTitle':'DBL - VBF HH to 4b 2018','fullTitle':'Search for $HH \\rightarrow b\\overline{b}bb\\overline{b}$ production via vector boson fusion using proton-proton collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector','pubShortTitle':'VBF HH to 4b','refCode':'ATLAS-CONF-2019-030','abstract':'A search for Higgs boson pair production via vector boson fusion (VBF) in the $b\\bar{b}b\\bar{b}$ final state is carried out with the ATLAS detector, using 126 fb$^{-1}$ of proton--proton collision data delivered at $\\sqrt{s}$ = 13 TeV by the Large Hadron Collider. This search is sensitive to VBF production of additional heavy bosons that may decay to Higgs boson pairs, and in a non-resonant topology it can constrain the parameters of pairs of Higgs bosons coupling with two vector bosons. No significant excess, relative to the Standard Model expectation, is observed and limits on the production cross-section are set at 95% confidence level for a heavy scalar resonance in the context of an extended Higgs sector, and for a non-resonant Standard Model Higgs boson pair production. Interpretation in terms of the coupling between a Higgs boson pair and two vector bosons is also provided.','cdsLink':'https://cds.cern.ch/record/2682801','journal':'Preliminary','journalSub':'11-JUL-19','ecm':'13','luminosity':'126 fb-1','keywords':'13 TeV,BSM resonance,BSM search,VBF,Di-Higgs,b-jets,All hadronic','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-030@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2019-030@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'11307','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=11307','shortTitle':'HGam low-mass resonance search','fullTitle':'Search for Scalar Diphoton Resonances','pubShortTitle':'Search BSM H-> gamma gamma','refCode':'ATLAS-CONF-2018-025','abstract':'A search for low-mass diphoton resonances is performed using 80 fb$^{-1}$ of $pp$ collision data collected with the ATLAS detector at the Large Hadron Collider. Pairs of isolated photon candidates with high transverse momentum are selected, probing the diphoton invariant mass spectrum in the range 65 to 110 GeV. No significant excess with respect to the Standard Model expectation is found, and a limit at the 95% confidence level is set on narrow resonance fiducial cross-section times branching ratio ranging from 30 to 101 fb.','cdsLink':'https://cds.cern.ch/record/2628760','journal':'Preliminary','journalSub':'04-JUL-18','ecm':'13','luminosity':'80 fb-1','keywords':'13 TeV,BSM resonance,Higgs to 2 photons,BSM search,Di-photon,Photon,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2018-025/@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2018-025/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'8489','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=8489','shortTitle':'HTop HBSM charged Higgs to tb','fullTitle':'Search for H+ -> tb with the ATLAS detector in 13 TeV pp collisions','pubShortTitle':'Search BSM H+ -> tb','refCode':'ATLAS-CONF-2016-089','abstract':'A search for charged Higgs bosons heavier than the top quark and decaying via $H^{\\pm} \\to tb$ is presented. The analysis uses 13.2 $\\mathrm{fb^{-1}}$ of $pp$ collision data at a centre-of-mass energy $\\sqrt{s } = 13$ TeV collected with the ATLAS detector at the Large Hadron Collider. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \\to tbH^{\\pm}$, is explored in the mass range 300 to 1000 GeV using multi-jet final states with one electron or muon from the top-quark decay. Events are categorised according to the multiplicity of jet and $b$-tagged jets. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and upper limits are set on the $tbH^{\\pm}$ production cross section times the branching fraction BR($H^ {\\pm}\\to tb$), together with their interpretation in benchmark scenarios of the Minimal Supersymmetric Standard Model.','cdsLink':'https://cds.cern.ch/record/2206809','journal':'Preliminary','journalSub':'09-AUG-16','ecm':'13','luminosity':'13.2 fb-1','keywords':'13 TeV,Charged Higgs searches,BSM resonance,BSM search,Higgs,b-jets,>=3 jets','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-089/@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-089/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'8547','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=8547','shortTitle':'HZZ high mass llqq','fullTitle':'Search for ZZ resonances in the llqq final state in pp collisions at √s = 13 TeV with the ATLAS detector','pubShortTitle':'Search BSM H->ZZ->lljj','refCode':'ATLAS-CONF-2016-016','abstract':'This note reports a search for heavy resonances decaying into a pair of $Z$ bosons, using 3.2 fb$^{-1}$ of proton--proton collision data at a centre-of-mass energy of $\\sqrt{s}=13$ TeV recorded with the ATLAS detector at the Large Hadron Collider. The search is performed in the final state in which one $Z$ boson decays to a pair of charged leptons (electrons or muons) and the other $Z$ boson decays hadronically. The hadronic $Z$ boson candidate is reconstructed either as a pair of small-radius jets or as one large-radius jet. The analysis searches for resonance structures in the invariant mass distributions of the $ZZ$ final state. No evidence for the production of resonances decaying to a $ZZ$ pair is observed. Upper bounds on the production cross sections at $\\sqrt{s}=13$ TeV times their decay branching ratios to $ZZ$ pairs ($\\sigma\\times{\\rm BR}$) are derived for a heavy Higgs boson and a spin-2 Randall-Sundrum graviton. The observed (expected) 95% CL limit on $\\sigma\\times{\\rm BR}$ varies from 5.6 (3.3) pb at 300 GeV to 0.21 (0.11) pb at 1000 GeV for the Higgs boson and from 0.62 (0.52) pb at 500 GeV to 0.20 (0.11) pb at 1000 GeV for the graviton.','cdsLink':'https://cds.cern.ch/record/2141005','journal':'Preliminary','journalSub':'18-MAR-16','ecm':'13','luminosity':'3.2 ','keywords':'13 TeV,BSM resonance,BSM resonance,Higgs to ZZ,BSM search,Higgs,ZZ,2 jets,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-016/@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-016/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'8487','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=8487','shortTitle':'Hbb HBSM A to ZH','fullTitle':'Search for the 2HDM A->ZH with H->bbbar decay','pubShortTitle':'','refCode':'ATLAS-CONF-2016-015','abstract':'A search for a heavy, CP-odd Higgs boson, A, decaying into a Z boson and a CP-even Higgs boson, h, with a mass of 125 GeV is performed using the ATLAS detector at the Large Hadron Collider. The search uses proton–proton collision data at a centre-of-mass energy of 13 TeV corresponding to an integrated luminosity of 3.2 fb−1. Decays of h bosons to pairs of bottom quarks, where the resulting hadronic jets are resolved or merged in the detector, are both considered. Final states of the Z boson decaying to a pair of charged leptons, Z → e+e− and Z → μ+μ−, or into neutrinos, Z → νν, are considered. No evidence for the production of an A boson in these channels is observed. The data are used to determine 95% confidence level upper limits on the product of production cross sections and branching fractions, σ(pp → A)·BR(A → Zh)·BR(h → bb), in the range of [4.0,0.017] pb ([6.9, 0.026] pb) for m A = [220, 2000] GeV assuming exclusively gluon-fusion (b-quark- associated) production. Results are also interpreted in the context of benchmark models for a two-Higgs doublet extension of the Standard Model.','cdsLink':'https://cds.cern.ch/record/2141003','journal':'Preliminary','journalSub':'16-MAR-16','ecm':'13','luminosity':'','keywords':'BSM resonance','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-015/@linkEnd@Documents@descriptionEnd@
','run':'2','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2016-015/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'4745','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=4745','shortTitle':'DBL - LSTC W/Z + pi_T to lv/ll + jj','fullTitle':'Search for LSTC W/Z+techni-pion decay to lv/ll jj at 8 TeV','pubShortTitle':'Search for W/Zjj+X','refCode':'ATLAS-CONF-2013-074','abstract':'A search for a dijet resonance with an invariant mass in the range between 130 and 300~GeV is performed in the processes $pp \\to Wjj+X$ with $W \\to \\ell^{\\pm}\\nu$ and $pp \\to Zjj+X$ with $Z \\to \\ell^+\\ell^-$ ($\\ell = e, \\mu$). The data used correspond to 20.3 fb$^{-1}$ of $pp$ collision data recorded at $\\sqrt{s}=$8~TeV with the ATLAS detector at the CERN Large Hadron Collider. The results are interpreted in terms of constraints on the Low Scale Technicolor model. No significant deviation from the Standard Model background prediction is observed. Upper limits on the production cross section times branching fraction are set for a hypothetical technipion produced in association with a $W$ or $Z$ boson from the decay of a technirho particle.','cdsLink':'https://cds.cern.ch/record/1562930','journal':'Preliminary','journalSub':'16-JUL-13','ecm':'8','luminosity':'20.3 fb-1','keywords':'8 TeV,Other new particle searches,BSM resonance,BSM search,Z,W,2 jets,2 leptons,1 lepton','links':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2013-074@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2013-074@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'3705','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=3705','shortTitle':'4GT - vector-like quarks search 2011','fullTitle':'Search for heavy vector-like quarks coupling to light generations in 5/fb proton-proton collisions at sqrt(s) = 7 TeV','pubShortTitle':'Light Generation Single VLQ search','refCode':'ATLAS-CONF-2012-137','abstract':'This analysis presents a search for singly-produced vector-like quarks (VLQs) coupling to light quark generations in events with a $W$ or $Z$ boson produced in association with two or more high transverse momentum jets. The vector boson produced in the VLQ decay is reconstructed in the $W\\to\\ell\\nu$ or $Z\\to\\ell\\ell$ modes, where $\\ell$ is an electron or a muon. In 4.64~$\\ifb$ of data taken in 2011 by the ATLAS experiment at a centre-of-mass energy of 7~TeV, no evidence of VLQs is observed above the expected background. A fit to the distribution of the invariant mass of the system composed of the vector boson and the highest transverse momentum jet is used to set limits on the heavy quark production cross section times branching ratio, and mass bounds are obtained for different couplings. For coupling equal to $v/m_Q$, 95\\% CL lower limits on the VLQ mass are determined to be $m_{Q}>1120\\gev$ and $m_{Q}>1420\\gev$ for VLQs of charge -1/3 and 5/3 in the $W\\to\\ell\\nu$ channel, and $m_{Q}>1080\\gev$ for a VLQ of charge 2/3 in the $Z\\to\\ell\\ell$ channel.','cdsLink':'https://cds.cern.ch/record/1480628','journal':'Preliminary','journalSub':'24-SEP-12','ecm':'7','luminosity':'5 fb-1','keywords':'7 TeV,Vector-like quarks,BSM resonance,BSM search,Z,W,2 jets,2 leptons,1 lepton','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2012-137@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2012-137@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'3725','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=3725','shortTitle':'NMSSM H to a0a0 to 4photons','fullTitle':'Search for a Higgs boson decaying to four photons through light CP-odd scalar coupling using 4.9 fb-1 of 7 TeV pp collision data taken with ATLAS detector at the LHC','pubShortTitle':'Search BSM H->2a->4gamma','refCode':'ATLAS-CONF-2012-079','abstract':'In some extensions of the Standard Model, such as MCHM or NMSSM, the Higgs boson can couple to light CP-odd scalar particles. This document presents a study of a possible contribution to a Higgs boson signal in the $H\\to\\gamma\\gamma$ channel due to $H\\to a a$ decays, where $a$ is a light CP-odd scalar particle that decays predominantly into two photons before reaching the electromagnetic calorimeter. Although this process yields four photon final states, we show that for $a$ in the mass range of 100-400 MeV, the two photons from each $a$ decay are often collimated so that they may be identified as a single photon. A large fraction of these events would contribute to an effective $H\\rightarrow\\gamma\\gamma$ signal. By following a selection similar to that of the $H\\to\\gamma\\gamma$ analysis, we set experimental limits for a generic class of Standard Model extensions having Higgs boson couplings to light scalar particles, assuming the $a$ decays before reaching the electromagnetic calorimeter. The 95$\\%$ confidence-level exclusion limits are provided on the Higgs boson production cross section times $H\\to a a \\to 4 \\gamma$ branching fraction in the range of $110\\gev < m_H < 150\\GeV$ and for the particle $a$ in the mass range from $100\\mev$ to $400\\MeV$.','cdsLink':'https://cds.cern.ch/record/1460391','journal':'Preliminary','journalSub':'28-JUN-12','ecm':'7','luminosity':'4.9 fb-1','keywords':'7 TeV,NMSSM,Exotic Higgs decays,BSM search,Photons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2012-079/@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2012-079/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'1921','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=1921','shortTitle':'Exotics 4 lepton searches','fullTitle':'Search for Evidence of New Physics in Events with Four Leptons','pubShortTitle':'','refCode':'ATLAS-CONF-2011-144','abstract':'We present two searches for new phenomena in events with four charged leptons, using data from $pp$ collisions at $\\sqrt{s}= 7$\\ TeV collected by the ATLAS detector corresponding to an integrated luminosity of 1.02 fb$^{-1}$. The first search examines the four-lepton dataset for events that contain no identified $Z\\rightarrow\\ell^+\\ell^-$ decays. Owing to the very low expected background, even a small number of such events would be of interest. After selection, $0.7^{+1.3}_{-0.6}{\\rm (stat)}\\ ^{+0.9}_{-0.5}{\\rm (syst)}$ events are expected from standard model backgrounds, and no events are observed. Using doubly-charged Higgs production as a benchmark model, upper limits are set on a fiducial cross-section for four-lepton production of 4.7 fb. A second search examines events with two identified $Z\\rightarrow\\ell^+\\ell^-$ decays for evidence of resonant production of $ZZ$ pairs via a massive graviton. For $M_{\\ell\\ell\\ell\\ell}>300$ GeV, $1.9^{+1.0}_{-0.1}{\\rm (stat)}\\ ^{+0.8}_{-0.1}{\\rm (syst)}$ events are expected from standard model processes, and 3 events are observed. Limits are set on production of $ZZ$ from high-mass sources, $< 0.9$\\ pb in the fiducial region at 95\\% C.L. Using the Randall-Sundrum framework to quantify the result we report limits on $\\sigma(pp\\rightarrow G) \\times BF(G\\rightarrow ZZ)$ of 2.6-3.3\\,pb, depending on the resonance mass. For a coupling of $k/\\bar{M_{pl}}=0.1$, the median expected 95\\% C.L. lower limit on the mass of the graviton is $M_{G}>575$ GeV, equal to the observed limit.','cdsLink':'https://cds.cern.ch/record/1388601','journal':'Preliminary','journalSub':'06-OCT-11','ecm':'7','luminosity':'1 fb-1','keywords':'>=3 leptons,Strong gravity,BSM resonance,BSM search,7 TeV,Di-Higgs,ZZ','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-144/@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-144/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'1241','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=1241','shortTitle':'tt resonances dilepton - 2011 data','fullTitle':'A Search for tt̄ Resonances in the Dilepton Channel in 1.04 fb-1 of pp Collisions at √s = 7 TeV','pubShortTitle':'Search for ttbar Resonances in the Dilepton Channel','refCode':'ATLAS-CONF-2011-123','abstract':'This note presents a search for a high mass ttbar resonance in pp collisions at \\sqrt(s) = 7 TeV at the LHC. We search for such a resonance using the final state where both $W$ bosons from the top quark decay into either an electron and electron-neutrino or a muon and muon-neutrino (dilepton final state). The data were recorded by the ATLAS experiment during 2011 and correspond to a total integrated luminosity of 1.04/fb. No statistically significant excess above the Standard Model expectation is observed. Upper limits at the 95\\% Confidence Limit (C.L) are set on the cross section times branching ratio of the resonance decaying to $t\\bar{t}$ pairs as a function of the resonance pole mass. A lower mass limit of 0.84~TeV is set for the case of a Kaluza Klein gluon resonance in the Randall-Sundrum Model.','cdsLink':'https://cds.cern.ch/record/1376423','journal':'Preliminary','journalSub':'20-AUG-11','ecm':'7','luminosity':'1 fb-1','keywords':'7 TeV,BSM resonance,Other top properties,Top properties measurements,BSM search,Top pair,2 leptons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-123/@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-123/@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'624','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=624','shortTitle':'Background for MSSM Charged Higgs in hadronic tau final state','fullTitle':'Data-driven estimation of the background to ATLAS charged Higgs boson searches with hadronic tau final states','pubShortTitle':'Background for MSSM Charged Higgs in hadronic tau final state','refCode':'ATLAS-CONF-2011-051','abstract':'The experimental observation of charged Higgs bosons, $H^{\\pm}$, which are theoretically predicted by many non-minimal Higgs scenarios, would indicate new physics beyond the Standard Model. In the Minimal Supersymmetric Standard Model, for example, the dominant production mode at the LHC for these Higgs bosons, when $m_{H^+} < m_t$, takes place in $t\\overline{t}$ events via the top-quark decay $t\\rightarrow H^{+}b$ with $H^{+}\\rightarrow\\tau \\nu$ dominating for most values of $\\tan\\beta$. Two channels with a hadronically decaying $\\tau$ coming from the charged Higgs boson are studied. The delivery of the first 37 pb$^{-1}$ of $\\sqrt{s}= 7$ TeV collision data allows many significant backgrounds to be estimated with data-driven methods, which represent the primary focus of this note and a crucial step towards ATLAS searches for the charged Higgs boson.','cdsLink':'https://cds.cern.ch/record/1341816','journal':'Preliminary','journalSub':'29-MAR-11','ecm':'7','luminosity':'37 pb-1','keywords':'7 TeV,Charged Higgs searches,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-051@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-051@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'625','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=625','shortTitle':'Discriminants for MSSM Charged Higgs in leptonic tau final state','fullTitle':'Study of discriminating variables for charged Higgs boson searches in ttbar events with leptons, using 35/pb of data from the ATLAS detector','pubShortTitle':'Study of discriminating variables for charged Higgs -> tau nu in ttbar events','refCode':'ATLAS-CONF-2011-018','abstract':'In several extensions of the Standard Model, the top-quark can decay to a bottom-quark and a light charged Higgs boson ($m_{H^+}<m_{\\text{top}}$) which is assumed to decay only into $\\tau\\nu$. Discriminating variables were identified, which allow the distinction between the leptons produced in $\\tau \\rightarrow l+ \\nu\\mbox{s}$ (arising in decays of $W$ or charged Higgs bosons) and the leptons coming directly from $W$ boson decays. This paper aims at validating these variables, in single-lepton and dilepton $t\\bar{t}$ events, through a comparison between Monte Carlo simulations and 35 pb$^{-1}$ of ATLAS data collected in 7 TeV proton-proton collisions at the LHC, in 2010. We find that Monte Carlo simulations agree well with the ATLAS data. The impact of systematic uncertainties is also discussed.','cdsLink':'https://cds.cern.ch/record/1336747','journal':'Preliminary','journalSub':'10-MAR-11','ecm':'7','luminosity':'35 pb-1','keywords':'7 TeV,Charged Higgs searches,Taus','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-018@linkEnd@Documents@descriptionEnd@
','run':'1','finalPubRef':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-018@linkEnd@Figures@descriptionEnd@','publicationType':'CONF','pressStatement':''},{'publicationId':'622','internalLink':'https://glance.cern.ch/atlas/analysis/confnotes/details.php?id=622','shortTitle':'NMSSM Higgs search in the a1->mumu channel','fullTitle':'A search for light CP-odd Higgs bosons decaying to mu+mu- in ATLAS','pubShortTitle':'Search NMSSM Higgs a1->mumu','refCode':'ATLAS-CONF-2011-020','abstract':'We present a search for a very light \\CP -odd Higgs boson, \\aone , decaying to \\mumu , using 36.7 \\ipb\\ of \\pp\\ collisions at \\rts\\ = 7 \\TeV\\ recorded by the ATLAS detector at the LHC. Such a light Higgs is predicted in Next-to-Minimal Supersymmetric Standard Models (NMSSM) designed to solve the $\\mu$-term problem of the Minimal Supersymmetric Standard Model (MSSM). Its presence can significantly alter the phenomenology of the MSSM Higgs sector. We set new limits on the production cross section times branching ratio, \\sigggaBamm , for \\aone\\ masses of 6 -- 9 \\GeV\\ and 11 -- 12 \\GeV , avoiding the region dominated by the \\Ups\\ resonances.','cdsLink':'https://cds.cern.ch/record/1336749','journal':'Preliminary','journalSub':'11-MAR-11','ecm':'7','luminosity':'39 pb-1','keywords':'2 leptons,NMSSM,BSM resonance,7 TeV,Higgs to 2 muons','links':'@linkBegin@https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2011-020/@linkEnd@Documents@descriptionEnd@
 Global Selections CM Energy Higgs and di-boson searches physics Signature'OR' logic within row 'AND' between rows Analysis characteristics
 Min luminosity : fbpbnbμb−1 Date : Filter by date:

Filtered results: [Papers Confnotes Pubnotes ]

>
>
<!-- stylesheet -->
<!-- Font Awesome stylesheet -->

<!-- Map container -->

 Global Selections CM Energy Physics theme B Physics and Light States Heavy Ion SM Top Higgs      HDBS SUSY Exotics Physics Modelling Tracking Egamma Muon Tau Jet/Etmiss Flavour tagging BSM Searches (SUSY, HDBS, Exotics)   Upgrade Studies
<!--
-->
 Click for further selections criteria ... Signature'OR' logic within row 'AND' between rows Analysis characteristics  Final state particles Min luminosity : fb pb nb μb -1 Date :     Filter by date:

Papers and publications
(Full list of ATLAS papers, List/RSS from CDS) Hide table

<!--
-->
Short Title Group Journal Reference Date √s (TeV) L Links
Conference (CONF) notes with preliminary results on data
(Full list of ATLAS CONF notes) Hide table

<!--
-->
Short Title Group Document Number Date √s (TeV) L Links
Public (PUB) notes with preliminary results on simulated data or interpretations
(Full list of ATLAS PUB notes) Hide table

<!--
-->
Short Title Group Document Number Date √s (TeV) Links

#### Revision 12019-01-31 - AndreasHoecker

Line: 1 to 1
>
>


META TOPICPARENT
name="WebHome"

<!--
Set ALLOWTOPICCHANGE   = GianlucaPicco, MaurizioColautti, atlas-phys-conveners, atlas-physics-coordinators, atlas-mgt-members, atlas-phys-office-developers

-->

<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE FOLLOWING LINES                      -->
<!-- **************************************************************************** -->

MathJax.Hub.Config({tex2jax: {inlineMath: [['$','$'], ['\$','\$']]}});

// ----- COMMON VARIABLES -----
// Color for buttons
var selectedColor = "#357EC7";
var NOTselectedColor = "#f2f2f2";
// Color for buttons' text
var selectedColorText = "#FFFFFF";
var NOTselectedColorText = "#000000";

var thoptions = " bgcolor=\"#357EC7\" valign=\"middle\" style=\"color: #fff;font-weight: normal;border-bottom: .5em solid white;\"";

var papers_header = "<a name=\"papers_table\"></a><span style=\"font-weight: 25px;color:#333333;font-size:130%;font-weight:normal;background-color: #ffffff;\">Papers:</span><span id=\"papers_number\" style=\"color:#AAAAAA;\"></span></br></br>";
papers_header += "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Journal reference</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol3 twikiLast\" align=\"center\">L</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

var papers_header_public = "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Journal reference</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol3 twikiLast\" align=\"center\">L</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

var papers_header_public_withgroup = "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Group</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Journal reference</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol3 twikiLast\" align=\"center\">L</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

var papers_header_public_withgroup_and_id = "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Group</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol1 twikiLast\" align=\"center\"><nobr>Journal reference</nobr></th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol3 twikiLast\" align=\"center\">L</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

var confnotes_header = "<hr style=\"border-top:5px solid #dddddd; margin-top:13px; margin-bottom:13px\">";
confnotes_header += "<a name=\"confnotes_table\"></a><span style=\"font-weight: 25px;color:#333333;font-size:130%;font-weight:normal;background-color: #ffffff;\">Conference notes:</span><span id=\"confnotes_number\" style=\"color:#AAAAAA;\"></span></br></br>";
confnotes_header += "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Document Number</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol3 twikiLast\" align=\"center\">L</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

var pubnotes_header = "<hr style=\"border-top:5px solid #dddddd; margin-top:13px; margin-bottom:13px\">";
pubnotes_header += "<a name=\"pubnotes_table\"></a><span style=\"font-weight: 25px;color:#333333;font-size:130%;font-weight:normal;background-color: #ffffff;\">Public notes:</span><span id=\"pubnotes_number\" style=\"color:#AAAAAA;\"></span></br></br>";
pubnotes_header += "<table cellspacing=\"0\" cellpadding=\"0\" width=\"100%\"><tr style=\"height:2.65em;\"><th"+thoptions+" width=\"50%\" class=\"twikiTableCol0 twikiFirstCol twikiLast\" align=\"left\">&nbsp;&nbsp;Short Title</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Document Number</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol2 twikiLast\" align=\"center\">Date</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLast\" align=\"center\">&radic;s (TeV)</th><th"+thoptions+" width=\"10%\" class=\"twikiTableCol0 twikiLastCol twikiLast\" align=\"center\">Links</th></tr>";

// ----- COMMON FUNCTIONS -----

function luminosityCheckResult(minLumi, minLumiUnit, lumi){
lumi = lumi.replaceAll(", ",",");
if (lumi != ""){
var lumi_array = lumi.split(",");
for (var i=0;i<lumi_array.length;i++){
var l_array = lumi_array[i].split(" ");
var lumiUnit = "";
if (l_array[1] != ""){
lumiUnit = l_array[1].substring(0,2);
}

var lumiConverted = "";

if (l_array[0] != ""){
lumiConverted = l_array[0];
}
if (lumiUnit == ""){
return false;
}else if (lumiUnit == "fb" && lumiConverted != ""){
lumiConverted = lumiConverted;
}else if (lumiUnit == "pb" && lumiConverted != ""){
lumiConverted = lumiConverted / 1000;
}else if (lumiUnit == "nb" && lumiConverted != ""){
lumiConverted = lumiConverted / 1000 / 1000;
}else{
lumiConverted = lumiConverted / 1000 / 1000 / 1000;
}

var minLumiConverted = minLumi;

if (minLumi == ""){
return false;
}else if (minLumiUnit == "fb" && minLumi != ""){
minLumiConverted = minLumi;
}else if (minLumiUnit == "pb" && minLumi != ""){
minLumiConverted = minLumi / 1000;
}else if (minLumiUnit == "nb" && minLumi != ""){
minLumiConverted = minLumi / 1000 / 1000;
}else{
minLumiConverted = minLumi / 1000 / 1000 / 1000;
}

if (parseFloat(lumiConverted) >= parseFloat(minLumiConverted)){
return true;
}
}
return false;
}else{
return false;
}
}

function filterLuminosity(){
var minLum = document.getElementById('min_luminosity').value;
if ((minLum == '') || (parseInt(minLum) < 0)){
}else{
if (document.getElementById('luminosityCheck').value == 'true'){
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('luminosityCheck').value = 'false';
document.getElementById('filter_luminosity').style.background=NOTselectedColor;
document.getElementById('filter_luminosity').style.color=NOTselectedColorText;
makelist();
}else{
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('luminosityCheck').value = 'true';
document.getElementById('filter_luminosity').style.background=selectedColor;
document.getElementById('filter_luminosity').style.color=selectedColorText;
makelist();
}
}
}

function filterDate(type){
var date = document.getElementById('id_min_date').value.split('-');
if (date == ''){
}else{
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('filter_date_lower').style.background = NOTselectedColor;
document.getElementById('filter_date_greater').style.background = NOTselectedColor;
document.getElementById('filter_date_lower').style.color = NOTselectedColorText;
document.getElementById('filter_date_greater').style.color = NOTselectedColorText;
if (type == 'lower'){
if (document.getElementById('dateCheck').value != 'lower'){
document.getElementById('dateCheck').value = 'lower';
document.getElementById('filter_date_lower').style.background = selectedColor;
document.getElementById('filter_date_greater').style.background = NOTselectedColor;
document.getElementById('filter_date_lower').style.color = selectedColorText;
document.getElementById('filter_date_greater').style.color = NOTselectedColorText;
}else{
document.getElementById('dateCheck').value = 'false';
}
}else{
if (document.getElementById('dateCheck').value != 'greater'){
document.getElementById('dateCheck').value = 'greater';
document.getElementById('filter_date_lower').style.background = NOTselectedColor;
document.getElementById('filter_date_greater').style.background = selectedColor;
document.getElementById('filter_date_lower').style.color = NOTselectedColorText;
document.getElementById('filter_date_greater').style.color = selectedColorText;
}else{
document.getElementById('dateCheck').value = 'false';
}
}
makelist();
}
}

String.prototype.replaceAll = function(search, replacement) {
var target = this;
return target.split(search).join(replacement);
};

function arrayContainsAnotherArray(needle, haystack){
var total = needle.length;
var found = 0;
for(var i = 0; i < needle.length; i++){
for(var j = 0; j < haystack.length; j++){
if (needle[i] == haystack[j]){
found = found +1;
}
}
}
if (found == total){
return true;
}else{
return false;
}
}

function goToAnchor(anchor) {
var loc = document.location.toString().split('#')[0];
document.location = loc + '#' + anchor;
return false;
}

function isNewRecord(date){
var dateToCeck = new Date(date);
var today = new Date();
today.setMonth(today.getMonth() - 1);

if (dateToCeck >= today){
return true;
}else{
return false;
}

}

function checkGroups(matrix,elToCheck){
for (var i=0;i<matrix.length;i++){
groupCheck = "";
if (matrix[i] == "B-physics and light states"){
groupCheck = "BPHY";
}else if (matrix[i] == "Heavy Ion"){
groupCheck = "HION";
}else if (matrix[i] == "SM"){
groupCheck = "STDM";
}
else if (matrix[i] == "Top"){
groupCheck = "TOPQ";
}
else if (matrix[i] == "Higgs"){
groupCheck = "HIGG";
}
else if (matrix[i] == "SUSY"){
groupCheck = "SUSY";
}
else if (matrix[i] == "Exotics"){
groupCheck = "EXOT";
}
else if (matrix[i] == "Physics Modelling"){
groupCheck = "PMGR";
}
else if (matrix[i] == "Tracking"){
groupCheck = "IDTR";
}
else if (matrix[i] == "Egamma"){
groupCheck = "EGAM";
}
else if (matrix[i] == "Muon"){
groupCheck = "MUON";
}
else if (matrix[i] == "Tau"){
groupCheck = "TAUP";
}
else if (matrix[i] == "Jet/Etmiss"){
groupCheck = "JETM";
}
else if (matrix[i] == "Flavour tagging"){
groupCheck = "FTAG";
}
//Check the values
if (elToCheck.indexOf(groupCheck) != -1){
return true;
}else if ((matrix[i] == "Physics Modelling") && (elToCheck.indexOf("MCGN") != -1)){
return true;
}
}
return false;
}

function fillRecordNrPaper(){
var result = document.getElementById('total_paper_record_number').value;
var publishedNr = document.getElementById('total_published_paper_record_number').value;
var acceptedNr = document.getElementById('total_accepted_paper_record_number').value;
var submittedNr = document.getElementById('total_submitted_paper_record_number').value;
document.getElementById('paper_records').innerHTML = "<font size=\"1em\" color=\"grey\">" + result + " documents (Published: " + publishedNr + " - Accepted: " + acceptedNr + " - Submitted: " + submittedNr + " )</font>";
}
function fillRecordNrConfnote(){
var result = document.getElementById('total_confnote_record_number').value;
document.getElementById('confnote_records').innerHTML = "<font size=\"1em\" color=\"grey\">" + result + " documents</font>";
}
function fillRecordNrPubnote(){
var result = document.getElementById('total_pubnote_record_number').value;
document.getElementById('pubnote_records').innerHTML = "<font size=\"1em\" color=\"grey\">" + result + " documents</font>";
}
function fillRecordNrPaperConf(){
var result = document.getElementById('total_paper_record_number').value;
var publishedNr = document.getElementById('total_published_paper_record_number').value;
var acceptedNr = document.getElementById('total_accepted_paper_record_number').value;
var submittedNr = document.getElementById('total_submitted_paper_record_number').value;
var conferencesNr = document.getElementById('total_conferences_record_number').value;
document.getElementById('paper_records').innerHTML = "<font size=\"1em\" color=\"grey\">" + result + " documents (Papers published: " + publishedNr + ", accepted: " + acceptedNr + ", submitted: " + submittedNr + "; Conference notes: "+conferencesNr+" )</font>";
}

/* ----- CSS STYLE DEFINITION ------ */

.twikiFirstCol{
}
.twikiLastCol{
}
.datepicker_class{
color: #999999;
}

button:focus {outline:0;}

.tooltip-wrap {
position: relative;
}
.tooltip-wrap .tooltip-content {
display: none;
position: absolute;
bottom: 100%;
left: 5%;
right: 5%;
width: 600px;
background-color: #FFFFFF;
border: 0.1px solid #F2F2F2;
box-shadow: 3px 3px 10px rgba(0, 0, 0, .4);
color: #000000;
}
.tooltip-wrap:hover .tooltip-content {
display: block;
}

var key_item = key;
if (key == "Signature@c_2@leptons@same@charge"){
key = "Signature@c_2@leptons@same@charge";
}

var section = key.substring(0,key.indexOf("_"));
var keyOK = key.substring(key.indexOf("_")+1,key.lenght).replaceAll("@"," ");
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
var generalTitlesArray = document.getElementById('generalTitles').value.substring(0,document.getElementById('generalTitles').value.length - 1).split(",");
var NOgeneralTitlesArray = document.getElementById('NOgeneralTitles').value.substring(0,document.getElementById('NOgeneralTitles').value.length - 1).split(",");
var selectedArray = document.getElementById('selected').value.substring(0,document.getElementById('selected').value.length - 1).split(",");
var selected = document.getElementById('selected').value;

var selectedSections = document.getElementById("selectedSections").value;
var selectedkeys = document.getElementById("selectedKeywords").value;

if (selectedSections.indexOf(section+",") != -1){
if (selectedkeys.indexOf(keyOK+",") != -1){
// KEY ALREADY SELECTED (REMOVE IT)
document.getElementById(key_item).style.background = NOTselectedColor;
document.getElementById(key_item).style.color = NOTselectedColorText;
document.getElementById('selectedKeywords').value = selectedkeys.replace(keyOK+",","");
document.getElementById('selectedSections').value = selectedSections.replace(section+",","");
document.getElementById('selected').value = selected.replace(key+",","");
document.getElementById(section).value = document.getElementById(section).value.replace(keyOK+",","");
}else{
// NEW KEY SAME SECTION (ADD IT)
document.getElementById(key_item).style.background = selectedColor;
document.getElementById(key_item).style.color = selectedColorText;
document.getElementById('selectedKeywords').value += keyOK+",";
document.getElementById('selectedSections').value += section+",";
document.getElementById('selected').value += key+",";
document.getElementById(section).value += keyOK+",";
}
}else{
// NEW SECTION SELECTED
//if (generalTitlesArray.includes(section)){
if (generalTitlesArray.indexOf(section) != -1){
// GENERAL SECTION
document.getElementById(key_item).style.background = selectedColor;
document.getElementById(key_item).style.color = selectedColorText;
document.getElementById('selectedKeywords').value += keyOK+",";
document.getElementById('selectedSections').value += section+",";
document.getElementById('selected').value += key+",";
document.getElementById(section).value += keyOK+",";
}else{
// SECTION IS NOT GENERAL
// (Check if I can add it or I need to remove all other section)
var sectionsWithNoGeneral = selectedSections;
// Remove all general from the selected sections (just for check)
for (var c=0;c<generalTitlesArray.length;c++){
sectionsWithNoGeneral = sectionsWithNoGeneral.replace(generalTitlesArray[c]+",","");
}
if (sectionsWithNoGeneral.length == 0){
// ONLY GENERAL KEYWORDS BEFORE, I CAN ADD THE KEY
document.getElementById(key_item).style.background = selectedColor;
document.getElementById(key_item).style.color = selectedColorText;
document.getElementById('selectedKeywords').value += keyOK+",";
document.getElementById('selectedSections').value += section+",";
document.getElementById('selected').value += key+",";
document.getElementById(section).value += keyOK+",";
}else{
// I MUST REMOVE ALL NO GENERAL KEYS
for (var s=0;s<selectedArray.length;s++){
var tempSection = selectedArray[s].substring(0,selectedArray[s].indexOf("_"));
var tempKey = selectedArray[s].substring(selectedArray[s].indexOf("_")+1,selectedArray[s].length).replaceAll("@"," ");
//if (!generalTitlesArray.includes(tempSection)){
if (generalTitlesArray.indexOf(tempSection) == -1){
// REMOVE ALL NON GENERAL KEYS
var tempKeyOK = tempKey.replaceAll("@"," ");
document.getElementById(selectedArray[s]).style.background = NOTselectedColor;
document.getElementById(selectedArray[s]).style.color = NOTselectedColorText;
document.getElementById('selectedKeywords').value = document.getElementById('selectedKeywords').value.replace(tempKeyOK+",","");
document.getElementById('selectedSections').value = document.getElementById('selectedSections').value.replace(tempSection+",","");
document.getElementById('selected').value = document.getElementById('selected').value.replace(selectedArray[s]+",","");
document.getElementById(tempSection).value = document.getElementById(section).value.replace(tempKeyOK+",","");
}
}
document.getElementById(key_item).style.background = selectedColor;
document.getElementById(key_item).style.color = selectedColorText;
document.getElementById('selectedKeywords').value += keyOK+",";
document.getElementById('selectedSections').value += section+",";
document.getElementById('selected').value += key+",";
document.getElementById(section).value += keyOK+",";
}
}
}
}

function makelist(){
var minLuminosity = document.getElementById('min_luminosity').value;
var minLuminosityUnit = document.getElementById('min_luminosity_unit').value;
var luminosityCheck = false;
if (document.getElementById('luminosityCheck').value == 'true'){
luminosityCheck = true;
}

var dateCheck = 'false';
if (document.getElementById('dateCheck').value != 'false'){
dateCheck = document.getElementById('dateCheck').value;
var date = document.getElementById('id_min_date').value.split('-');

var d = new Date(date[0],date[1]-1,date[2]);
}

// RETRIEVE NEEDED HIDDEN FIELDS's VALUES
document.getElementById("spanList").innerHTML = "";
var generalTitlesArray = document.getElementById('generalTitles').value.substring(0,document.getElementById('generalTitles').value.length - 1).split(",");
var NOgeneralTitlesArray = document.getElementById('NOgeneralTitles').value.substring(0,document.getElementById('NOgeneralTitles').value.length - 1).split(",");
var selectedKeywordsArray = document.getElementById('selectedKeywords').value.substring(0,document.getElementById('selectedKeywords').value.length - 1).split(",");
var selectedSectionArray = document.getElementById('selectedSections').value.substring(0,document.getElementById('selectedSections').value.length - 1).split(",");
var selectedArray = document.getElementById('selected').value.substring(0,document.getElementById('selected').value.length - 1).split(",");

var matrix = [];

var uniqueSections = [];

// REMOVE DUPLICATE SECTIONS NAMES
$.each(selectedSectionArray, function(i, el){ if($.inArray(el, uniqueSections) === -1) uniqueSections.push(el);
});

// IF I HAVE SOME SECTION ADD THE KEYWORDS TO keysArr
if (uniqueSections[0] != ""){
for (var s=0;s<uniqueSections.length;s++){
var tempKeyForArray = document.getElementById(uniqueSections[s]).value.substring(0,document.getElementById(uniqueSections[s]).value.length - 1).replaceAll("2 leptons same charge","2 leptons (same charge)");
var keysArray = tempKeyForArray.split(",");
matrix.push(keysArray);
}
}else if (luminosityCheck){
// IF NO SECTIONS SELECTED BUT LUMINOSITY CHECK NEEDED ADD ALL THE SECTIONS
uniqueSections = generalTitlesArray.concat(NOgeneralTitlesArray);
for (var s=0;s<uniqueSections.length;s++){
var tempKeyForArray = document.getElementById(uniqueSections[s]).value.substring(0,document.getElementById(uniqueSections[s]).value.length - 1).replaceAll("2 leptons same charge","2 leptons (same charge)");
var keysArray = tempKeyForArray.split(",");
matrix.push(keysArray);
}
}else if (dateCheck != ""){
// IF NO SECTIONS SELECTED BUT DATE CHECK NEEDED ADD ALL THE SECTIONS
uniqueSections = generalTitlesArray.concat(NOgeneralTitlesArray);
for (var s=0;s<uniqueSections.length;s++){
var tempKeyForArray = document.getElementById(uniqueSections[s]).value.substring(0,document.getElementById(uniqueSections[s]).value.length - 1).replaceAll("2 leptons same charge","2 leptons (same charge)");
var keysArray = tempKeyForArray.split(",");
matrix.push(keysArray);
}
}

var n_matrix = matrix.length;

var json = document.getElementById("publicationList").value;
json = json.replaceAll("'","\"");
myArr = JSON.parse(json);

var rowNumber_paper = 0;
var rowNumber_conf = 0;
var rowNumber_pub = 0;
var results_table_paper = "";
var results_table_conf = "";
var results_table_pub = "";

var monthsDict = {};
monthsDict.JAN = "01";monthsDict.FEB = "02";monthsDict.MAR = "03";monthsDict.APR = "04";monthsDict.MAY = "05";monthsDict.JUN = "06";
monthsDict.JUL = "07";monthsDict.AUG = "08";monthsDict.SEP = "09";monthsDict.OCT = "10";monthsDict.NOV = "11";monthsDict.DEC = "12";

for (var j=0;j<myArr.papers.length;j++){
var elToCheck = myArr.papers[j].keywords.split(",");
var elToCheckECM = myArr.papers[j].ecm.split(",");
var results = [];
var ecmCheck = [];

var paperECM = myArr.papers[j].ecm.split(",");
for (var e=0;e<selectedKeywordsArray.length;e++){
if ((selectedKeywordsArray[e] == "900 GeV") || (selectedKeywordsArray[e] == "5.02 TeV") || (selectedKeywordsArray[e] == "7 TeV") || (selectedKeywordsArray[e] == "8 TeV") || (selectedKeywordsArray[e] == "13 TeV")){
ecmCheck[ecmCheck.length] = selectedKeywordsArray[e].replace("900 GeV","0.9").replace(" TeV","");
}
}

var luminosityOK = false;
if (parseInt(myArr.papers[j].luminosity) <= minLuminosity){
luminosityOK = true;
}

var dateOK = false;
// Get the record date
if (dateCheck != 'false'){
var thisDateSplitted = myArr.papers[j].journalSub.split("-");
var year = "20"+thisDateSplitted[2];
var thisd = new Date(year,monthsDict[thisDateSplitted[1]]-1,thisDateSplitted[0]);
}

// CHECK IF ITEM CONTAINS KEYWORDS
// matrix contains the keys selected
// elToCheck contains the keys associated to a record
for (var c=0;c<n_matrix;c++){
var approved_condition = false;
for (var i=0;i<elToCheck.length;i++){
if (matrix[c].indexOf(elToCheck[i]) != -1){
// KEY PRESENT
approved_condition = true;
results[c] = true;
break;
}else{
// KEY NOT PRESENT
if (((matrix[c].indexOf("7 TeV") != -1) || (matrix[c].indexOf("900 GeV") != -1) || (matrix[c].indexOf("5.02 TeV") != -1) || (matrix[c].indexOf("8 TeV") != -1) || (matrix[c].indexOf("13 TeV") != -1)) && ((results[c] == false) || (results[c] === undefined))){
// Record have no keywords but should have the right ecm value inside must check it
if (myArr.papers[j].ecm != " "){
var ecmTempArray = myArr.papers[j].ecm.split(",");
for (var e=0;e<ecmTempArray.length;e++){
var value = ecmTempArray[e].replace(" ","").replace("/NN","");
if (value == "0.9"){
value = "900 GeV";
}else{
value = value + " TeV";
}
if (matrix[c].indexOf(value) != -1){
approved_condition = true;
results[c] = true;
break;
}else{
approved_condition = false;
results[c] = false;
}
}
}
}else{
if (results[c] != true){
approved_condition = false;
results[c] = false;
}
}
}
}
}

var final_result = false;
var luminosityValue = myArr.papers[j].luminosity;

for (var r=0;r<results.length;r++){
if (keysArray[0] == ""){
// NO ELEMENT TO CHECK
if (luminosityCheck){
// CHECK LUMI
if (dateCheck != 'false'){
// CHECK LUMI + DATE
if (dateCheck == 'lower'){
if ((luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)) && (thisd <= d)){
final_result = true;
}else{
final_result = false;
break;
}
}else{
if ((luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)) && (thisd >= d)){
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
// CHECK ONLY LUMI
if (luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)){
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
if (dateCheck != 'false'){
// CHECK DATE
if (dateCheck == 'lower'){
if (thisd <= d){
final_result = true;
}else{
final_result = false;
break;
}
}else{
if (thisd >= d){
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
if (results[r] == true){
final_result = true;
}else{
final_result = false;
break;
}
}
}
}else{
// SOME ELEMENT TO CHECK + MAYBE LUMI
if (luminosityCheck){
if (dateCheck != 'false'){
// CHECK ELEMENT + LUMI + DATE
if (dateCheck == 'lower'){
if ((luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)) && (results[r] == true) && (thisd <= d)) {
final_result = true;
}else{
final_result = false;
break;
}
}else{
if ((luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)) && (results[r] == true) && (thisd >= d)) {
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
// CHECK ELEMENT + LUMI
if ((luminosityCheckResult(minLuminosity, minLuminosityUnit, luminosityValue)) && (results[r] == true)) {
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
// CHECK ELEMENT
if (dateCheck != 'false'){
// CHECK ELEMENT + DATE
if (dateCheck == 'lower'){
if ((results[r] == true) && (thisd <= d)) {
final_result = true;
}else{
final_result = false;
break;
}
}else{
if ((results[r] == true) && (thisd >= d)) {
final_result = true;
}else{
final_result = false;
break;
}
}
}else{
if (results[r] == true){
final_result = true;
}else{
final_result = false;
break;
}
}
}
}
}

if (final_result){

// COMMON VARIABLES
var pubShortTitleFix = myArr.papers[j].pubShortTitle.replaceAll("###","$"); var fullTitleFix = myArr.papers[j].fullTitle.replaceAll("###","$");

var finalPubRefFix = "";

var title = '';
if (pubShortTitleFix == ''){
title = fullTitleFix;
}else{
title = pubShortTitleFix;
}

var abstractResult = "";
if (myArr.papers[j].abstract != ""){
abstractResult = "<p><b>Abstract: </b>"+myArr.papers[j].abstract.replaceAll("MC@@NLO","MC@NLO")+"</p>";
}

// Style definitions
var color = "bgcolor=\"#eeeeee\"";
/*if (rowNumber_paper % 2 == 0){
color = "bgcolor=\"#edf4f9\"";
}*/
var newImageOption = "";
if (isNewRecord(myArr.papers[j].journalSub)){
newImageOption = "&nbsp;&nbsp;<img src=\"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSOFFICE/new-icon.png\">";
}

if (myArr.papers[j].publicationType == "PAPER") {
//PAPER
}

finalPubRefArray = myArr.papers[j].finalPubRef.split(",");
var doiDescription = "";
var JournalReferenceDescription = "";
for (var k=0;k<finalPubRefArray.length;k++){
console.log(k);
if (finalPubRefArray[k].indexOf("DOI") != -1 || finalPubRefArray[k].indexOf("doi") != -1){
}else if ((finalPubRefArray[k] != "") && (finalPubRefArray[k].toUpperCase().indexOf("INSPIRE") == -1) && (finalPubRefArray[k].toUpperCase().indexOf("ERRATUM") == -1) && (finalPubRefArray[k].toUpperCase().indexOf("ADDENDUM") == -1)){
}
if (doiLink != "" && JournalReferenceDescription != ""){
finalPubRefLink = '<a href="' + doiLink + '" target="_blank">' + JournalReferenceDescription + '</a>';
}else if (doiLink != "" && JournalReferenceDescription == ""){
finalPubRefLink = '<a href="' + doiLink + '" target="_blank">' + doiDescription + '</a>';
}else if (doiLink == "" && JournalReferenceLink != "" && JournalReferenceDescription != ""){
finalPubRefLink = '<a href="' + JournalReferenceLink + '" target="_blank">' + JournalReferenceDescription + '</a>';
}

}

if ((finalPubRefFix == "<a href='' target=\"_blank\"></a>") || (finalPubRefFix == "")){
finalPubRefFix = "Submitted to " + myArr.papers[j].journal;
}

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

results_table_paper += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
results_table_paper += "</td><td width=\"10%\" style=\""+columnStyle+"\">"+finalPubRefFix+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].luminosity+"</td><td width=\"10%\" style=\""+columnStyle+"white-space: nowrap;\">"+linkFix+"</td></tr>";
rowNumber_paper += 1;

}else if (myArr.papers[j].publicationType == "CONF") {
//CONFNOTE
}

if (myArr.papers[j].publicationType == 'CONF'){
finalPubRefFix = myArr.papers[j].journal;
}else{
finalPubRefFix = finalPubRefFix.replaceAll("@descriptionEnd@","</a>");
if (finalPubRefFix == ""){
finalPubRefFix = myArr.papers[j].journal;
}
}

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

var DocumentNumber = "";
}else{
DocumentNumber = myArr.papers[j].refCode
}

results_table_conf += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
//<td width=\"10%\" style=\""+columnStyle+"\">"+finalPubRefFix+"</td>
results_table_conf += "</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\"><nobr>"+DocumentNumber+"</nobr></td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].luminosity+"</td><td width=\"10%\" style=\""+columnStyle+"white-space: nowrap;\">"+linkFix+"</td></tr>";
rowNumber_conf += 1;
}else if (myArr.papers[j].publicationType == "PUB") {
//PUBNOTE
}

if (myArr.papers[j].publicationType == 'CONF'){
finalPubRefFix = myArr.papers[j].journal;
}else{
finalPubRefFix = finalPubRefFix.replaceAll("@descriptionEnd@","</a>");
if (finalPubRefFix == ""){
finalPubRefFix = myArr.papers[j].journal;
}
}

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

var DocumentNumber = "";
}else{
DocumentNumber = myArr.papers[j].refCode
}

results_table_pub += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
results_table_pub += "</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\"><nobr>"+DocumentNumber+"</nobr></td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\"style=\""+columnStyle+"white-space: nowrap;\" >"+linkFix+"</td></tr>";
rowNumber_pub += 1;
}
}
}
if (results_table_paper == "" && results_table_conf == "" && results_table_pub == ""){
}
document.getElementById("spanList").innerHTML = "";
if (results_table_paper != ""){
document.getElementById("spanList").innerHTML = "</table>"+results_table_paper;
}
if (results_table_conf != ""){
document.getElementById("spanList").innerHTML += "</table>"+results_table_conf;
}
if (results_table_pub != ""){
document.getElementById("spanList").innerHTML += "</table>"+results_table_pub;
}

// SET THE TOTAL NUMBER OF RESULTS
if (document.getElementById("papers_number")){
document.getElementById("papers_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_paper+")";
}
if (document.getElementById("confnotes_number")){
document.getElementById("confnotes_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_conf+")";
}
if (document.getElementById("pubnotes_number")){
document.getElementById("pubnotes_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_pub+")";
}

MathJax.Hub.Queue(["Typeset",MathJax.Hub]);
}

function makeListTotal(max){
if(max === undefined) {
max = 9999;
}
console.log("Make list total: "+max);
var json = document.getElementById("publicationList").value;
//console.log(json);
json = json.replaceAll("'","\"");
myArr = JSON.parse(json);

var rowNumber_paper = 0;
var maxNumber_paper = max;
var rowNumber_conf = 0;
var maxNumber_conf = max;
var rowNumber_pub = 0;
var maxNumber_pub = max;
var results_table_paper = "";
var results_table_conf = "";
var results_table_pub = "";

for (var j=0;j<myArr.papers.length;j++){
// Common Variables
var pubShortTitleFix = myArr.papers[j].pubShortTitle.replaceAll("###","$"); var fullTitleFix = myArr.papers[j].fullTitle.replaceAll("###","$");
var finalPubRefFix = "";

if (myArr.papers[j].publicationType == "PUB"){
}

var title = '';
if (pubShortTitleFix == ''){
title = fullTitleFix;
}else{
title = pubShortTitleFix;
}

var abstractResult = "";
if (myArr.papers[j].abstract != ""){
abstractResult = "<p><b>Abstract: </b>"+myArr.papers[j].abstract+"</p>";
}

// Style definitions
var color = "bgcolor=\"#eeeeee\"";
/*if (rowNumber_paper % 2 == 0){
color = "bgcolor=\"#edf4f9\"";
}*/
var newImageOption = "";
if (isNewRecord(myArr.papers[j].journalSub)){
newImageOption = "&nbsp;&nbsp;<img src=\"https://atlas.web.cern.ch/Atlas/GROUPS/PHYSOFFICE/new-icon.png\">"
}

if ((myArr.papers[j].publicationType == "PAPER") && (rowNumber_paper < maxNumber_paper)){
//PAPER
console.log('PAPER');

}

finalPubRefArray = myArr.papers[j].finalPubRef.split(",");
var doiDescription = "";
var JournalReferenceDescription = "";
for (var k=0;k<finalPubRefArray.length;k++){
console.log(k);
if (finalPubRefArray[k].indexOf("DOI") != -1 || finalPubRefArray[k].indexOf("doi") != -1){
}else if ((finalPubRefArray[k] != "") && (finalPubRefArray[k].toUpperCase().indexOf("INSPIRE") == -1) && (finalPubRefArray[k].toUpperCase().indexOf("ERRATUM") == -1) && (finalPubRefArray[k].toUpperCase().indexOf("ADDENDUM") == -1)){
}
if (doiLink != "" && JournalReferenceDescription != ""){
finalPubRefLink = '<a href="' + doiLink + '" target="_blank">' + JournalReferenceDescription + '</a>';
}else if (doiLink != "" && JournalReferenceDescription == ""){
finalPubRefLink = '<a href="' + doiLink + '" target="_blank">' + doiDescription + '</a>';
}else if (doiLink == "" && JournalReferenceLink != "" && JournalReferenceDescription != ""){
finalPubRefLink = '<a href="' + JournalReferenceLink + '" target="_blank">' + JournalReferenceDescription + '</a>';
}

}

if ((finalPubRefFix == "<a href='' target=\"_blank\"></a>") || (finalPubRefFix == "")){
finalPubRefFix = "Submitted to " + myArr.papers[j].journal;
}

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

results_table_paper += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
results_table_paper += "<td width=\"10%\" style=\""+columnStyle+"\">"+finalPubRefFix+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].luminosity+"</td><td width=\"10%\" style=\""+columnStyle+"white-space: nowrap;\">"+linkFix+"</td></tr>";
rowNumber_paper += 1;
}else if ((myArr.papers[j].publicationType == "CONF") && (rowNumber_conf < maxNumber_conf)){
//CONFNOTE
console.log('CONFNOTE');

}

finalPubRefFix = myArr.papers[j].journal;

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

var DocumentNumber = "";
}else{
DocumentNumber = myArr.papers[j].refCode
}

results_table_conf += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
results_table_conf += "</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\"><nobr>"+DocumentNumber+"</nobr></td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].luminosity+"</td><td width=\"10%\" style=\""+columnStyle+"\"white-space: nowrap;>"+linkFix+"</td></tr>";
rowNumber_conf += 1;
}else if ((myArr.papers[j].publicationType == "PUB") && (rowNumber_pub < maxNumber_pub)) {
//PUBNOTE
console.log('PUBNOTE');

}

finalPubRefFix = finalPubRefFix.replaceAll("@descriptionEnd@","</a>");
if (finalPubRefFix == ""){
finalPubRefFix = myArr.papers[j].journal;
}

if (myArr.papers[j].pressStatement != ""){
linkFix += ' <a href="'+myArr.papers[j].pressStatement+'" target=\"_blank\">Press Statement</a> | ';
}

var DocumentNumber = "";
}else{
DocumentNumber = myArr.papers[j].refCode
}

results_table_pub += "<tr "+color+"><td width=\"50%\" style=\""+columnStyle+"\"><span class=\"tooltip-wrap\" onmouseover=\"document.getElementById('previsouTextColor').value=this.parentElement.style.color;this.parentElement.style.color = '#357EC7';\" onmouseout=\"this.parentElement.style.color = document.getElementById('previsouTextColor').value;\">"+title+newImageOption+"<span class=\"tooltip-content\"><b>Full Title:</b> "+myArr.papers[j].fullTitle+abstractResult+"<p style=\"font-size:0.8em;color:grey;\"><b>Keywords:</b> "+myArr.papers[j].keywords.replaceAll(",",", ")+"</p></span></span></td>";
results_table_pub += "</td><td width=\"10%\"  style=\""+columnStyle+"\" align=\"center\"><nobr>"+DocumentNumber+"</nobr></td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].journalSub+"</td><td width=\"10%\" style=\""+columnStyle+"\" align=\"center\">"+myArr.papers[j].ecm+"</td><td width=\"10%\" style=\""+columnStyle+"\"white-space: nowrap;>"+linkFix+"</td></tr>";
rowNumber_pub += 1;
}
}
if (results_table_paper == "" && results_table_conf == "" && results_table_pub == ""){
}
document.getElementById("spanList").innerHTML = "";
if (results_table_paper != ""){
document.getElementById("spanList").innerHTML = "</table>"+results_table_paper;
}
if (results_table_conf != ""){
document.getElementById("spanList").innerHTML += "</table>"+results_table_conf;
}
if (results_table_pub != ""){
document.getElementById("spanList").innerHTML += "</table>"+results_table_pub;
}

// SET THE TOTAL NUMBER OF RESULTS
if (document.getElementById("papers_number")){
document.getElementById("papers_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_paper+")";
}
if (document.getElementById("confnotes_number")){
document.getElementById("confnotes_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_conf+")";
}
if (document.getElementById("pubnotes_number")){
document.getElementById("pubnotes_number").innerHTML = "&nbsp;&nbsp;&nbsp;("+rowNumber_pub+")";
}

MathJax.Hub.Queue(["Typeset",MathJax.Hub]);
}

function filterLuminosity(){
var minLum = document.getElementById('min_luminosity').value;
if ((minLum == '') || (parseInt(minLum) < 0)){
}else{
if (document.getElementById('luminosityCheck').value == 'true'){
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('luminosityCheck').value = 'false';
document.getElementById('filter_luminosity').style.background=NOTselectedColor;
document.getElementById('filter_luminosity').style.color=NOTselectedColorText;
makelist();
}else{
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('luminosityCheck').value = 'true';
document.getElementById('filter_luminosity').style.background=selectedColor;
document.getElementById('filter_luminosity').style.color=selectedColorText;
makelist();
}
}
}

function filterDate(type){
var date = document.getElementById('id_min_date').value.split('-');
if (date == ''){
}else{
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
document.getElementById('filter_date_lower').style.background = NOTselectedColor;
document.getElementById('filter_date_greater').style.background = NOTselectedColor;
document.getElementById('filter_date_lower').style.color = NOTselectedColorText;
document.getElementById('filter_date_greater').style.color = NOTselectedColorText;
if (type == 'lower'){
if (document.getElementById('dateCheck').value != 'lower'){
document.getElementById('dateCheck').value = 'lower';
document.getElementById('filter_date_lower').style.background = selectedColor;
document.getElementById('filter_date_greater').style.background = NOTselectedColor;
document.getElementById('filter_date_lower').style.color = selectedColorText;
document.getElementById('filter_date_greater').style.color = NOTselectedColorText;
}else{
document.getElementById('dateCheck').value = 'false';
}
}else{
if (document.getElementById('dateCheck').value != 'greater'){
document.getElementById('dateCheck').value = 'greater';
document.getElementById('filter_date_lower').style.background = NOTselectedColor;
document.getElementById('filter_date_greater').style.background = selectedColor;
document.getElementById('filter_date_lower').style.color = NOTselectedColorText;
document.getElementById('filter_date_greater').style.color = selectedColorText;
}else{
document.getElementById('dateCheck').value = 'false';
}
}
makelist();
}
}

function showtable(id) {
var visible = document.getElementById('visible_table').value;
if (visible == ""){
document.getElementById(id).style.display = '';
document.getElementById(id.replaceAll("_table","_button")).style.background=selectedColor;
document.getElementById(id.replaceAll("_table","_button")).style.color=selectedColorText;
document.getElementById('visible_table').value = id;
}else{
if (visible == id){
document.getElementById(id).style.display = 'none';
document.getElementById(id.replaceAll("_table","_button")).style.background=NOTselectedColor;
document.getElementById(id.replaceAll("_table","_button")).style.color=NOTselectedColorText;
document.getElementById('visible_table').value = '';
}else{
document.getElementById(id).style.display = '';
document.getElementById(id.replaceAll("_table","_button")).style.background=selectedColor;
document.getElementById(id.replaceAll("_table","_button")).style.color=selectedColorText;
document.getElementById(visible).style.display = 'none';
document.getElementById(visible.replaceAll("_table","_button")).style.background=NOTselectedColor;
document.getElementById(visible.replaceAll("_table","_button")).style.color=NOTselectedColorText;
document.getElementById('visible_table').value = id;
}
}
}

function showAll(){
document.getElementById('luminosityCheck').value = "false";
makeListTotal();
if (document.getElementById("globalSelection").value == ""){
document.getElementById("showAll_button").style.background = selectedColor;
document.getElementById("showAll_button").style.color = selectedColorText;
document.getElementById("globalSelection").value = "showAll";
clearButtonsSelection();
}else if (document.getElementById("globalSelection").value == "showAll"){
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
}else if (document.getElementById("globalSelection").value == "deselectAll"){
document.getElementById("showAll_button").style.background = selectedColor;
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.color = selectedColorText;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "showAll";
clearButtonsSelection();
document.getElementById("showAll_button").style.background = selectedColor;
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.color = selectedColorText;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "showAll";
clearButtonsSelection();
}
}

document.getElementById('luminosityCheck').value = "false";
makeListTotal(20);
if (document.getElementById("globalSelection").value == ""){
clearButtonsSelection();
}else if (document.getElementById("globalSelection").value == "showAll"){
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
}else if (document.getElementById("globalSelection").value == "deselectAll"){
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
}
}
}

function deselectAll(){
document.getElementById('luminosityCheck').value = "false";
if (document.getElementById("globalSelection").value == ""){
document.getElementById("deselectAll_button").style.background = selectedColor;
document.getElementById("deselectAll_button").style.color = selectedColorText;
document.getElementById("globalSelection").value = "deselectAll";
document.getElementById("spanList").innerHTML = "";
clearButtonsSelection();
// selectedbutton to hide
}else if (document.getElementById("globalSelection").value == "deselectAll"){
document.getElementById("deselectAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "";
}else if (document.getElementById("globalSelection").value == "showAll"){
document.getElementById("deselectAll_button").style.background = selectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = selectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "deselectAll";
document.getElementById("spanList").innerHTML = "";
clearButtonsSelection();
document.getElementById("deselectAll_button").style.background = selectedColor;
document.getElementById("showAll_button").style.background = NOTselectedColor;
document.getElementById("deselectAll_button").style.color = selectedColorText;
document.getElementById("showAll_button").style.color = NOTselectedColorText;
document.getElementById("globalSelection").value = "deselectAll";
document.getElementById("spanList").innerHTML = "";
clearButtonsSelection();
}
}

function clearButtonsSelection(){
var toDeselectTemp = document.getElementById("selected").value.substring(0,document.getElementById("selected").value.length-1);
toDeselectTemp = toDeselectTemp.replaceAll("Signature@c_2@leptons","Signature@c_2@leptons@same@charge");
var toDeselect = toDeselectTemp.split(",");
if (toDeselect[0] != ""){
for (var i=0;i<toDeselect.length;i++){
console.log(toDeselect[i]);
document.getElementById(toDeselect[i]).style.background = NOTselectedColor;
document.getElementById(toDeselect[i]).style.color = NOTselectedColorText;
var sect = toDeselect[i].split("_");
document.getElementById(sect[0]).value = ""
}
}
document.getElementById("filter_luminosity").style.background = NOTselectedColor;
document.getElementById("filter_date_lower").style.background = NOTselectedColor;
document.getElementById("filter_date_greater").style.background = NOTselectedColor;
document.getElementById("filter_luminosity").style.color = NOTselectedColorText;
document.getElementById("filter_date_lower").style.color = NOTselectedColorText;
document.getElementById("filter_date_greater").style.color = NOTselectedColorText;
document.getElementById("selectedKeywords").value = "";
document.getElementById("selectedSections").value = "";
document.getElementById("selected").value = "";
}

<!-- **************************************************************************** -->
<!--                        DO NOT EDIT THE PREVIOUS LINES                      -->
<!-- **************************************************************************** -->

Higgs and Diboson Searches

Contact: ATLAS HDBS Working Group Conveners

This page gives access to the publicly-available studies and results from the ATLAS Higgs and Diboson Searches (HDBS) Working Group. Only this material is approved for showing in public by speakers from ATLAS or other collaborations.

<!--            Include: Filtering tables, Papers, Confnotes, Pubnotes, Plots              -->

<!-- ***********************INCLUDE PLOT SECTION************************************* -->

Filter Documents

Select the desired keywords to filter the results. Selections within a section row are combined with a logical OR, while selections among different section rows are combined with a logical AND.
<!-- ***********************INCLUDE FILTER SECTION************************************* -->