Difference: PhysicsResultsEXO12048 (32 vs. 33)

Revision 332014-09-02 - PhatSrimanobhas

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META TOPICPARENT name="HcalRocMonoJet2012"

Search for new physics in monojet events in pp collisions at sqrt(s) = 8 TeV

Abstract

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A search has been made for events containing an energetic jet and an imbalance in transverse momentum using a data sample of pp collisions at a center-of-mass energy of 8 TeV. The data were collected by the CMS detector at the LHC and correspond to an integrated luminosity of 19.5fb-1. The number of observed events is consistent with the standard model expectation. Constraints on the dark matter-nucleon scattering cross sections are determined for both spin-independent and spin-dependent interaction models. Limits are also placed on the Arkani-Hamed, Dimopoulos, and Dvali model parameter MD determined as a function of the number of extra dimensions and the production of Unparticles. The Physics Analysis Summary is here: EXO-12-048 PAS
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Results are presented from a search for particle dark matter (DM), extra dimensions, and unparticles using events containing a jet and an imbalance in transverse momentum. The data were collected by the CMS detector in proton-proton collisions at the LHC and correspond to an integrated luminosity of 19.7 fb-1 at a centre-of-mass energy of 8 TeV. The number of observed events is found to be consistent with the standard model prediction. Limits are placed on the DM-nucleon scattering cross section as a function of the DM particle mass for spin-dependent and spin-independent interactions. Limits are also placed on the scale parameter MD in the ADD model of large extra dimensions, and on the unparticle model parameter ΛU. The constraints on ADD models and unparticles are the most stringent limits in this channel and those on the DM-nucleon scattering cross section are an improvement over previous collider results.
 
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Approved Plots from EXO-12-048 PAS

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Approved plots and figures from EXO-12-048

 
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Figure Caption
Jet1Pt_overflow.jpg Transverse momentum distribution of the leading pT jet . The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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Jet1Eta.jpg Pseudorapidity distribution of the leading pT jet . The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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NJet_Nm1.jpg The jet multiplicity distribution. The figure is shown with all analysis cuts applied, except jet multiplicity. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, and ∆φ(j1, j2) < 2.5.
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dPhi_Jet1_Jet2_Nm1.jpg The ∆φ(j1, j2) distribution. The figure is shown with all analysis cuts applied except ∆φ(j1, j2). Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, and NJets ≤ 2.
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Met.jpg Met_NoRatio.jpg Missing transverse momentum after all selection cuts for data and SM backgrounds. Representative signal points for dark matter, ADD and Unparticles are also overlaid. Events with Emiss > 1 TeV are included in the overflow bin.
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ZleplepM_60_120.jpg The dimuon invariant mass distribution is shown for data (black full points with error bars) and simulation (histogram) for 60 < Mμμ < 120 GeV/c2. The MC prediction has been normalized to the data yields. There is no significant non-Z background.
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ZleplepPT_60_120.jpg The dimuon pT distribution is shown for data (black full points with error bars) and simulation (histogram) for 60 < Mμμ < 120 GeV/c2. The MC prediction has been normalized to the data yields. There is no significant non-Z background.
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WlepnuMT_50_100.jpg The transverse mass distribution MT in the single muon data control sample and predictions for W(μν), t ̄t, Z(μμ) and single-top production.
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WlepnuPT2_50_100.jpg The W transverse momentum distribution in the single muon data control sample and predictions for W(μν), t ̄t, Z(μμ) and single-top production.
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ADD_2012_LimitComparison.jpg Comparison of lower limits on MD versus the number of extra dimensions with LEP, CDF, and D0.
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Lambda_SpinIndependent.jpg Limits on the contact interaction scale Λ as a function of the DM mass for the the spin independent model of the current analysis using 19.5 fb−1 of 8 TeV data. Also shown is the result from the previous analysis using 5 fb−1 of 7 TeV data.
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Lambda_SpinDependent.jpg Limits on the contact interaction scale Λ as a function of the DM mass for the the spin dependent model of the current analysis using 19.5 fb−1 of 8 TeV data. Also shown is the result from the previous analysis using 5 fb−1 of 7 TeV data.
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SpinDependent_woScalar.jpg dm_limit_si_v2.jpg Comparison of CMS MonoJet 90% CL upper limits on the nucleon cross section versus dark matter mass for the spin independent model with CDF, XENON100, CoGeNT and CDMSII. (left) The original figure from the PAS. (right) An alternative figure used in CERN COURIER, May 22, 2013. For this plot, 68% and 90% contours are included for the candidate events from CDMS (arXiv:1304.4279 [hep-ex]).
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SpinDependent_Scalar.jpg CMS MonoJet 90% CL upper limit on the nucleon cross section versus dark matter mass for the scalar operator model.
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SpinDependent.jpg dm_limit_sd_v2.jpg Comparison of CMS MonoJet 90% CL upper limits on the nucleon cross section versus dark matter mass for the spin dependent model with CDF, SIMPLE, CDMSII, COUPP, Super-K, and IceCube. At left, the original figure from the PAS. On the right, an alternative figure used in CERN COURIER, May 22, 2013, which include the 68% and 90% contours for the candidate events from CDMS (arXiv:1304.4279 [hep-ex]).
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SpinDependent_shade.jpg Observed limits on Λ as a function of the mass of the mediator (M), assuming vector interactions and a dark matter mass of 50 GeV (blue) and 500 GeV (red). The width of the mediator was varied between M/3, M/10 and M/8Pi.
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LimitComparison_Unparticle_Spin0_19fb.jpg 95% CL upper limits on the unparticle production rate in pb compared to limits from previous CMS analyses.
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Supplementary Plots from EXO-12-048

 
Figure Caption
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Jet2Pt.jpg Transverse momentum distribution of the second leading pT jet . The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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Jet2Eta.jpg Pseudorapidity distribution of the second leading pT jet . The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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dPhi_Jet1_Jet2_Cut.jpg The ∆φ(j1, j2) distribution. The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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NJet.jpg Jet multiplicity distribution. The figure is shown with all analysis cuts applied. Cuts include pT(j1) > 110GeV/c, pT(j2)>30GeV/c, abs(η(j1)) < 2.4, NJets ≤ 2 and ∆φ(j1, j2) < 2.5.
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ADD_2012_LimitComparison_2.jpg Comparison of lower limits on MD versus the number of extra dimensions with ATLAS, LEP, CDF, and D0.
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ADD_D3.jpg Observed and expected 95% CLs limits on ADD versus theoretical cross section and as a function of MD. Limits are shown on dimension δ=3.
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ModelIndependent_Plot.jpg The observed (solid lines) and expected (dashed lines) 95% CLs limits on σ × A × ε on the possible contributions from new physics passing the selection requirements for the different signal regions.
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Feynman diagrams for the pair production of DM particles for the case of a contact interaction (a) and the exchange of a mediator (b).
(a) Download PDF Download JPG
(b) Download PDF Download JPG
Feynman diagrams for the production of a graviton (G) or unparticles (U) in association with a jet.
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Missing transverse energy (MET) after all selections for data and SM backgrounds. The processes contributing to the SM background are from simulation, normalised to the estimation from data using the MET threshold of 500 GeV. The shaded bands in the lower panel represent the statistical uncertainty. Overflow events are included in the last bin.
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The model-independent observed and expected 95% CL upper limits on the visible cross section times acceptance times efficiency (σ × A × ε) for non-SM production of events. Shaded areas show the ±1σ and ±2σ bands on the expected limits.
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Upper limits on the DM-nucleon cross section, at 90% CL, plotted against DM particle mass and compared with previously published results. (a) limits for the vector and scalar operators from the previous CMS analysis, together with results from the CoGeNT, SIMPLE, COUPP, CDMS, SuperCDMS, XENON100, and LUX collaborations. The solid and hatched yellow contours show the 68% and 90% CL contours respectively for a possible signal from CDMS. (b): limits for the axial-vector operator from the previous CMS analysis, together with results from the SIMPLE, COUPP, Super-K, and IceCube collaborations.
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Download PDF Download JPG
SpinDependent_shade.jpg Observed limits on the mediator mass divided by coupling, M/√gχgq, as a function of the mass of the mediator, M, assuming vector interactions and a dark matter mass of 50 GeV (blue, filled) and 500 GeV (red, hatched). The width, Γ, of the mediator is varied between M/3 and M/8π. The dashed lines show contours of constant coupling √gχgq.
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ADD_2012_LimitComparison.jpg Lower limits at 95% CL on MD plotted against the number of extra dimensions δ, with results from the ATLAS, CMS, LEP, CDF, and DŲ collaborations.
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LimitComparison_Unparticle_Spin0_19fb.jpg The expected and observed lower limits on the unparticle model parameters ΛU as a function of dU at 95% CL, compared to previous result. The shaded region indicates the side of the curve that is excluded.
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Event Displays from EXO-12-048

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Event displays from EXO-12-048

 (click on the event display to get PNG)
Event Details ρφ View ρZ View 3D View
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Run 204553

Event 36479045

W(mu+nu) + jets candidate event. The W(mu+nu) + jets events are used to predict the remaining W+jets background in monojet analysis.

W_Rho-Phi.png W_Rho-Z.png W_3DTower_AllDet.png
Run 204564

Event 448966153

Z(mu+mu) + jets candidate event. The Z(mu+mu) + jets events are used to predict the invisible Z background in monojet analysis.

Z_Rho-Phi.png Z_Rho-Z.png Z_3DTower_AllDet.png
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Standard Model MC samples

Process x-sec (pb) Details
DY + Jets, Pt(Z) > 100 GeV/c, leptonic decays 34.1 Z(l,l)+0,1,2,3,4 jets, Jet Pt min = 10 GeV, Pt(l,l) > 100 GeV/c, MLM matching with qcut = 10 GeV, xqcut = 20 GeV, cteq6l1
W + Jets (leptonic W decays) 67812 W(LNu)+0,1,2,3,4 jets, Jet Pt min = 10 GeV/c, MLM matching with qcut = 10 GeV, xqcut = 20 GeV, cteq6l1
t-tbar 225.2 t+tbar+0,1,2,3 jets, pt(t) > 20 GeV/c, pt(b)>20 GeV/c, MLM matching with qcut = 20 GeV, xqcut = 20 GeV, cteq6l1
Single t, s-channel 2.82
Single t, t-channel 47.0
Single t, tW-channel 10.7
Single tbar, s-channel 1.57
Single tbar, t-channel 25.0
Single tbar, tW-channel 10.7
QCD (pT-hat bin 300 - 470 GeV/c) 1759.55 MSEL = 1 (QCD hight pT processes), CKIN(3) = 300, CKIN(4) = 470, pythia6 tune Z2star
QCD (pT-hat bin 470 - 600 GeV/c) 113.88 MSEL = 1 (QCD hight pT processes), CKIN(3) = 470, CKIN(4) = 600, pythia6 tune Z2star
QCD (pT-hat bin 600 - 800 GeV/c) 27.0 MSEL = 1 (QCD hight pT processes), CKIN(3) = 600, CKIN(4) = 800, pythia6 tune Z2star
QCD (pT-hat bin 800 - 1000 GeV/c) 3.6 MSEL = 1 (QCD hight pT processes), CKIN(3) = 800, CKIN(4) = 1000, pythia6 tune Z2star
QCD (pT-hat bin 1000 - 1400 GeV/c) 0.74 MSEL = 1 (QCD hight pT processes), CKIN(3) = 1000, CKIN(4) = 1400, pythia6 tune Z2star
QCD (pT-hat bin 1400 - 1800 GeV/c) 0.034 MSEL = 1 (QCD hight pT processes), CKIN(3) = 1400, CKIN(4) = 1800, pythia6 tune Z2star
QCD (pT-hat bin 1800+ GeV/c) 0.0018 MSEL = 1 (QCD hight pT processes), CKIN(3) = 1800, pythia6 tune Z2star
Z(nu,nu) + Jets (HT bin 50 - 100 GeV/c) 381.2 Z(Nu,Nu)+0,1,2,3,4 jets, Jet Pt min = 10 GeV/c, 50 < HT < 100, MLM matching with qcut = 10 GeV, xqcut = 15 GeV, cteq6l1
Z(nu,nu) + Jets (HT bin 100 - 200 GeV/c) 160.3 Z(Nu,Nu)+0,1,2,3,4 jets, Jet Pt min = 10 GeV/c, 100 < HT < 200, MLM matching with qcut = 10 GeV, xqcut = 15 GeV, cteq6l1
Z(nu,nu) + Jets (HT bin 200 - 400 GeV/c) 41.5 Z(Nu,Nu)+0,1,2,3,4 jets, Jet Pt min = 10 GeV/c, 200 < HT < 400, MLM matching with qcut = 10 GeV, xqcut = 15 GeV, cteq6l1
Z(nu,nu) + Jets (HT bin 400+ GeV/c) 5.3 Z(Nu,Nu)+0,1,2,3,4 jets, Jet Pt min = 10 GeV/c, 400 < HT, MLM matching with qcut = 10 GeV, xqcut = 15 GeV, cteq6l1

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