Difference: LHCHXSWGMSSMNeutral (1 vs. 130)

Revision 1302019-07-24 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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  Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.

Current recommendation for interpretation

Changed:
<
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  • Current BETA VERSION 2018 benchmark scenarios are recommended to be used for for interpretations.
  • ROOT file verion from 2016 is still the recommended for hMSSM
>
>
  • 2018 MSSM benchmark scenarios are recommended to be used for for interpretations.
  • ROOT file version from 2016 is still the recommended for hMSSM.
 

2018 Content of the ROOT files

Line: 105 to 105
 
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): Download the header file and the implementation file and the python wrapper. Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. Example calls can be found here.
Changed:
<
<
  • Access tool version 2.0 (for 8, 13 (and 14 TeV)): Download the header file and the implementation file and the python wrapper. Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. The ROOT files were generated with ROOT 6.13. Older ROOT versions might have problems in reading the content.
>
>
  • Access tool version 2.1 (for 8, 13 (and 14 TeV)): Download the header file and the implementation file and the python wrapper. Please remove the "v_2.1" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. The ROOT files were generated with ROOT 6.13. Older ROOT versions might have problems in reading the content.
  The routines are mostly identical to tool version 1.0 with the following exceptions: The 4FS/5FS/Santander matched cross sections for bottom-quark annihilation are replaced with SCET/FONLL numbers, which are accessed through bbH_A/H/h. Also charged Higgs cross sections are available now. For the naming conventions and the implemented uncertainties please check the routines that can be found in mssm_xs_tools.h.
Added:
>
>
From 2.0 to 2.1 the python wrapper was updated.
 
     root -l
     .L mssm_xs_tools.C++
Line: 122 to 123
  mssm.xsec("gg->H",300,3)
Changed:
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ROOT histograms: 2018 MSSM benchmark scenarios for 8, 13 (and 14 TeV) - Access tool version 2.0

>
>

ROOT histograms: 2018 MSSM benchmark scenarios for 8, 13 (and 14 TeV) - Access tool version 2.0/2.1

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios for Run 2 and Beyond"
Line: 467 to 468
 
META FILEATTACHMENT attachment="mh125_align_8.root" attr="" comment="" date="1552833378" name="mh125_align_8.root" path="mh125_align_8.root" size="45198661" user="sliebler" version="3"
META FILEATTACHMENT attachment="mh125_align_13.root" attr="" comment="" date="1552834003" name="mh125_align_13.root" path="mh125_align_13.root" size="45366612" user="sliebler" version="3"
META FILEATTACHMENT attachment="mh125_align_14.root" attr="" comment="" date="1552834620" name="mh125_align_14.root" path="mh125_align_14.root" size="44929855" user="sliebler" version="3"
Added:
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.C_v2.1" attr="" comment="" date="1563978392" name="mssm_xs_tools.C_v2.1" path="mssm_xs_tools.C_v2.1" size="6701" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v2.1" attr="" comment="" date="1563978392" name="mssm_xs_tools.h_v2.1" path="mssm_xs_tools.h_v2.1" size="27801" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v2.1" attr="" comment="" date="1563978392" name="mssm_xs_tools.py_v2.1" path="mssm_xs_tools.py_v2.1" size="4339" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1292019-07-17 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 105 to 105
 
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): Download the header file and the implementation file and the python wrapper. Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. Example calls can be found here.
Changed:
<
<
>
>
  Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. The ROOT files were generated with ROOT 6.13. Older ROOT versions might have problems in reading the content. The routines are mostly identical to tool version 1.0 with the following exceptions: The 4FS/5FS/Santander matched cross sections for bottom-quark annihilation are replaced with SCET/FONLL numbers, which are accessed through bbH_A/H/h. Also charged Higgs cross sections are available now. For the naming conventions and the implemented uncertainties please check the routines that can be found in mssm_xs_tools.h.
Line: 132 to 132
 Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:
Changed:
<
<
BETA VERSION : Now updated to include Yb*Yt term in bbh XS.
>
>
January 2019: Updated to include Yb*Yt term in bbh XS.
No further changes to be expected. Only additional information will be added, like branching ratios of the heavy Higgs bosons into individual pairs of electroweakinos.
 
Changed:
<
<
  • BETA VERSION: $M_h^{125}$
>
>
  • $M_h^{125}$
 
Changed:
<
<
  • BETA VERSION: $M_h^{125}(\tilde \chi)$
>
>
  • $M_h^{125}(\tilde \chi)$
 
Changed:
<
<
  • BETA VERSION: $M_h^{125}(\tilde\tau)$
>
>
  • $M_h^{125}(\tilde\tau)$
 
Changed:
<
<
  • BETA VERSION: $M_h^{125}$(alignment)
>
>
  • $M_h^{125}$(alignment)
 
    • This scenario yields a SM-like Higgs boson h also for low values of mA at about tanβ=7 due to alignment. In contrast to the definition in arXiv:1808.07542 the ROOT files start only at mA > 120 GeV due to a theoretically inaccessible region at low mA < 120 GeV and tanβ>10.
    • mh125_align_8.root: 8 TeV, tanβ= 1-20, mA = 120-1000 GeV
    • mh125_align_13.root: 13 TeV, tanβ= 1-20, mA = 120-1000 GeV

Revision 1282019-07-10 - PietroSlavich

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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  If you use the ROOT files from 2018 and later provided on this webpage, you must cite a fraction of the subsequent technical papers.
Which papers need to be cited depends on which cross sections and branching ratios your analysis is using, see the citation guide right after the list of bibliography. If you are in doubt, ask the group members!
Changed:
<
<
Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.
>
>
Also don't forget to cite the publications that suggested the benchmark scenarios. Those are listed next to the ROOT files.
 Relevant publications:
  1. FeynHiggs program
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria, Bahl:2016brp, Bahl:2017aev

Revision 1272019-07-08 - PietroSlavich

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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Group Members

Changed:
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In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
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<
>
>
 

Bibliography

Line: 126 to 126
  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios for Run 2 and Beyond"
Changed:
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<
Henning Bahl, Elina Fuchs, Thomas Hahn, Sven Heinemeyer, Stefan Liebler, Shruti Patel, Pietro Slavich, Tim Stefaniak, Carlos E.M. Wagner, Georg Weiglein
>
>
Emanuele Bagnaschi, Henning Bahl, Elina Fuchs, Thomas Hahn, Sven Heinemeyer, Stefan Liebler, Shruti Patel, Pietro Slavich, Tim Stefaniak, Carlos E.M. Wagner, Georg Weiglein
 arXiv:1808.07542

Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.

Revision 1262019-05-23 - GuillermoHamity

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 75 to 74
  Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.
Added:
>
>

Current recommendation for interpretation

  • Current BETA VERSION 2018 benchmark scenarios are recommended to be used for for interpretations.
  • ROOT file verion from 2016 is still the recommended for hMSSM
 

2018 Content of the ROOT files

Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:

Revision 1252019-03-17 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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META FILEATTACHMENT attachment="mh125_14.root" attr="" comment="" date="1546950496" name="mh125_14.root" path="mh125_14.root" size="48835648" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_14.root" attr="" comment="" date="1546950497" name="mh125_lc_14.root" path="mh125_lc_14.root" size="49895193" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_ls_14.root" attr="" comment="" date="1546950498" name="mh125_ls_14.root" path="mh125_ls_14.root" size="49664464" user="sliebler" version="1"
Changed:
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META FILEATTACHMENT attachment="mh125_align_8.root" attr="" comment="" date="1550831886" name="mh125_align_8.root" path="mh125_align_8.root" size="45242075" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_align_13.root" attr="" comment="" date="1550831887" name="mh125_align_13.root" path="mh125_align_13.root" size="45411091" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_align_14.root" attr="" comment="" date="1550831888" name="mh125_align_14.root" path="mh125_align_14.root" size="44990329" user="sliebler" version="2"
>
>
META FILEATTACHMENT attachment="mh125_align_8.root" attr="" comment="" date="1552833378" name="mh125_align_8.root" path="mh125_align_8.root" size="45198661" user="sliebler" version="3"
META FILEATTACHMENT attachment="mh125_align_13.root" attr="" comment="" date="1552834003" name="mh125_align_13.root" path="mh125_align_13.root" size="45366612" user="sliebler" version="3"
META FILEATTACHMENT attachment="mh125_align_14.root" attr="" comment="" date="1552834620" name="mh125_align_14.root" path="mh125_align_14.root" size="44929855" user="sliebler" version="3"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1242019-02-22 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 146 to 146
 
Changed:
<
<
  • BETA VERSION (SOON 20.02.19): $M_h^{125}$(alignment)
    • This scenario yields a SM-like Higgs boson h also for low values of mA at about tanβ=7 due to alignment. Note that the region at very low mA<120GeV and larger tanβ>10 is theoretically not accessible. Some entries in the ROOT files might not be resonable in this region.
    • mh125_align_8.root: 8 TeV, tanβ= 1-20, mA = 100-1000 GeV
    • mh125_align_13.root: 13 TeV, tanβ= 1-20, mA = 100-1000 GeV
    • mh125_align_14.root: 14 TeV, tanβ= 1-20, mA = 100-1000 GeV
>
>
  • BETA VERSION: $M_h^{125}$(alignment)
    • This scenario yields a SM-like Higgs boson h also for low values of mA at about tanβ=7 due to alignment. In contrast to the definition in arXiv:1808.07542 the ROOT files start only at mA > 120 GeV due to a theoretically inaccessible region at low mA < 120 GeV and tanβ>10.
    • mh125_align_8.root: 8 TeV, tanβ= 1-20, mA = 120-1000 GeV
    • mh125_align_13.root: 13 TeV, tanβ= 1-20, mA = 120-1000 GeV
    • mh125_align_14.root: 14 TeV, tanβ= 1-20, mA = 120-1000 GeV
  Charged Higgs cross sections have a limited range in the charged Higgs boson masses, see above. Scenarios named in orange are obtained with the setup that will be described in a public note of the LHCHXSWG. The setup equals mostly the one presented in arXiv:1808.07542.
Line: 460 to 460
 
META FILEATTACHMENT attachment="mh125_14.root" attr="" comment="" date="1546950496" name="mh125_14.root" path="mh125_14.root" size="48835648" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_14.root" attr="" comment="" date="1546950497" name="mh125_lc_14.root" path="mh125_lc_14.root" size="49895193" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_ls_14.root" attr="" comment="" date="1546950498" name="mh125_ls_14.root" path="mh125_ls_14.root" size="49664464" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="mh125_align_8.root" attr="" comment="" date="1550831886" name="mh125_align_8.root" path="mh125_align_8.root" size="45242075" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_align_13.root" attr="" comment="" date="1550831887" name="mh125_align_13.root" path="mh125_align_13.root" size="45411091" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_align_14.root" attr="" comment="" date="1550831888" name="mh125_align_14.root" path="mh125_align_14.root" size="44990329" user="sliebler" version="2"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1232019-02-20 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 146 to 146
 
Changed:
<
<
  • BETA VERSION: $M_h^{125}$(alignment)
>
>
  • BETA VERSION (SOON 20.02.19): $M_h^{125}$(alignment)
 
    • This scenario yields a SM-like Higgs boson h also for low values of mA at about tanβ=7 due to alignment. Note that the region at very low mA<120GeV and larger tanβ>10 is theoretically not accessible. Some entries in the ROOT files might not be resonable in this region.
    • mh125_align_8.root: 8 TeV, tanβ= 1-20, mA = 100-1000 GeV
    • mh125_align_13.root: 13 TeV, tanβ= 1-20, mA = 100-1000 GeV

Revision 1222019-02-20 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 146 to 146
 
Added:
>
>
  • BETA VERSION: $M_h^{125}$(alignment)
    • This scenario yields a SM-like Higgs boson h also for low values of mA at about tanβ=7 due to alignment. Note that the region at very low mA<120GeV and larger tanβ>10 is theoretically not accessible. Some entries in the ROOT files might not be resonable in this region.
    • mh125_align_8.root: 8 TeV, tanβ= 1-20, mA = 100-1000 GeV
    • mh125_align_13.root: 13 TeV, tanβ= 1-20, mA = 100-1000 GeV
    • mh125_align_14.root: 14 TeV, tanβ= 1-20, mA = 100-1000 GeV

Charged Higgs cross sections have a limited range in the charged Higgs boson masses, see above.

 Scenarios named in orange are obtained with the setup that will be described in a public note of the LHCHXSWG. The setup equals mostly the one presented in arXiv:1808.07542.

ROOT histograms: 2013-2016 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Revision 1212019-01-08 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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  • BETA VERSION: $M_h^{125}$
Added:
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>
 
Added:
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Added:
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  Scenarios named in orange are obtained with the setup that will be described in a public note of the LHCHXSWG. The setup equals mostly the one presented in arXiv:1808.07542.
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META FILEATTACHMENT attachment="citationguide2013-16.txt" attr="" comment="" date="1544432006" name="citationguide2013-16.txt" path="citationguide2013-16.txt" size="2524" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_ls_8.root" attr="" comment="" date="1544606278" name="mh125_ls_8.root" path="mh125_ls_8.root" size="50109033" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_ls_13.root" attr="" comment="" date="1544606280" name="mh125_ls_13.root" path="mh125_ls_13.root" size="50629010" user="sliebler" version="1"
Added:
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META FILEATTACHMENT attachment="mh125_14.root" attr="" comment="" date="1546950496" name="mh125_14.root" path="mh125_14.root" size="48835648" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_14.root" attr="" comment="" date="1546950497" name="mh125_lc_14.root" path="mh125_lc_14.root" size="49895193" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_ls_14.root" attr="" comment="" date="1546950498" name="mh125_ls_14.root" path="mh125_ls_14.root" size="49664464" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1202019-01-08 - StefanLiebler

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META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 103 to 103
  Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. Example calls can be found here.

Changed:
<
<
Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
>
>
Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. The ROOT files were generated with ROOT 6.13. Older ROOT versions might have problems in reading the content.
  The routines are mostly identical to tool version 1.0 with the following exceptions: The 4FS/5FS/Santander matched cross sections for bottom-quark annihilation are replaced with SCET/FONLL numbers, which are accessed through bbH_A/H/h. Also charged Higgs cross sections are available now. For the naming conventions and the implemented uncertainties please check the routines that can be found in mssm_xs_tools.h.

Revision 1192018-12-17 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 70 to 70
  * Cross sections for bottom-quark initiated Higgs production rely on matched predictions [13], which are based on the five flavour NNLO QCD calculation [11] and the four flavour NLO QCD calculation [12].
Changed:
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* Charged Higgs cross sections for charged Higgs masses in the window 145-2000GeV are determined from the predictions provided in Refs. [14] by applying the reweighting procedure explained on
>
>
* Charged Higgs cross sections for charged Higgs masses in the window 200-1400GeV at 8TeV, 145-2000GeV at 13TeV and 200-600GeV at 14TeV are determined from the predictions provided in Refs. [14] by applying the reweighting procedure explained on
 the webpage of the charged Higgs subgroup.

Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.

Line: 82 to 82
 
  • masses and widths of the scalar bosons h/H/A/Hp.
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
  • cross sections for b-associated h/H/A production in the SCET/FONLL scheme including uncertainties.
Changed:
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<
  • cross sections for charged Higgs production including uncertainties (for 13TeV includes the window of charged Higgs masses between 145-200GeV).
>
>
  • cross sections for charged Higgs production including uncertainties (charged Higgs masses between 200-1400GeV at 8TeV, 145-2000GeV at 13TeV and 200-600GeV at 14TeV).
 
  • branching ratios of h/H/A/Hp to various SM and SUSY particles, see also BR subgroup.

The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.

Revision 1182018-12-12 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 131 to 131
  BETA VERSION : Now updated to include Yb*Yt term in bbh XS.
Changed:
<
<
  • BETA VERSION: m_h^125
>
>
  • BETA VERSION: $M_h^{125}$
 
Changed:
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  • BETA VERSION: m_h^125(chi)
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>
  • BETA VERSION: $M_h^{125}(\tilde \chi)$
 
Changed:
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  • BETA VERSION: m_h^125(stau)
>
>
  • BETA VERSION: $M_h^{125}(\tilde\tau)$
 

Revision 1172018-12-12 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 129 to 129
 Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:
Changed:
<
<
BETA VERSION : Small changes in bbH XS expected due to inclusion of Yb*Yt term.
>
>
BETA VERSION : Now updated to include Yb*Yt term in bbh XS.
 
  • BETA VERSION: m_h^125
Line: 139 to 139
 
Added:
>
>
 Scenarios named in orange are obtained with the setup that will be described in a public note of the LHCHXSWG. The setup equals mostly the one presented in arXiv:1808.07542.

ROOT histograms: 2013-2016 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

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META FILEATTACHMENT attachment="choiceofinputparameters.txt" attr="" comment="" date="1544200792" name="choiceofinputparameters.txt" path="choiceofinputparameters.txt" size="2120" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.C_v2.0" attr="" comment="" date="1544201197" name="mssm_xs_tools.C_v2.0" path="mssm_xs_tools.C_v2.0" size="6701" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v2.0" attr="" comment="" date="1544201197" name="mssm_xs_tools.h_v2.0" path="mssm_xs_tools.h_v2.0" size="28124" user="sliebler" version="1"
Changed:
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META FILEATTACHMENT attachment="mh125_8.root" attr="" comment="" date="1544201333" name="mh125_8.root" path="mh125_8.root" size="49545606" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544201333" name="mh125_13.root" path="mh125_13.root" size="50058293" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_8.root" attr="" comment="" date="1544276809" name="mh125_lc_8.root" path="mh125_lc_8.root" size="50331009" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_13.root" attr="" comment="" date="1544277524" name="mh125_lc_13.root" path="mh125_lc_13.root" size="50857063" user="sliebler" version="1"
>
>
META FILEATTACHMENT attachment="mh125_8.root" attr="" comment="" date="1544606169" name="mh125_8.root" path="mh125_8.root" size="49278500" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544606201" name="mh125_13.root" path="mh125_13.root" size="49793843" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_lc_8.root" attr="" comment="" date="1544606228" name="mh125_lc_8.root" path="mh125_lc_8.root" size="50330653" user="sliebler" version="2"
META FILEATTACHMENT attachment="mh125_lc_13.root" attr="" comment="" date="1544606256" name="mh125_lc_13.root" path="mh125_lc_13.root" size="50855759" user="sliebler" version="2"
 
META FILEATTACHMENT attachment="citationguide2013-16.txt" attr="" comment="" date="1544432006" name="citationguide2013-16.txt" path="citationguide2013-16.txt" size="2524" user="sliebler" version="2"
Added:
>
>
META FILEATTACHMENT attachment="mh125_ls_8.root" attr="" comment="" date="1544606278" name="mh125_ls_8.root" path="mh125_ls_8.root" size="50109033" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_ls_13.root" attr="" comment="" date="1544606280" name="mh125_ls_13.root" path="mh125_ls_13.root" size="50629010" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1162018-12-11 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 57 to 57
 In the first place, please cite the LHC Higgs cross-section working group for providing cross-sections and BRs (by citing the Yellow Reports).

For all except the hMSSM, Higgs masses and mixing (and effective Yukawa couplings) have been calculated with Feynhiggs [1].

Changed:
<
<
Whereas in the hMSSM branching ratios are solely computed with HDECAY [2], all other scenarios combine the most precise results of FeynHiggs [1], HDECAY [2] and PROPHECY4f. Relevant references are listed in [3], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.
>
>
Whereas in the hMSSM branching ratios are solely computed with HDECAY [2], all other scenarios combine the most precise results of FeynHiggs [1], HDECAY [2] and PROPHECY4f. Relevant references are listed in [3], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.
  If your analysis makes use of gluon-fusion cross sections, bottom-quark initiated production or charged Higgs production, then please cite the corresponding block of references as follows:
Line: 138 to 139
 
Changed:
<
<
Scenarios named in orange are obtained with the setup described in xxx.
>
>
Scenarios named in orange are obtained with the setup that will be described in a public note of the LHCHXSWG. The setup equals mostly the one presented in arXiv:1808.07542.
 

ROOT histograms: 2013-2016 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Revision 1152018-12-10 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 23 to 23
 
  1. FeynHiggs program
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria, Bahl:2016brp, Bahl:2017aev
  2. HDECAY
Changed:
<
<
    • Djouadi:1997yw, Djouadi:2006bz
>
>
    • Djouadi:1997yw, Djouadi:2018xqq
 
  1. Work of the BR subgroup, which is based upon the publications given in this tex-file.
  2. SusHi program
    • Harlander:2012pb, Harlander:2016hcx
Line: 35 to 35
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
Deleted:
<
<
  1. ggH@NNLO program
    • Harlander:2002wh
 
  1. ggH NNLO for scalar Higgs
Changed:
<
<
    • Anastasiou:2002yz, Ravindran:2003um
>
>
    • Harlander:2002wh, Anastasiou:2002yz, Ravindran:2003um
 
  1. ggH NNLO for pseudoscalar Higgs
    • Harlander:2002vv, Anastasiou:2002wq
  2. ggH N3LO for scalar Higgs in threshold expansion
Line: 63 to 61
  If your analysis makes use of gluon-fusion cross sections, bottom-quark initiated production or charged Higgs production, then please cite the corresponding block of references as follows:
Changed:
<
<
* For the gluon-fusion process inclusive cross sections are obtained with SusHi [3], which includes NLO QCD corrections [5], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [7,8,9] and electroweak effects by light quarks [11].
>
>
* For the gluon-fusion process inclusive cross sections are obtained with SusHi [3], which includes NLO QCD corrections [5], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [7,8] and electroweak effects by light quarks [10].
 For all scenarios but the hMSSM and the EFT scenarios please add:
SusHi includes NLO supersymmetric-QCD corrections [6] in expansions of heavy SUSY masses.
If you make use of the cross sections of the SM-like Higgs boson at 125 GeV please add:
Changed:
<
<
For the SM-like Higgs boson SusHi adds N3LO corrections in the effective theory of a heavy top quark in a threshold expansion [10].
>
>
For the SM-like Higgs boson SusHi adds N3LO corrections in the effective theory of a heavy top quark in a threshold expansion [9].
 
Changed:
<
<
* Cross sections for bottom-quark initiated Higgs production rely on matched predictions [14], which are based on the five flavour NNLO QCD calculation [12] and the four flavour NLO QCD calculation [13].
>
>
* Cross sections for bottom-quark initiated Higgs production rely on matched predictions [13], which are based on the five flavour NNLO QCD calculation [11] and the four flavour NLO QCD calculation [12].
 
Changed:
<
<
* Charged Higgs cross sections for charged Higgs masses in the window 145-2000GeV are determined from the predictions provided in Refs. [15] by applying the reweighting procedure explained on
>
>
* Charged Higgs cross sections for charged Higgs masses in the window 145-2000GeV are determined from the predictions provided in Refs. [14] by applying the reweighting procedure explained on
 the webpage of the charged Higgs subgroup.

Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.

Revision 1142018-12-10 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 130 to 130
 Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:
Added:
>
>
BETA VERSION : Small changes in bbH XS expected due to inclusion of Yb*Yt term.
 
  • BETA VERSION: m_h^125

Revision 1132018-12-10 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 16 to 16
  If you use the ROOT files from 2016 and earlier provided on this webpage, please follow the citation guide shifted to this file.
If you use the ROOT files from 2018 and later provided on this webpage, you must cite a fraction of the subsequent technical papers.
Changed:
<
<
Which papers need to be cited depends on which cross sections and branching ratios your analysis is using, see the description after the subsequent list.
>
>
Which papers need to be cited depends on which cross sections and branching ratios your analysis is using, see the citation guide right after the list of bibliography.
 If you are in doubt, ask the group members!
Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.
Relevant publications:
Deleted:
<
<
  1. HIGLU program
    • Spira:1995mt
  2. SusHi program
    • Harlander:2012pb, Harlander:2016hcx
 
  1. FeynHiggs program
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria, Bahl:2016brp, Bahl:2017aev
Changed:
<
<
  1. ggH@NNLO program
    • Harlander:2002wh
  2. bbh@nnlo (5FS) program
    • Harlander:2003ai
  3. bbH NLO (4FS)
    • Dittmaier:2003ej, Dawson:2003kb
  4. bbH matched predictions
    • Bonvini:2015pxa, Bonvini:2016fgf, Forte:2015hba, Forte:2016sja
>
>
  1. HDECAY
    • Djouadi:1997yw, Djouadi:2006bz
  2. Work of the BR subgroup, which is based upon the publications given in this tex-file.
  3. SusHi program
    • Harlander:2012pb, Harlander:2016hcx
 
  1. ggH NLO massive
    • Spira:1995rr
Deleted:
<
<
  1. ggH NNLO for scalar Higgs
    • Anastasiou:2002yz, Ravindran:2003um
  2. ggH N3LO for scalar Higgs in threshold expansion
    • Anastasiou:2014lda, Anastasiou:2015yha, Anastasiou:2016cez
  3. ggH NNLO for pseudoscalar Higgs
    • Harlander:2002vv, Anastasiou:2002wq
  4. Electroweak corrections by light fermions
    • Aglietti:2004nj, Bonciani:2010ms
 
  1. (N)NLO (S)QCD corrections for h/H/A
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
Added:
>
>
  1. ggH@NNLO program
    • Harlander:2002wh
  2. ggH NNLO for scalar Higgs
    • Anastasiou:2002yz, Ravindran:2003um
  3. ggH NNLO for pseudoscalar Higgs
    • Harlander:2002vv, Anastasiou:2002wq
  4. ggH N3LO for scalar Higgs in threshold expansion
    • Anastasiou:2014lda, Anastasiou:2015yha, Anastasiou:2016cez
  5. Electroweak corrections by light fermions
    • Aglietti:2004nj, Bonciani:2010ms
  6. bbh@nnlo (5FS) program
    • Harlander:2003ai
  7. bbH NLO (4FS)
    • Dittmaier:2003ej, Dawson:2003kb
  8. bbH matched predictions
    • Bonvini:2015pxa, Bonvini:2016fgf, Forte:2015hba, Forte:2016sja
 
  1. Charged Higgs cross sections
    • Berger:2003sm, Dittmaier:2009np, Flechl:2014wfa, Degrande:2015vpa, Degrande:2016hyf
Deleted:
<
<
  1. HDECAY
    • Djouadi:1997yw, Djouadi:2006bz
  2. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
 
Changed:
<
<
Example usage of references in public document:
>
>

Citation guide

In the first place, please cite the LHC Higgs cross-section working group for providing cross-sections and BRs (by citing the Yellow Reports).

For all except the hMSSM, Higgs masses and mixing (and effective Yukawa couplings) have been calculated with Feynhiggs [1]. Whereas in the hMSSM branching ratios are solely computed with HDECAY [2], all other scenarios combine the most precise results of FeynHiggs [1], HDECAY [2] and PROPHECY4f. Relevant references are listed in [3], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.

If your analysis makes use of gluon-fusion cross sections, bottom-quark initiated production or charged Higgs production, then please cite the corresponding block of references as follows:

* For the gluon-fusion process inclusive cross sections are obtained with SusHi [3], which includes NLO QCD corrections [5], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [7,8,9] and electroweak effects by light quarks [11].
For all scenarios but the hMSSM and the EFT scenarios please add:
SusHi includes NLO supersymmetric-QCD corrections [6] in expansions of heavy SUSY masses.
If you make use of the cross sections of the SM-like Higgs boson at 125 GeV please add:
For the SM-like Higgs boson SusHi adds N3LO corrections in the effective theory of a heavy top quark in a threshold expansion [10].

* Cross sections for bottom-quark initiated Higgs production rely on matched predictions [14], which are based on the five flavour NNLO QCD calculation [12] and the four flavour NLO QCD calculation [13].

* Charged Higgs cross sections for charged Higgs masses in the window 145-2000GeV are determined from the predictions provided in Refs. [15] by applying the reweighting procedure explained on the webpage of the charged Higgs subgroup.

 
Changed:
<
<
to be updated
>
>
Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.
 

2018 Content of the ROOT files

Line: 423 to 439
 
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544201333" name="mh125_13.root" path="mh125_13.root" size="50058293" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_8.root" attr="" comment="" date="1544276809" name="mh125_lc_8.root" path="mh125_lc_8.root" size="50331009" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_13.root" attr="" comment="" date="1544277524" name="mh125_lc_13.root" path="mh125_lc_13.root" size="50857063" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="citationguide2013-16.txt" attr="" comment="" date="1544391069" name="citationguide2013-16.txt" path="citationguide2013-16.txt" size="2504" user="sliebler" version="1"
>
>
META FILEATTACHMENT attachment="citationguide2013-16.txt" attr="" comment="" date="1544432006" name="citationguide2013-16.txt" path="citationguide2013-16.txt" size="2524" user="sliebler" version="2"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1122018-12-09 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 14 to 14
 

Bibliography

Changed:
<
<
OUTDATED If you use numbers provided on this webpage you must cite the following papers:
>
>
If you use the ROOT files from 2016 and earlier provided on this webpage, please follow the citation guide shifted to this file.
If you use the ROOT files from 2018 and later provided on this webpage, you must cite a fraction of the subsequent technical papers.
Which papers need to be cited depends on which cross sections and branching ratios your analysis is using, see the description after the subsequent list. If you are in doubt, ask the group members!
Also don't forget to cite the publications, which suggested the benchmark scenarios. Those are listed next to the ROOT files.
Relevant publications:
 
  1. HIGLU program
    • Spira:1995mt
  2. SusHi program
Changed:
<
<
    • Harlander:2012pb
>
>
    • Harlander:2012pb, Harlander:2016hcx
 
  1. FeynHiggs program
Changed:
<
<
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria
>
>
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria, Bahl:2016brp, Bahl:2017aev
 
  1. ggH@NNLO program
    • Harlander:2002wh
  2. bbh@nnlo (5FS) program
    • Harlander:2003ai
  3. bbH NLO (4FS)
    • Dittmaier:2003ej, Dawson:2003kb
Added:
>
>
  1. bbH matched predictions
    • Bonvini:2015pxa, Bonvini:2016fgf, Forte:2015hba, Forte:2016sja
 
  1. ggH NLO massive
    • Spira:1995rr
  2. ggH NNLO for scalar Higgs
    • Anastasiou:2002yz, Ravindran:2003um
Added:
>
>
  1. ggH N3LO for scalar Higgs in threshold expansion
    • Anastasiou:2014lda, Anastasiou:2015yha, Anastasiou:2016cez
 
  1. ggH NNLO for pseudoscalar Higgs
    • Harlander:2002vv, Anastasiou:2002wq
  2. Electroweak corrections by light fermions
Line: 41 to 50
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
Added:
>
>
  1. Charged Higgs cross sections
    • Berger:2003sm, Dittmaier:2009np, Flechl:2014wfa, Degrande:2015vpa, Degrande:2016hyf
 
  1. HDECAY
    • Djouadi:1997yw, Djouadi:2006bz
  2. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.

Example usage of references in public document:

Changed:
<
<
In the first place, please cite the LHC Higgs cross-section working group for providing cross-sections and BRs (by citing the Yellow Reports).

For all except the hMSSM, Higgs masses and mixing (and effective Yukawa couplings) have been calculated with Feynhiggs [3].

Cross sections:

  • For the gluon-fusion process inclusive cross sections are obtained with SusHi [2], which includes NLO supersymmetric-QCD corrections [7,11], N^3LO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9,tbc] and electroweak effects by light quarks [10]. (HIGLU [1] is used for "classic" mhmax scenario - see details below.)

  • For the bbH process we now use the SCET/FONLL scheme provided by the bbh subgroup. Outdated cross sections are the five flavour NNLO QCD inclusive cross sections calculated with SusHi [2] based on bbh@nnlo [5] and the four flavour NLO QCD calculation [6].

Branching ratios:

Whereas in the hMSSM branching ratios are solely computed with HDECAY [12], all other scenarios combine the most precise results of HDECAY [12], FeynHiggs [3] and PROPHECY4f. Relevant references are listed in [13], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.

>
>
to be updated
 

2018 Content of the ROOT files

Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:

  • masses and widths of the scalar bosons h/H/A/Hp.
Changed:
<
<
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
>
>
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
 
  • cross sections for b-associated h/H/A production in the SCET/FONLL scheme including uncertainties.
  • cross sections for charged Higgs production including uncertainties (for 13TeV includes the window of charged Higgs masses between 145-200GeV).
Changed:
<
<
  • branching ratios of h/H/A/Hp to various SM and SUSY particles, see also BR subgroup.
>
>
  • branching ratios of h/H/A/Hp to various SM and SUSY particles, see also BR subgroup.
  The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.
Line: 425 to 423
 
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544201333" name="mh125_13.root" path="mh125_13.root" size="50058293" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_8.root" attr="" comment="" date="1544276809" name="mh125_lc_8.root" path="mh125_lc_8.root" size="50331009" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_13.root" attr="" comment="" date="1544277524" name="mh125_lc_13.root" path="mh125_lc_13.root" size="50857063" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="citationguide2013-16.txt" attr="" comment="" date="1544391069" name="citationguide2013-16.txt" path="citationguide2013-16.txt" size="2504" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1112018-12-08 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 116 to 116
 Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:
Changed:
<
<
  • BETA VERSION: mh125
>
>
  • BETA VERSION: m_h^125
 
Added:
>
>
 Scenarios named in orange are obtained with the setup described in xxx.

ROOT histograms: 2013-2016 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Line: 419 to 423
 
META FILEATTACHMENT attachment="mssm_xs_tools.h_v2.0" attr="" comment="" date="1544201197" name="mssm_xs_tools.h_v2.0" path="mssm_xs_tools.h_v2.0" size="28124" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_8.root" attr="" comment="" date="1544201333" name="mh125_8.root" path="mh125_8.root" size="49545606" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544201333" name="mh125_13.root" path="mh125_13.root" size="50058293" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="mh125_lc_8.root" attr="" comment="" date="1544276809" name="mh125_lc_8.root" path="mh125_lc_8.root" size="50331009" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_lc_13.root" attr="" comment="" date="1544277524" name="mh125_lc_13.root" path="mh125_lc_13.root" size="50857063" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1102018-12-07 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 62 to 62
 Whereas in the hMSSM branching ratios are solely computed with HDECAY [12], all other scenarios combine the most precise results of HDECAY [12], FeynHiggs [3] and PROPHECY4f. Relevant references are listed in [13], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.
Changed:
<
<

Available benchmark scenarios

>
>

2018 Content of the ROOT files

  Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:
Line: 122 to 122
  Scenarios named in orange are obtained with the setup described in xxx.
Changed:
<
<

ROOT histograms: 2013-2015 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

>
>

ROOT histograms: 2013-2016 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the

Revision 1092018-12-07 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 14 to 14
 

Bibliography

Changed:
<
<
If you use numbers provided on this webpage you must cite the following papers:
>
>
OUTDATED If you use numbers provided on this webpage you must cite the following papers:
 
  1. HIGLU program
    • Spira:1995mt
  2. SusHi program
Line: 66 to 66
  Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:
Changed:
<
<
  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
>
>
  • masses and widths of the scalar bosons h/H/A/Hp.
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
 
  • cross sections for b-associated h/H/A production in the SCET/FONLL scheme including uncertainties.
  • cross sections for charged Higgs production including uncertainties (for 13TeV includes the window of charged Higgs masses between 145-200GeV).
Changed:
<
<
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons, see also BR subgroup.
>
>
  • branching ratios of h/H/A/Hp to various SM and SUSY particles, see also BR subgroup.
  The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.
Line: 79 to 79
 For the benchmark scenarios released in 2018 we provide a new version of the access tool v2.0, which is not compatible with the old ROOT files. We keep the old access tool for compatibility.
Changed:
<
<
ALERT! Please note that for both access tools the cross section predictions (and uncertainties) are consistently provided in pb .
>
>
ALERT! Please note that for all access tools the cross section predictions (and uncertainties) are consistently provided in pb .
 
  • Access tool version 0.5 (for 7 and 8 TeV): Download the header file and the implementation file. For information about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.
Changed:
<
<
     root -l
     .L mssm_xs_tools.C++
     mssm_xs_tools test
     test.SetInput("out.mhmax_mu200_7_nnlo.tanBeta_gte1.root")
     test.help()
     test.Give_BR_A_tautau(120,30)
     test.Give_Xsec_ggFA(120,30)
     test.Give_XsecUnc_muup_ggFA(120,30)
     test.Give_XsecUnc_mudown_ggFA(120,30)
     test.Give_XsecUnc_pdfalphas68up_ggFA(120,30)
     test.Give_XsecUnc_pdfalphas68down_ggFA(120,30)
     ...
     
>
>
Example calls can be found here.
 
Changed:
<
<
Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
     root -l
     .L mssm_xs_tools.C++
     
Then either the python wrapper or the .C file could be used:
     mssm=mssm_xs_tools("hMSSM_8TeV.root",true,0)   // "true" enables interpolation between the grid points, "0" avoids messages by the access tool, set to "3" or "100" for additional information
     mssm.mass("H",300,3)   
     mssm.width("H",300,3)   
     mssm.br("H-­>tautau",300,3)   
     mssm.xsec("gg->H",300,3)   
     mssm.xsec("bb5F->H",300,3)   
     mssm.xsec("bb4F-­>H",300,3)   
     mssm.xsec("bbSantander->H",300,3)  
     mssm.xsec("gg->H::scaleUp",300,3)   
     mssm.xsec("gg->H::pdfasUp",300,3)   
     
>
>
Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled. Example calls can be found here.
 
Changed:
<
<
>
>
  Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
Added:
>
>
The routines are mostly identical to tool version 1.0 with the following exceptions: The 4FS/5FS/Santander matched cross sections for bottom-quark annihilation are replaced with SCET/FONLL numbers, which are accessed through bbH_A/H/h. Also charged Higgs cross sections are available now. For the naming conventions and the implemented uncertainties please check the routines that can be found in mssm_xs_tools.h.
 
     root -l
     .L mssm_xs_tools.C++
     
Then either the python wrapper or the .C file could be used:

Changed:
<
<
mssm=mssm_xs_tools("hMSSM_8TeV.root",true,0) // "true" enables interpolation between the grid points, "0" avoids messages by the access tool, set to "3" or "100" for additional information
>
>
mssm=mssm_xs_tools("mh125_13.root",true,0) // "true" enables interpolation between the grid points, "0" avoids messages by the access tool, set to "3" or "100" for additional information
  mssm.mass("H",300,3) mssm.width("H",300,3) mssm.br("H-­>tautau",300,3) mssm.xsec("gg->H",300,3)
Changed:
<
<

Discussion of MSSM scenarios with low tanβ and Heavy SUSY

Please check the dedicated twiki page here and the information provided in:

"Benchmark scenarios for low tanβ in the MSSM"
E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
LHCHXSWG-2015-002

ROOT histograms: MSSM benchmark scenarios for 8, 13 (and 14 TeV) - Access tool version 2.0

>
>

ROOT histograms: 2018 MSSM benchmark scenarios for 8, 13 (and 14 TeV) - Access tool version 2.0

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios for Run 2 and Beyond"
Line: 151 to 116
 Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:
Changed:
<
<
SOON AVAILABLE
>
>
  • BETA VERSION: mh125

Scenarios named in orange are obtained with the setup described in xxx.

 
Changed:
<
<

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

>
>

ROOT histograms: 2013-2015 MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the
Line: 217 to 186
 
Changed:
<
<

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

>
>

ROOT histograms: <2013 MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

  The scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=1 and 60. For lower values of tanβ between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
Line: 333 to 302
 
  • Bottom-quark annihilation (5FS) cross section: bbh@nnlo
  • Gluon fusion (incl. SQCD and EW) and bottom-quark annihilation (5FS) cross section: SusHi
Changed:
<
<

Meetings

>
>

Discussion of MSSM scenarios with low tanβ and Heavy SUSY

 
Changed:
<
<

Choice of input parameters

>
>
Please check the dedicated twiki page here and the information provided in:
 
Changed:
<
<
All SusHi runs make use of the naive Δ_b resummation (Y_b -> Y_b/(1+ Δ_b)) using the Δ_b from FeynHiggs for gluon fusion and the full resummation for bottom-quark annihilation (5FS) (see SusHi manual). They include NLO squark contributions expanded in heavy SUSY masses and electroweak corrections by light quarks.
>
>
"Benchmark scenarios for low tanβ in the MSSM"
E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
LHCHXSWG-2015-002
 
Changed:
<
<
HIGLU Standard Model parameters
α_S(MZ) 0.12018, 2 loop
Lambda_QCD^(5) 226 MeV
PDF MSTW2008nlo68cl
Mcharm 1.40 GeV
Mbottom 4.75 GeV
Mtop 172.5 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
MW 80.398 GeV

ggH@NNLO Standard Model parameters
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl
Mbottom (Mbottom) 4.213 GeV
Mtop 172.5 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
   
SusHi 1.0.6 Standard Model parameters
α_S(MZ) 0.119 / PDF value
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl
Mcharm 1.40 GeV
Mbottom 4.75 GeV
Mtop 172.5 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV

FeynHiggs 2.7.4 and 2.8.6 with default flags
Standard Model parameters
Mtop 172.5 GeV
mb(mb) MSbar 4.213 GeV
α_S(MZ) 0.119
   
SusHi 1.4.1 Standard Model parameters
α_S(MZ) 0.119 / PDF value
1/α_EW(MZ) 127.67 / fictitious value to obtain mW=80.398 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
mc(mc) MSbar 1.28 GeV
mb(mb) MSbar 4.16 GeV
Mbottom^pole 4.75 GeV
Mtop^pole 172.5 GeV
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl

FeynHiggs 2.10.2 with default flags
Standard Model parameters
α_S(MZ) 0.119
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
MW 80.398 GeV
mc(mc) MSbar 1.28 GeV
mb(mb) MSbar 4.16 GeV
Mtop^pole 172.5 GeV
>
>

Meetings

 

Outdated discussions (kept for the sake of completeness)

Changed:
<
<
Considerations on H->tautau (~2011)
>
>
Considerations on H->tautau (~2011)
Choice of input parameters (<2016)
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
Line: 498 to 413
 
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1464351602" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="7587152" user="sliebler" version="4"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1464351663" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="5932404" user="sliebler" version="4"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1464351681" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="5932470" user="sliebler" version="4"
Added:
>
>
META FILEATTACHMENT attachment="oldaccesstoolexamples.txt" attr="" comment="" date="1544200262" name="oldaccesstoolexamples.txt" path="oldaccesstoolexamples.txt" size="1197" user="sliebler" version="1"
META FILEATTACHMENT attachment="choiceofinputparameters.txt" attr="" comment="" date="1544200792" name="choiceofinputparameters.txt" path="choiceofinputparameters.txt" size="2120" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.C_v2.0" attr="" comment="" date="1544201197" name="mssm_xs_tools.C_v2.0" path="mssm_xs_tools.C_v2.0" size="6701" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v2.0" attr="" comment="" date="1544201197" name="mssm_xs_tools.h_v2.0" path="mssm_xs_tools.h_v2.0" size="28124" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_8.root" attr="" comment="" date="1544201333" name="mh125_8.root" path="mh125_8.root" size="49545606" user="sliebler" version="1"
META FILEATTACHMENT attachment="mh125_13.root" attr="" comment="" date="1544201333" name="mh125_13.root" path="mh125_13.root" size="50058293" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 1082018-12-07 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 10 to 10
 
Changed:
<
<
>
>
 

Bibliography

Line: 53 to 53
  Cross sections:
Changed:
<
<
  • For the gluon-fusion process inclusive cross sections are obtained with SusHi [2], which includes NLO supersymmetric-QCD corrections [7,11], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9] and electroweak effects by light quarks [10]. (HIGLU [1] is used for "classic" mhmax scenario - see details below.)
>
>
  • For the gluon-fusion process inclusive cross sections are obtained with SusHi [2], which includes NLO supersymmetric-QCD corrections [7,11], N^3LO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9,tbc] and electroweak effects by light quarks [10]. (HIGLU [1] is used for "classic" mhmax scenario - see details below.)
 
Changed:
<
<
  • For the bbH process
    • Five flavour NNLO QCD inclusive cross sections are calculated with SusHi [2] based on bbh@nnlo [5]. The results are combined with the
    • Four flavour NLO QCD calculation [6]
    • to Santander matched cross sections (reference in next section).
>
>
  • For the bbH process we now use the SCET/FONLL scheme provided by the bbh subgroup. Outdated cross sections are the five flavour NNLO QCD inclusive cross sections calculated with SusHi [2] based on bbh@nnlo [5] and the four flavour NLO QCD calculation [6].
  Branching ratios:
Line: 70 to 67
 Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:

  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
Changed:
<
<
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • cross sections for b-associated h/H/A production in the 4 flavour scheme (4FS) (NLO QCD) including scale uncertainties.
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
>
>
  • cross sections for b-associated h/H/A production in the SCET/FONLL scheme including uncertainties.
  • cross sections for charged Higgs production including uncertainties (for 13TeV includes the window of charged Higgs masses between 145-200GeV).
  • cross sections for gluon-gluon fusion h/H/A production (top at N^3LO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties.
 
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons, see also BR subgroup.
Deleted:
<
<
The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available:
"Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach"
R. Harlander, M. Krämer, and M. Schumacher
Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.

santandermatching-hks.pdf: Description of Santander matching procedure for inclusive pp-->H(bb) cross-section
 The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.

Access tool for the ROOT files

Changed:
<
<
For the 13 and 14 TeV runs we provide a new version of the access tool, which is not compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
>
>
For the benchmark scenarios released in 2018 we provide a new version of the access tool v2.0, which is not compatible with the old ROOT files. We keep the old access tool for compatibility.
  ALERT! Please note that for both access tools the cross section predictions (and uncertainties) are consistently provided in pb .
Line: 127 to 118
  mssm.xsec("gg->H::pdfasUp",300,3)
Added:
>
>
  • SOON AVAILABLE Access tool version 2.0 (for 8, 13 (and 14 TeV)): Download the header file and the implementation file and the python wrapper. Please remove the "v_2.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
         root -l
         .L mssm_xs_tools.C++
         
    Then either the python wrapper or the .C file could be used:
         mssm=mssm_xs_tools("hMSSM_8TeV.root",true,0)   // "true" enables interpolation between the grid points, "0" avoids messages by the access tool, set to "3" or "100" for additional information
         mssm.mass("H",300,3)   
         mssm.width("H",300,3)   
         mssm.br("H-­>tautau",300,3)   
         mssm.xsec("gg->H",300,3)   
         
 

Discussion of MSSM scenarios with low tanβ and Heavy SUSY

Please check the dedicated twiki page here and the information provided in:

Line: 135 to 141
 E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
LHCHXSWG-2015-002
Added:
>
>

ROOT histograms: MSSM benchmark scenarios for 8, 13 (and 14 TeV) - Access tool version 2.0

Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios for Run 2 and Beyond"
Henning Bahl, Elina Fuchs, Thomas Hahn, Sven Heinemeyer, Stefan Liebler, Shruti Patel, Pietro Slavich, Tim Stefaniak, Carlos E.M. Wagner, Georg Weiglein
arXiv:1808.07542

Most scans in the m_A-tanβ-plane have been made between m_A=70 GeV and m_A=2600 GeV and between tanβ=0.5 and 60.
ROOT histograms:

SOON AVAILABLE

 

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:

Revision 1072018-09-05 - GuillermoHamity

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Changed:
<
<
In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
<
<
>
>
 
Line: 17 to 17
  If you use numbers provided on this webpage you must cite the following papers:
  1. HIGLU program
    • Spira:1995mt
Changed:
<
<
  1. SusHi program
>
>
  1. SusHi program
 
    • Harlander:2012pb
Changed:
<
<
  1. FeynHiggs program
>
>
  1. FeynHiggs program
 
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria
Changed:
<
<
  1. ggH@NNLO program
>
>
  1. ggH@NNLO program
 
    • Harlander:2002wh
Changed:
<
<
  1. bbh@nnlo (5FS) program
>
>
  1. bbh@nnlo (5FS) program
 
    • Harlander:2003ai
Changed:
<
<
  1. bbH NLO (4FS)
>
>
  1. bbH NLO (4FS)
 
    • Dittmaier:2003ej, Dawson:2003kb
Changed:
<
<
  1. ggH NLO massive
>
>
  1. ggH NLO massive
 
    • Spira:1995rr
Changed:
<
<
  1. ggH NNLO for scalar Higgs
>
>
  1. ggH NNLO for scalar Higgs
 
    • Anastasiou:2002yz, Ravindran:2003um
Changed:
<
<
  1. ggH NNLO for pseudoscalar Higgs
>
>
  1. ggH NNLO for pseudoscalar Higgs
 
    • Harlander:2002vv, Anastasiou:2002wq
Changed:
<
<
  1. Electroweak corrections by light fermions
>
>
  1. Electroweak corrections by light fermions
 
    • Aglietti:2004nj, Bonciani:2010ms
Changed:
<
<
  1. (N)NLO (S)QCD corrections for h/H/A
>
>
  1. (N)NLO (S)QCD corrections for h/H/A
 
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
Changed:
<
<
  1. HDECAY
>
>
  1. HDECAY
 
    • Djouadi:1997yw, Djouadi:2006bz
Changed:
<
<
  1. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
>
>
  1. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
  Example usage of references in public document:

Revision 1062018-08-13 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Changed:
<
<
In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
<
<
>
>
 

Bibliography

Revision 1052018-05-23 - DavidEnglert

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 154 to 154
 
  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
    • hMSSM_8TeV.root: 8 TeV, tanβ= 0.8-60, mA = 130-1000 GeV (updated 27.05.2016)
Changed:
<
<
    • hMSSM_13TeV.root: 13 TeV, tanβ= 0.8-60, mA = 130-1000 GeV (updated 27.05.2016)
>
>
    • hMSSM_13TeV.root: 13 TeV, tanβ= 0.8-60, mA = 130-1000 GeV (updated 27.05.2016). Bug found in May 2018: Please be aware that the heavy Higgs gluon-fusion cross section (`xs_gg_H` histogram in the .root file) contains some duplicated values along tanb (tanb having a stepsize of 0.1 at lower tanb). If you need cross section values at this resolution, please contact the MSSMNeutral team to request the original ASCII file.
 

Revision 1042017-07-27 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 43 to 43
 
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
  1. HDECAY
    • Djouadi:1997yw, Djouadi:2006bz
Changed:
<
<
  1. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
>
>
  1. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
  Example usage of references in public document:

Revision 1032017-07-27 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 42 to 42
 
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
  1. HDECAY
Changed:
<
<
    • Djouadi:1997yw
>
>
    • Djouadi:1997yw, Djouadi:2006bz
 
  1. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.

Example usage of references in public document:

Revision 1022017-07-13 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 40 to 40
 
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
Changed:
<
<
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
>
>
    • Degrassi:2012vt (NLO-stop scalar mH != 0)
 
  1. HDECAY
    • Djouadi:1997yw
  2. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.

Revision 1012017-02-21 - RogerWolf

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Changed:
<
<
In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
<
<
>
>
 

Bibliography

Revision 1002016-07-06 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 172 to 172
 
Changed:
<
<
  • light stop files
>
>
  • light stop files : The scenario differs from the original one in arXiv:1302.7033 by M1=350 GeV, M2=μ=400 GeV to avoid bounds from direct stop searches.
 

Revision 992016-06-18 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 47 to 47
  Example usage of references in public document:
Changed:
<
<
In the first place, cite LHC Higgs cross-section working group for cross-sections and BRs (use relevant Yellow Report for citation).
>
>
In the first place, please cite the LHC Higgs cross-section working group for providing cross-sections and BRs (by citing the Yellow Reports).
 
Changed:
<
<
Cross-sections for the gluon fusion process are calculated using Sushi [2] (HIGLU [1] is used for "classic" mhmax scenario - more details later in this page).
>
>
For all except the hMSSM, Higgs masses and mixing (and effective Yukawa couplings) have been calculated with Feynhiggs [3].
 
Changed:
<
<
  • For gluon-fusion calculation in Sushi this includes NLO supersymmetric-QCD corrections [7,11], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9] and electroweak effects by light quarks [10]
>
>
Cross sections:
 
Changed:
<
<
  • For the bbH process:
    • Five flavour bbH NNLO QCD calculation is used, as implemented in Sushi [2] based on BBH@NNLO [5]
    • Four flavour NLO QCD calculation [6]
    • Combined using Santander matching (reference in next section)
>
>
  • For the gluon-fusion process inclusive cross sections are obtained with SusHi [2], which includes NLO supersymmetric-QCD corrections [7,11], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9] and electroweak effects by light quarks [10]. (HIGLU [1] is used for "classic" mhmax scenario - see details below.)
 
Changed:
<
<
For all except hMSSM, Higgs masses and mixing and effective Yukawa couplings have been calculated with Feynhiggs [3]
>
>
  • For the bbH process
    • Five flavour NNLO QCD inclusive cross sections are calculated with SusHi [2] based on bbh@nnlo [5]. The results are combined with the
    • Four flavour NLO QCD calculation [6]
    • to Santander matched cross sections (reference in next section).
 
Changed:
<
<
Higgs boson branching fraction to tau leptons has been obtained with FeynHiggs [3] for all scenarios except hMSSM, and with HDECAY for hMSSM [12]. Note if other branching fractions are used the correct references must be checked, they are in general a mixture of HDECAY, FeynHiggs and Prophecy4f (see [13]).
>
>
Branching ratios:
 
Added:
>
>
Whereas in the hMSSM branching ratios are solely computed with HDECAY [12], all other scenarios combine the most precise results of HDECAY [12], FeynHiggs [3] and PROPHECY4f. Relevant references are listed in [13], see LHCHXSWG-2015-002, page 10 bottom, for an example how to cite them.
 

Available benchmark scenarios

Revision 982016-06-17 - RebeccaLane

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 15 to 15
 

Bibliography

If you use numbers provided on this webpage you must cite the following papers:

Changed:
<
<
  • HIGLU program
>
>
  1. HIGLU program
 
    • Spira:1995mt
Changed:
<
<
  • SusHi program
>
>
  1. SusHi program
 
    • Harlander:2012pb
Changed:
<
<
  • FeynHiggs program
>
>
  1. FeynHiggs program
 
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria
Changed:
<
<
  • ggH@NNLO program
>
>
  1. ggH@NNLO program
 
    • Harlander:2002wh
Changed:
<
<
  • bbh@nnlo (5FS) program
>
>
  1. bbh@nnlo (5FS) program
 
    • Harlander:2003ai
Changed:
<
<
  • bbH NLO (4FS)
>
>
  1. bbH NLO (4FS)
 
    • Dittmaier:2003ej, Dawson:2003kb
Changed:
<
<
  • ggH NLO massive
>
>
  1. ggH NLO massive
 
    • Spira:1995rr
Changed:
<
<
  • ggH NNLO for scalar Higgs
>
>
  1. ggH NNLO for scalar Higgs
 
    • Anastasiou:2002yz, Ravindran:2003um
Changed:
<
<
  • ggH NNLO for pseudoscalar Higgs
>
>
  1. ggH NNLO for pseudoscalar Higgs
 
    • Harlander:2002vv, Anastasiou:2002wq
Changed:
<
<
  • Electroweak corrections by light fermions
>
>
  1. Electroweak corrections by light fermions
 
    • Aglietti:2004nj, Bonciani:2010ms
Changed:
<
<
  • (N)NLO (S)QCD corrections for h/H/A
>
>
  1. (N)NLO (S)QCD corrections for h/H/A
 
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Changed:
<
<
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
>
>
  1. HDECAY
    • Djouadi:1997yw
  2. Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.

Example usage of references in public document:

In the first place, cite LHC Higgs cross-section working group for cross-sections and BRs (use relevant Yellow Report for citation).

Cross-sections for the gluon fusion process are calculated using Sushi [2] (HIGLU [1] is used for "classic" mhmax scenario - more details later in this page).

  • For gluon-fusion calculation in Sushi this includes NLO supersymmetric-QCD corrections [7,11], NNLO QCD corrections for the top-quark contribution in the effective theory of a heavy top quark [4,8,9] and electroweak effects by light quarks [10]

  • For the bbH process:
    • Five flavour bbH NNLO QCD calculation is used, as implemented in Sushi [2] based on BBH@NNLO [5]
    • Four flavour NLO QCD calculation [6]
    • Combined using Santander matching (reference in next section)

For all except hMSSM, Higgs masses and mixing and effective Yukawa couplings have been calculated with Feynhiggs [3]

Higgs boson branching fraction to tau leptons has been obtained with FeynHiggs [3] for all scenarios except hMSSM, and with HDECAY for hMSSM [12]. Note if other branching fractions are used the correct references must be checked, they are in general a mixture of HDECAY, FeynHiggs and Prophecy4f (see [13]).

 

Available benchmark scenarios

Revision 972016-05-27 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 64 to 64
 

Access tool for the ROOT files

Changed:
<
<
For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
>
>
For the 13 and 14 TeV runs we provide a new version of the access tool, which is not compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
  ALERT! Please note that for both access tools the cross section predictions (and uncertainties) are consistently provided in pb .
Line: 124 to 124
 Most scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=2000 GeV and between tanβ=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM:
Added:
>
>
ALERT! 27.05.2016: Update of the (8,) 13 and 14TeV ROOT histograms with corrected bbH cross sections .
 
  • low-tb-high files
Changed:
<
<
>
>
 
  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
Changed:
<
<
>
>
    • hMSSM_8TeV.root: 8 TeV, tanβ= 0.8-60, mA = 130-1000 GeV (updated 27.05.2016)
    • hMSSM_13TeV.root: 13 TeV, tanβ= 0.8-60, mA = 130-1000 GeV (updated 27.05.2016)
 
  • mh-max files
Changed:
<
<
>
>
 
  • mh-mod+ files
Changed:
<
<
>
>
 
  • mh-mod- files
Changed:
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<
>
>
 
  • light stau files
Changed:
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<
>
>
 
  • light stop files
Changed:
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<
>
>
 
  • tauphobic files
Changed:
<
<
>
>
 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties. An update of the scenarios compatible with v1.0 will follow.)
Line: 443 to 445
 
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1444123587" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30560" user="amccarn" version="3"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1448451958" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="7579912" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1448451977" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="7582180" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1448452001" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="5202303" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1448452023" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="5203061" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1448452046" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="7580753" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1448452071" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="7582484" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1448452162" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="7591249" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1448452181" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="7593066" user="ffrensch" version="3"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1448452115" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="7589569" user="ffrensch" version="3"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1448452138" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="7588967" user="ffrensch" version="3"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1448452205" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="5931670" user="ffrensch" version="3"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1448452224" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="5933947" user="ffrensch" version="3"
>
>
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1464351304" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="7580969" user="sliebler" version="4"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1464351326" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="7580331" user="sliebler" version="4"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1464351371" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="5202162" user="sliebler" version="4"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1464351386" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="5202769" user="sliebler" version="4"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1464351421" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="7581713" user="sliebler" version="4"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1464351447" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="7580651" user="sliebler" version="4"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1464351486" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="7592501" user="sliebler" version="4"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1464351526" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="7591272" user="sliebler" version="4"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1464351574" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="7590680" user="sliebler" version="4"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1464351602" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="7587152" user="sliebler" version="4"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1464351663" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="5932404" user="sliebler" version="4"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1464351681" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="5932470" user="sliebler" version="4"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 962016-02-11 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Changed:
<
<
In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
<
<
>
>
 

Bibliography

Revision 952016-02-04 - RogerWolf

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 65 to 65
 

Access tool for the ROOT files

For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.

Added:
>
>
ALERT! Please note that for both access tools the cross section predictions (and uncertainties) are consistently provided in pb .
 
  • Access tool version 0.5 (for 7 and 8 TeV): Download the header file and the implementation file. For information about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.

Revision 942016-01-28 - RogerWolf

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Changed:
<
<
In case of questions or problems, please report them to all the conveners.
>
>
In case of questions or problems, please report them to all the conveners.
 
Changed:
<
<
>
>
 
Deleted:
<
<
Don't forget to remove 'SPAMNOT' in the email addresses before sending.
 

Bibliography

If you use numbers provided on this webpage you must cite the following papers:

Revision 932015-12-03 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 152 to 152
 

  • tauphobic files
Changed:
<
<
>
>
 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties. An update of the scenarios compatible with v1.0 will follow.)

Revision 922015-11-25 - AllisonMcCarn

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 129 to 129
 
  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
Changed:
<
<
>
>
 

Revision 912015-11-25 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

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META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1444123587" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30560" user="amccarn" version="3"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1447683239" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="27368436" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1447683265" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="27369700" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1447684029" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="9106327" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1447684051" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="9106350" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1447683915" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="26929170" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1447684002" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="26929627" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1447684338" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="26950979" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1447684368" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="26951167" user="ffrensch" version="2"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1447685082" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="26939557" user="ffrensch" version="2"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1447685115" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="26937261" user="ffrensch" version="2"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1447685137" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="21066341" user="ffrensch" version="2"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1447685194" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="21068728" user="ffrensch" version="2"
>
>
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1448451958" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="7579912" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1448451977" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="7582180" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1448452001" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="5202303" user="ffrensch" version="3"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1448452023" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="5203061" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1448452046" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="7580753" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1448452071" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="7582484" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1448452162" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="7591249" user="ffrensch" version="3"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1448452181" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="7593066" user="ffrensch" version="3"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1448452115" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="7589569" user="ffrensch" version="3"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1448452138" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="7588967" user="ffrensch" version="3"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1448452205" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="5931670" user="ffrensch" version="3"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1448452224" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="5933947" user="ffrensch" version="3"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 902015-11-16 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 442 to 442
 
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1444123587" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30560" user="amccarn" version="3"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1439303475" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="27367721" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1439303477" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="27368981" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1439303477" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="9215322" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1439303478" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="9215319" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1439303480" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="26928422" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1439303482" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="26928917" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1439303484" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="26950225" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1439303486" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="26950421" user="amccarn" version="1"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1439305359" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="26938819" user="amccarn" version="1"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1439305361" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="26936510" user="amccarn" version="1"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1439305362" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="21065686" user="amccarn" version="1"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1439305363" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="21068047" user="amccarn" version="1"
>
>
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1447683239" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="27368436" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1447683265" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="27369700" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1447684029" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="9106327" user="ffrensch" version="2"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1447684051" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="9106350" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1447683915" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="26929170" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1447684002" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="26929627" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1447684338" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="26950979" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1447684368" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="26951167" user="ffrensch" version="2"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1447685082" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="26939557" user="ffrensch" version="2"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1447685115" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="26937261" user="ffrensch" version="2"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1447685137" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="21066341" user="ffrensch" version="2"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1447685194" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="21068728" user="ffrensch" version="2"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 892015-11-03 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 148 to 148
 

  • light stop files
Changed:
<
<
>
>
 
Line: 163 to 163
 

Scenarios named in green are obtained with the following setup:

Changed:
<
<
FeynHiggs 2.10.2 with default flags + SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms)
>
>
FeynHiggs 2.10.2 with default flags + SusHi 1.4.1 (=1.5.0) + bbH (4FS) (including Yt*Yb terms)
 
  • ggH choices:
    • μ_R=μ_F=m_Phi/2.
    • Scale uncertainties: Seven combinations of scales μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2

Revision 882015-11-03 - AllisonMcCarn

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 128 to 128
 

  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
Changed:
<
<
>
>
 

  • mh-max files

Revision 872015-10-28 - AllisonMcCarn

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 128 to 128
 

  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
Changed:
<
<
>
>
 

Revision 862015-10-06 - AllisonMcCarn

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 439 to 439
 
META FILEATTACHMENT attachment="mssm_xs_tools.C_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.C_v0.5" path="mssm_xs_tools.C_v0.5" size="27365" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.h_v0.5" path="mssm_xs_tools.h_v0.5" size="11534" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.C_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.C_v1.0" path="mssm_xs_tools.C_v1.0" size="6688" user="ffrensch" version="2"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30494" user="ffrensch" version="2"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1444123587" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30560" user="amccarn" version="3"
 
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1439303475" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="27367721" user="amccarn" version="1"

Revision 852015-09-18 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 43 to 43
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Changed:
<
<
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
>
>
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
 

Available benchmark scenarios

Line: 109 to 109
 Please check the dedicated twiki page here and the information provided in:

"Benchmark scenarios for low tanβ in the MSSM"

Changed:
<
<
E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
>
>
E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
 LHCHXSWG-2015-002

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Line: 123 to 123
 Most scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=2000 GeV and between tanβ=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM:
Changed:
<
<

  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices

>
>

  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices

 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties. An update of the scenarios compatible with v1.0 will follow.)
Line: 357 to 357
 

Outdated discussions (kept for the sake of completeness)

Changed:
<
<
Considerations on H->tautau (~2011)
>
>
Considerations on H->tautau (~2011)
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"

Revision 842015-08-12 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 43 to 43
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Changed:
<
<
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in .
>
>
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
 

Available benchmark scenarios

Revision 832015-08-12 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 120 to 120
 M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
arXiv:1302.7033
Changed:
<
<
The scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=0.5 and 60.
>
>
Most scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=2000 GeV and between tanβ=0.5 and 60.
 ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM:

  • low-tb-high files
Changed:
<
<
>
>
 
Changed:
<
<
  • hMSSM files: Produced with SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
>
>
  • hMSSM files: Produced with SusHi 1.4.1 (with 2HDM input)+ bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices
 
  • mh-max files
Changed:
<
<
>
>
 
  • mh-mod+ files
Changed:
<
<
>
>
 
  • mh-mod- files
Changed:
<
<
>
>
 
  • light stau files
Changed:
<
<
>
>
 
  • light stop files
Changed:
<
<
>
>
 
  • tauphobic files
Changed:
<
<
>
>
 
Changed:
<
<
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties.)
>
>
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties. An update of the scenarios compatible with v1.0 will follow.)
 

Revision 822015-08-11 - AllisonMcCarn

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 121 to 121
 arXiv:1302.7033

The scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=0.5 and 60.

Changed:
<
<
ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM are on the way.
>
>
ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM:

  • hMSSM files: Produced with SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms) and green ggH and bbH choices

 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties.)
Line: 410 to 442
 
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30494" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="lightstau1_13TeV.root" attr="" comment="" date="1439303475" name="lightstau1_13TeV.root" path="lightstau1_13TeV.root" size="27367721" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstau1_14TeV.root" attr="" comment="" date="1439303477" name="lightstau1_14TeV.root" path="lightstau1_14TeV.root" size="27368981" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstopmod_13TeV.root" attr="" comment="" date="1439303477" name="lightstopmod_13TeV.root" path="lightstopmod_13TeV.root" size="9215322" user="amccarn" version="1"
META FILEATTACHMENT attachment="lightstopmod_14TeV.root" attr="" comment="" date="1439303478" name="lightstopmod_14TeV.root" path="lightstopmod_14TeV.root" size="9215319" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodm_13TeV.root" attr="" comment="" date="1439303480" name="mhmodm_13TeV.root" path="mhmodm_13TeV.root" size="26928422" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodm_14TeV.root" attr="" comment="" date="1439303482" name="mhmodm_14TeV.root" path="mhmodm_14TeV.root" size="26928917" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodp_mu200_13TeV.root" attr="" comment="" date="1439303484" name="mhmodp_mu200_13TeV.root" path="mhmodp_mu200_13TeV.root" size="26950225" user="amccarn" version="1"
META FILEATTACHMENT attachment="mhmodp_mu200_14TeV.root" attr="" comment="" date="1439303486" name="mhmodp_mu200_14TeV.root" path="mhmodp_mu200_14TeV.root" size="26950421" user="amccarn" version="1"
META FILEATTACHMENT attachment="newmhmax_mu200_13TeV.root" attr="" comment="" date="1439305359" name="newmhmax_mu200_13TeV.root" path="newmhmax_mu200_13TeV.root" size="26938819" user="amccarn" version="1"
META FILEATTACHMENT attachment="newmhmax_mu200_14TeV.root" attr="" comment="" date="1439305361" name="newmhmax_mu200_14TeV.root" path="newmhmax_mu200_14TeV.root" size="26936510" user="amccarn" version="1"
META FILEATTACHMENT attachment="tauphobic_13TeV.root" attr="" comment="" date="1439305362" name="tauphobic_13TeV.root" path="tauphobic_13TeV.root" size="21065686" user="amccarn" version="1"
META FILEATTACHMENT attachment="tauphobic_14TeV.root" attr="" comment="" date="1439305363" name="tauphobic_14TeV.root" path="tauphobic_14TeV.root" size="21068047" user="amccarn" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 812015-08-04 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 47 to 47
 

Available benchmark scenarios

Changed:
<
<
Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tan(β) plane. In detail the histograms contain:
>
>
Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tanβ plane. In detail the histograms contain:
 
  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
Line: 104 to 104
  mssm.xsec("gg->H::pdfasUp",300,3)
Changed:
<
<

Discussion of MSSM scenarios with low tan(β) and Heavy SUSY

>
>

Discussion of MSSM scenarios with low tanβ and Heavy SUSY

  Please check the dedicated twiki page here and the information provided in:
Changed:
<
<
"Benchmark scenarios for low tan(β) in the MSSM"
>
>
"Benchmark scenarios for low tanβ in the MSSM"
 E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
LHCHXSWG-2015-002
Line: 120 to 120
 M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
arXiv:1302.7033
Changed:
<
<
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tan(β)-high scenario/hMSSM are on the way.
>
>
The scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tanβ-high scenario/hMSSM are on the way.
 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties.)
Changed:
<
<
>
>
 
Line: 144 to 144
 

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

Changed:
<
<
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
>
>
The scans in the m_A-tanβ-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=1 and 60. For lower values of tanβ between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
 
  • mhmodm
Changed:
<
<
>
>
 
  • mhmodp (with μ=200 GeV)
Changed:
<
<

>
>

 
  • lightstau
Changed:
<
<
>
>
 
Changed:
<
<
  • lightstopmod (tan(β) below 0.7 is not used due to problematic two-loop stop mass corrections
>
>
  • lightstopmod (tanβ below 0.7 is not used due to problematic two-loop stop mass corrections
  SUSY QCD corrections above m_A> 600 GeV are not reliable due to the stop quark threshold.)
Changed:
<
<
>
>
 
  • tauphobic
    • Please find below the tauphobic scenario with A_τ=A_t and μ=2000GeV, available since 18.11.2014:
Changed:
<
<
>
>
 
Changed:
<
<
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed):
>
>
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tanβ=7 and tanβ=8 have a numerical instability. Interpolation needed):
 
  • mhmax
Changed:
<
<
>
>
  Scenarios named in red are obtained with the following setup:
FeynHiggs 2.8.6 with default flags + SusHi 1.0.6 + bbH (4FS) scans
Line: 220 to 220
  Subsequently you may find the numbers for the 'traditional mhmax' scenario, which is defined by the parameter choice:
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
Changed:
<
<
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tan(β) plane.
>
>
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tanβ plane.
 
Changed:
<
<
We present the ROOT histograms produced by the MSSM subgroup at an early stage in the m_A-tan(β)-plane for 7 TeV and for 14 TeV. The scans have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan). For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. They are kept for documentation:
>
>
We present the ROOT histograms produced by the MSSM subgroup at an early stage in the m_A-tanβ-plane for 7 TeV and for 14 TeV. The scans have been made between m_A=90 GeV and m_A=1000 GeV and between tanβ=1 and 60 (5 and 70 for the 14 TeV scan). For very low tanβ, the scan is done between tanβ=0.5 and 0.9 in steps of 0.1. They are kept for documentation:
  FeynHiggs 2.7.4 with default flags + HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
Line: 239 to 239
 
  • bbH (5FS) scale choices:
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
Changed:
<
<
>
>
  The scenario is availabe for other (negative) values of μ as well, see attachments!

Revision 802015-08-03 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 64 to 64
  The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.
Changed:
<
<

Access tool for the ROOT files

>
>

Access tool for the ROOT files

  For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
Line: 104 to 104
  mssm.xsec("gg->H::pdfasUp",300,3)
Changed:
<
<

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

>
>

Discussion of MSSM scenarios with low tan(β) and Heavy SUSY

Please check the dedicated twiki page here and the information provided in:

"Benchmark scenarios for low tan(β) in the MSSM"
E. Bagnaschi, F. Frensch, S. Heinemeyer, G. Lee, S. Liebler, M. Mühlleitner, A. Mc Carn, J. Quevillon, N. Rompotis, P. Slavich, M. Spira, C. Wagner, R. Wolf
LHCHXSWG-2015-002

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the
Line: 134 to 142
 
Changed:
<
<

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

>
>

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

  The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
Line: 208 to 216
  Please use v5 of the access tool (remove "_v0.5" tag): header file and implementation file.
Changed:
<
<

ROOT histograms: 'traditional mhmax' benchmark scenario - Access tool version 0.4

>
>

ROOT histograms: 'traditional mhmax' benchmark scenario - Access tool version 0.4

  Subsequently you may find the numbers for the 'traditional mhmax' scenario, which is defined by the parameter choice:
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
Line: 240 to 248
  To read these files please use the old tool (v4): header file and implementation file.
Deleted:
<
<

Discussion of MSSM scenarios with low tan(beta) and Heavy SUSY

See dedicated twiki page here.

Some consideration on h/H/A ->tau tau (xs * BR)

This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.

We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(β)) points (which is not so useful).

That being said, we recommend the following:

2a) As far as the PDF error is concerned, the simplest way out is to determine the PDF error on the sum of different production mechanisms (in the usual way), rather than on each of the cross sections separately. Then the correlation is automatically taken into account. (comment by S. Forte)

2b) Therefore, in combining ggF and bbH one has to take into full account one caveat: since the b-PDFs so far are only contructed as being purely perturbative, i.e. fully generated by g -> bb spitting at LL level, a sum of the PDF uncertainties - linear as well as quadratic - seems to double count the gluon PDF uncertainties. Thus, one would prefer a scheme in which the PDF uncertainties of the sum ggF+bbH are computed as those to a single observable. The situation will only become different once there are data on b-PDFs... Noone knows until now if there is a non-perturbative intrinsic b contribution or not, i.e. whether the non-perturbative component is sizeable or not. We believe that 4-5 GeV as the input scale is deep in the perturbative regime. (comment by M. Spira)

2b) To summarize: we recommend to do once the check 2a) and compare the result with the simple addition in quadrature: it could well be that even though in principles the g and b are correlated, in practice the simple sum in quadrature works well. (comment by S. Forte)

3) Typically we vary scales in some range (like M_H/2 to 2M_H), but we never start thinking about it as if that represents the true uncertainty. It only represents `the best we can do'. But this should be clear from the YR.

The scale variation follows the recommendation of Harlander/Kilgore. It serves as a conservative estimate of the scale dependence for this process. (comment by M. Spira and M. Warsinsky)

4a) SUSY-QCD corrections: Statements that SUSY-QCD corrections are just of this and that size cannot be made, because they strongly depend a) on the scenario, b) on the details how LO is defined.

To a): The variety of all scenarios is too large and rich for overall statements in the YR. To b): residual corrections typically are small (not like 30% or so) if LO is based on loop-corrected masses of the external Higgs particles and appropriate effective couplings.

4b) SUSY-QCD corrections:

Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Δ_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Δ_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)

5) Δ_b: We know exactly where to place Δ_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)

6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)

 

Tools and Programs

If you aim to get cross sections and branching ratios for other scenarios than the ones on this webpage, you may use the following codes, which were also used to calculate the provided numbers:

Line: 349 to 323
 
Mtop^pole 172.5 GeV
Added: >
>

Outdated discussions (kept for the sake of completeness)

Considerations on H->tautau (~2011) 

META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
META FILEATTACHMENT attachment="out.mhmax_7_nnlo.root" attr="" comment="Scan which include the ggF+bbH combined PDF uncertainty" date="1296827611" name="out.mhmax_7_nnlo.root" path="out.mhmax_7_nnlo.root" size="28151505" user="monicava" version="1"
Line: 431 to 409 
META FILEATTACHMENT attachment="mssm_xs_tools.C_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.C_v1.0" path="mssm_xs_tools.C_v1.0" size="6688" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30494" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
Added: >
>
META FILEATTACHMENT attachment="considerationsonhiggstotautau.txt" attr="" comment="Discussion on H->tau tau at the time of YR1" date="1438592629" name="considerationsonhiggstotautau.txt" path="considerationsonhiggstotautau.txt" size="3676" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 792015-08-03 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 428 to 428
 
META FILEATTACHMENT attachment="mhmodp_mu-1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-1000_8TeV.root" path="mhmodp_mu-1000_8TeV.root" size="8579361" user="sliebler" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.C_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.C_v0.5" path="mssm_xs_tools.C_v0.5" size="27365" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.h_v0.5" path="mssm_xs_tools.h_v0.5" size="11534" user="ffrensch" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools.C_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.C_v1.0" path="mssm_xs_tools.C_v1.0" size="6689" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30775" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="1"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.C_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.C_v1.0" path="mssm_xs_tools.C_v1.0" size="6688" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30494" user="ffrensch" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438591735" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="2"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 782015-07-31 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 43 to 43
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Changed:
<
<
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
>
>
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in .
 

Available benchmark scenarios

Line: 67 to 67
 

Access tool for the ROOT files

For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.

Changed:
<
<
>
>
  For information about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4.
Changed:
<
<
To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.
>
>
Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.
 
     root -l
     .L mssm_xs_tools.C++
Line: 84 to 84
  test.Give_XsecUnc_pdfalphas68down_ggFA(120,30) ...
Changed:
<
<
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): Download the header file and the implementation file and the python wrapper. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
>
>
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): Download the header file and the implementation file and the python wrapper. Please remove the "v_1.0" tag at the end of the files. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
 
     root -l
Changed:
<
<
.L mssm_xs_tools_v1.0.C++
>
>
.L mssm_xs_tools.C++
  Then either the python wrapper or the .C file could be used:

Line: 206 to 206
 
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
Changed:
<
<
Please use v5 of the access tool: header file and implementation file.
>
>
Please use v5 of the access tool (remove "_v0.5" tag): header file and implementation file.
 

ROOT histograms: 'traditional mhmax' benchmark scenario - Access tool version 0.4

Line: 351 to 351
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
Deleted:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools.h" attr="" comment="Access tool: version 0.5" date="1386172658" name="mssm_xs_tools.h" path="mssm_xs_tools.h" size="11337" user="monicava" version="4"
META FILEATTACHMENT attachment="mssm_xs_tools.C" attr="" comment="Access tool: version 0.5" date="1386172658" name="mssm_xs_tools.C" path="mssm_xs_tools.C" size="27175" user="monicava" version="10"
 


META FILEATTACHMENT attachment="out.mhmax_7_nnlo.root" attr="" comment="Scan which include the ggF+bbH combined PDF uncertainty" date="1296827611" name="out.mhmax_7_nnlo.root" path="out.mhmax_7_nnlo.root" size="28151505" user="monicava" version="1"
META FILEATTACHMENT attachment="santandermatching-hks.pdf" attr="" comment="Description of Santander matching procedure for inclusive pp-->H(bb) cross-section" date="1307193388" name="santandermatching-hks.pdf" path="santandermatching-hks.pdf" size="181607" stream="santandermatching-hks.pdf" tmpFilename="/usr/tmp/CGItemp52250" user="schumach" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_7_nnlo.root" attr="" comment="mhmax mu=200, 7 TeV" date="1321004712" name="out.mhmax_mu200_7_nnlo.root" path="out.mhmax_mu200_7_nnlo.root" size="28151505" user="monicava" version="1"
Line: 428 to 426
 
META FILEATTACHMENT attachment="mhmodp_mu-200_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-200_8TeV.root" path="mhmodp_mu-200_8TeV.root" size="11704522" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-500_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-500_8TeV.root" path="mhmodp_mu-500_8TeV.root" size="11708284" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-1000_8TeV.root" path="mhmodp_mu-1000_8TeV.root" size="8579361" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.C" attr="" comment="access tools v1.0" date="1437749103" name="mssm_xs_tools_v1.0.C" path="mssm_xs_tools_v1.0.C" size="6694" user="sliebler" version="2"
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.h" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.h" path="mssm_xs_tools_v1.0.h" size="30775" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.py.txt" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.py.txt" path="mssm_xs_tools_v1.0.py.txt" size="4755" user="ffrensch" version="1"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.C_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.C_v0.5" path="mssm_xs_tools.C_v0.5" size="27365" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v0.5" attr="" comment="Access tool: version 0.5" date="1438379552" name="mssm_xs_tools.h_v0.5" path="mssm_xs_tools.h_v0.5" size="11534" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.C_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.C_v1.0" path="mssm_xs_tools.C_v1.0" size="6689" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.h_v1.0" path="mssm_xs_tools.h_v1.0" size="30775" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.py_v1.0" attr="" comment="Access tool: version 1.0" date="1438379632" name="mssm_xs_tools.py_v1.0" path="mssm_xs_tools.py_v1.0" size="4755" user="ffrensch" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 772015-07-24 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 88 to 88
  To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
     root -l
Changed:
<
<
.L mssm_xs_tools.C++
>
>
.L mssm_xs_tools_v1.0.C++
  Then either the python wrapper or the .C file could be used:

Changed:
<
<
mssm=mssm_xs_tools("hMSSM_8TeV.root",True,0) mssm.mass("H,300,3) mssm.width("H,300,3) mssm.br("H-­>tautau,300,3) mssm.xsec("gg->H,300,3) mssm.xsec(?bb5F->H,300,3) mssm.xsec(?bb4F-­>H,300,3) mssm.xsec("bbSantander->H,300,3) mssm.xsec("gg->H::scaleUp,300,3) mssm.xsec("gg->H::pdfasUp,300,3)
>
>
mssm=mssm_xs_tools("hMSSM_8TeV.root",true,0) // "true" enables interpolation between the grid points, "0" avoids messages by the access tool, set to "3" or "100" for additional information mssm.mass("H",300,3) mssm.width("H",300,3) mssm.br("H-­>tautau",300,3) mssm.xsec("gg->H",300,3) mssm.xsec("bb5F->H",300,3) mssm.xsec("bb4F-­>H",300,3) mssm.xsec("bbSantander->H",300,3) mssm.xsec("gg->H::scaleUp",300,3) mssm.xsec("gg->H::pdfasUp",300,3)
 

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Line: 428 to 428
 
META FILEATTACHMENT attachment="mhmodp_mu-200_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-200_8TeV.root" path="mhmodp_mu-200_8TeV.root" size="11704522" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-500_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-500_8TeV.root" path="mhmodp_mu-500_8TeV.root" size="11708284" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-1000_8TeV.root" path="mhmodp_mu-1000_8TeV.root" size="8579361" user="sliebler" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.C" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.C" path="mssm_xs_tools_v1.0.C" size="6689" user="ffrensch" version="1"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.C" attr="" comment="access tools v1.0" date="1437749103" name="mssm_xs_tools_v1.0.C" path="mssm_xs_tools_v1.0.C" size="6694" user="sliebler" version="2"
 
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.h" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.h" path="mssm_xs_tools_v1.0.h" size="30775" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.py.txt" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.py.txt" path="mssm_xs_tools_v1.0.py.txt" size="4755" user="ffrensch" version="1"
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 762015-07-22 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 22 to 22
 
  • SusHi program
    • Harlander:2012pb
  • FeynHiggs program
Changed:
<
<
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh
>
>
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh, Hahn:2013ria
 
  • ggH@NNLO program
    • Harlander:2002wh
  • bbh@nnlo (5FS) program
Line: 43 to 43
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Added:
>
>
  • Last but not least acknowledge the work of the BR subgroup, which is based upon the publications given in this tex-file.
 

Available benchmark scenarios

Revision 752015-07-14 - FelixFrensch

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 43 to 44
 
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA != 0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Deleted:
<
<
 

Available benchmark scenarios

Changed:
<
<
Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tan(β) plane. In detail the histograms contain:
>
>
Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tan(β) plane. In detail the histograms contain:
 
  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
Changed:
<
<
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
>
>
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
 
  • cross sections for b-associated h/H/A production in the 4 flavour scheme (4FS) (NLO QCD) including scale uncertainties.
Changed:
<
<
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
>
>
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
 
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons, see also BR subgroup.

The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available:
"Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach"
R. Harlander, M. Krämer, and M. Schumacher

Changed:
<
<
Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
>
>
Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
 santandermatching-hks.pdf: Description of Santander matching procedure for inclusive pp-->H(bb) cross-section

The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.

Line: 67 to 67
  For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
Changed:
<
<
For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4.
>
>
For information about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4.
  To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.
     root -l
Changed:
<
<
.L mssm_xs_tools.C
>
>
.L mssm_xs_tools.C++
  mssm_xs_tools test test.SetInput("out.mhmax_mu200_7_nnlo.tanBeta_gte1.root") test.help()
Line: 83 to 83
  test.Give_XsecUnc_pdfalphas68down_ggFA(120,30) ...
Changed:
<
<
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): to be released.
>
>
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): Download the header file and the implementation file and the python wrapper. To work with the access tool you have to include the corresponding C++ class. First a shared library has to be compiled.
         root -l
         .L mssm_xs_tools.C++
         
    Then either the python wrapper or the .C file could be used:
         mssm=mssm_xs_tools("hMSSM_8TeV.root",True,0)   
         mssm.mass("H,300,3)   
         mssm.width("H,300,3)   
         mssm.br("H-­>tautau,300,3)   
         mssm.xsec("gg->H,300,3)   
         mssm.xsec(?bb5F->H,300,3)   
         mssm.xsec(?bb4F-­>H,300,3)   
         mssm.xsec("bbSantander->H,300,3)  
         mssm.xsec("gg->H::scaleUp,300,3)   
         mssm.xsec("gg->H::pdfasUp,300,3)   
         
 

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the Discovery of a Higgs-like Particle"

Changed:
<
<
M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
>
>
M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
 arXiv:1302.7033
Changed:
<
<
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tan(β)-high scenario/hMSSM are on the way.
>
>
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tan(β)-high scenario/hMSSM are on the way.
 
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties.)
Changed:
<
<
>
>
  Scenarios named in green are obtained with the following setup:
FeynHiggs 2.10.2 with default flags + SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms)
  • ggH choices:
Changed:
<
<
    • μ_R=μ_F=m_Phi/2.
    • Scale uncertainties: Seven combinations of scales μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
>
>
    • μ_R=μ_F=m_Phi/2.
    • Scale uncertainties: Seven combinations of scales μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
 
  • bbH (5FS) choices:
Changed:
<
<
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale uncertainties: Seven combinations of scales μ_R={m_Phi/2,m_Phi,2m_Phi} and μ_F={m_Phi/8,m_Phi/4,m_Phi/2} with the constraint 2 ≤ μ_R/μ_F ≤ 8
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
>
>
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale uncertainties: Seven combinations of scales μ_R={m_Phi/2,m_Phi,2m_Phi} and μ_F={m_Phi/8,m_Phi/4,m_Phi/2} with the constraint 2 ≤ μ_R/μ_F ≤ 8
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
 

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

Changed:
<
<
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
>
>
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
 
  • mhmodm
Changed:
<
<

>
>

 
  • lightstau
Changed:
<
<

>
>

 
  • tauphobic
Changed:
<
<
>
>
 
Changed:
<
<
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed):
>
>
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed):
 
  • mhmax
Changed:
<
<
>
>
  Scenarios named in red are obtained with the following setup:
FeynHiggs 2.8.6 with default flags + SusHi 1.0.6 + bbH (4FS) scans
  • ggH scale choices:
Changed:
<
<
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • bbH (5FS) scale choices:
Changed:
<
<
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
>
>
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
  Scenarios named in blue are obtained with the following setup:
HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
Changed:
<
<
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • bbH (5FS) scale choices:
Changed:
<
<
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
>
>
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
  Please use v5 of the access tool: header file and implementation file.

ROOT histograms: 'traditional mhmax' benchmark scenario - Access tool version 0.4

Subsequently you may find the numbers for the 'traditional mhmax' scenario, which is defined by the parameter choice:

Changed:
<
<
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tan(β) plane.
>
>
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tan(β) plane.
 
Changed:
<
<
We present the ROOT histograms produced by the MSSM subgroup at an early stage in the m_A-tan(β)-plane for 7 TeV and for 14 TeV. The scans have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan). For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. They are kept for documentation:
>
>
We present the ROOT histograms produced by the MSSM subgroup at an early stage in the m_A-tan(β)-plane for 7 TeV and for 14 TeV. The scans have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan). For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. They are kept for documentation:
  FeynHiggs 2.7.4 with default flags + HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
Changed:
<
<
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • out.mhmax_7.root: mhmax, 7 TeV
  • out.mhmax_7.root: mhmax, 14 TeV (no bbh 4FS and thus no Santander-matched XS and no PDF uncertainties! You obtain unreasonable results by the access tool!)

For 7 and 8 TeV please make use of the subsequent ROOT histograms:
HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans

  • ggH scale choices:
Changed:
<
<
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • bbH (5FS) scale choices:
Changed:
<
<
>
>
 
Changed:
<
<
The scenario is availabe for other (negative) values of μ as well, see attachments!
>
>
The scenario is availabe for other (negative) values of μ as well, see attachments!
  To read these files please use the old tool (v4): header file and implementation file.
Line: 229 to 247
  This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.
Changed:
<
<
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(β)) points (which is not so useful).
>
>
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(β)) points (which is not so useful).
  That being said, we recommend the following:
Line: 249 to 267
  4b) SUSY-QCD corrections:
Changed:
<
<
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Δ_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Δ_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)
>
>
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Δ_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Δ_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)
 
Changed:
<
<
5) Δ_b: We know exactly where to place Δ_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)
>
>
5) Δ_b: We know exactly where to place Δ_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)
  6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)
Line: 269 to 288
 

Choice of input parameters

Changed:
<
<
All SusHi runs make use of the naive Δ_b resummation (Y_b -> Y_b/(1+ Δ_b)) using the Δ_b from FeynHiggs for gluon fusion and the full resummation for bottom-quark annihilation (5FS) (see SusHi manual). They include NLO squark contributions expanded in heavy SUSY masses and electroweak corrections by light quarks.
>
>
All SusHi runs make use of the naive Δ_b resummation (Y_b -> Y_b/(1+ Δ_b)) using the Δ_b from FeynHiggs for gluon fusion and the full resummation for bottom-quark annihilation (5FS) (see SusHi manual). They include NLO squark contributions expanded in heavy SUSY masses and electroweak corrections by light quarks.
 
HIGLU Standard Model parameters
Changed:
<
<
α_S(MZ) 0.12018, 2 loop
>
>
α_S(MZ) 0.12018, 2 loop
 
Lambda_QCD^(5) 226 MeV
PDF MSTW2008nlo68cl
Mcharm 1.40 GeV
Line: 292 to 310
 
MZ 91.1876 GeV
   
SusHi 1.0.6 Standard Model parameters
Changed:
<
<
α_S(MZ) 0.119 / PDF value
>
>
α_S(MZ) 0.119 / PDF value
 
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl
Mcharm 1.40 GeV
Line: 305 to 323
 
Standard Model parameters
Mtop 172.5 GeV
mb(mb) MSbar 4.213 GeV
Changed:
<
<
α_S(MZ) 0.119
>
>
α_S(MZ) 0.119
    
SusHi 1.4.1 Standard Model parameters
Changed:
<
<
α_S(MZ) 0.119 / PDF value
1/α_EW(MZ) 127.67 / fictitious value to obtain mW=80.398 GeV
>
>
α_S(MZ) 0.119 / PDF value
1/α_EW(MZ) 127.67 / fictitious value to obtain mW=80.398 GeV
 
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
mc(mc) MSbar 1.28 GeV
Line: 321 to 339
 
FeynHiggs 2.10.2 with default flags
Standard Model parameters
Changed:
<
<
α_S(MZ) 0.119
>
>
α_S(MZ) 0.119
 
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
MW 80.398 GeV
Line: 410 to 427
 
META FILEATTACHMENT attachment="mhmodp_mu-200_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-200_8TeV.root" path="mhmodp_mu-200_8TeV.root" size="11704522" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-500_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-500_8TeV.root" path="mhmodp_mu-500_8TeV.root" size="11708284" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-1000_8TeV.root" path="mhmodp_mu-1000_8TeV.root" size="8579361" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.C" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.C" path="mssm_xs_tools_v1.0.C" size="6689" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.h" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.h" path="mssm_xs_tools_v1.0.h" size="30775" user="ffrensch" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v1.0.py.txt" attr="" comment="access tools v1.0" date="1436874775" name="mssm_xs_tools_v1.0.py.txt" path="mssm_xs_tools_v1.0.py.txt" size="4755" user="ffrensch" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 742015-07-01 - RogerWolf

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 9 to 9
  In case of questions or problems, please report them to all the conveners.

Changed:
<
<
>
>
 

Don't forget to remove 'SPAMNOT' in the email addresses before sending.

Revision 732015-06-12 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 309 to 309
    
SusHi 1.4.1 Standard Model parameters
α_S(MZ) 0.119 / PDF value
Changed:
<
<
1/α_EW(MZ) 127.67 / fictious value to obtain mW=80.398 GeV
>
>
1/α_EW(MZ) 127.67 / fictitious value to obtain mW=80.398 GeV
 
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
mc(mc) MSbar 1.28 GeV

Revision 722015-04-25 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 96 to 96
 The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tan(β)-high scenario/hMSSM are on the way.
Changed:
<
<
  • mhmodp (For the time being, you may use the old access tool for these scenarios, although you have no access to uncertainties.)
>
>
  • mhmodp (For the time being, you may use the old access tool version 0.5 for these scenarios, although you have no access to uncertainties.)
 
Line: 107 to 107
 FeynHiggs 2.10.2 with default flags + SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms)
  • ggH choices:
    • μ_R=μ_F=m_Phi/2.
Changed:
<
<
    • Scale uncertainties: Seven combination of scales according to μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass
>
>
    • Scale uncertainties: Seven combinations of scales μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
 
  • bbH (5FS) choices:
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
Changed:
<
<
    • Scale uncertainties: Seven combination of scales according to μ_R={m_Phi/2,m_Phi,2m_Phi} and μ_F={m_Phi/8,m_Phi/4,m_Phi/2} with the constraint 2 ≤ μ_R/μ_F ≤ 8
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass
>
>
    • Scale uncertainties: Seven combinations of scales μ_R={m_Phi/2,m_Phi,2m_Phi} and μ_F={m_Phi/8,m_Phi/4,m_Phi/2} with the constraint 2 ≤ μ_R/μ_F ≤ 8
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass using MSTW2008
 

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

Line: 125 to 125
 
Changed:
<
<
  • mhmodp
>
>
  • mhmodp (with μ=200 GeV)
 

Revision 712015-04-24 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 61 to 61
 Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
santandermatching-hks.pdf: Description of Santander matching procedure for inclusive pp-->H(bb) cross-section
Changed:
<
<
The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Download the header file and the implementation file. For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. The current version of the access tool is v5 provided by Monica Vazquez Acosta, Trevor Vickey, Markus Warsinsky and Felix Frensch.
>
>
The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Details can be found below.
 
Changed:
<
<

Start the access tool

>
>

Access tool for the ROOT files

 
Added:
>
>
For the 13 and 14 TeV runs we are working on an update of the access tool, which will not be compatible with the old ROOT files. We keep the old access tool for compatibility with the 7 and 8TeV ROOT files.
  • Access tool version 0.5 (for 7 and 8 TeV): Download the header file and the implementation file. For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4.
 To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.
root -l
Line: 79 to 82
 test.Give_XsecUnc_pdfalphas68up_ggFA(120,30) test.Give_XsecUnc_pdfalphas68down_ggFA(120,30) ...
Deleted:
<
<
 
Added:
>
>
  • Access tool version 1.0 (for (8,) 13 and 14 TeV): to be released.
 
Changed:
<
<

ROOT histograms: new MSSM benchmark scenarios

>
>

ROOT histograms: MSSM benchmark scenarios for (8,) 13 and 14 TeV - Access tool version 1.0

  Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the
Line: 90 to 93
 M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
arXiv:1302.7033
Added:
>
>
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=0.5 and 60.
ROOT histograms for 13 and 14 TeV as well as for the low-tan(β)-high scenario/hMSSM are on the way.

Scenarios named in green are obtained with the following setup:
FeynHiggs 2.10.2 with default flags + SusHi 1.4.1 + bbH (4FS) (including Yt*Yb terms)

  • ggH choices:
    • μ_R=μ_F=m_Phi/2.
    • Scale uncertainties: Seven combination of scales according to μ_R=μ_F={m_Phi/4,m_Phi/2,m_Phi} with the constraint 1/2 ≤ μ_R/μ_F ≤ 2
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass
  • bbH (5FS) choices:
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale uncertainties: Seven combination of scales according to μ_R={m_Phi/2,m_Phi,2m_Phi} and μ_F={m_Phi/8,m_Phi/4,m_Phi/2} with the constraint 2 ≤ μ_R/μ_F ≤ 8
    • PDF(+α_s) uncertainties: obtained for a SM Higgs boson with corresponding mass
  • For the SM input to FeynHiggs and SusHi we refer to the bottom of the page.

ROOT histograms: MSSM benchmark scenarios for 7 and 8 TeV - Access tool version 0.5

 The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
Deleted:
<
<
ROOT histograms for 13 and 14 TeV as well as for a scenario with high SUSY masses in combination with low tan(β) are on the way.
 
Line: 163 to 189
  Please use v5 of the access tool: header file and implementation file.
Changed:
<
<

ROOT histograms: 'traditional mhmax' benchmark scenario

>
>

ROOT histograms: 'traditional mhmax' benchmark scenario - Access tool version 0.4

  Subsequently you may find the numbers for the 'traditional mhmax' scenario, which is defined by the parameter choice:
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
Line: 280 to 306
 
Mtop 172.5 GeV
mb(mb) MSbar 4.213 GeV
α_S(MZ) 0.119
Added:
>
>
   
SusHi 1.4.1 Standard Model parameters
α_S(MZ) 0.119 / PDF value
1/α_EW(MZ) 127.67 / fictious value to obtain mW=80.398 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
mc(mc) MSbar 1.28 GeV
mb(mb) MSbar 4.16 GeV
Mbottom^pole 4.75 GeV
Mtop^pole 172.5 GeV
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl

FeynHiggs 2.10.2 with default flags
Standard Model parameters
α_S(MZ) 0.119
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
MW 80.398 GeV
mc(mc) MSbar 1.28 GeV
mb(mb) MSbar 4.16 GeV
Mtop^pole 172.5 GeV
 
Line: 357 to 405
 
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332562" name="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" path="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" size="1414511" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_ataueq0_mu2000.root" attr="" comment="tauphobic scenario with A_tau=0 and mu=2000GeV" date="1419432988" name="tauphobic_7TeV_ataueq0_mu2000.root" path="tauphobic_7TeV_ataueq0_mu2000.root" size="14292492" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_ataueq0_mu2000.root" attr="" comment="tauphobic scenario with A_tau=0 and mu=2000GeV" date="1419433114" name="tauphobic_8TeV_ataueq0_mu2000.root" path="tauphobic_8TeV_ataueq0_mu2000.root" size="14283291" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="mhmodp_mu500_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875786" name="mhmodp_mu500_8TeV.root" path="mhmodp_mu500_8TeV.root" size="11797247" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu1000_8TeV.root" path="mhmodp_mu1000_8TeV.root" size="11614545" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-200_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-200_8TeV.root" path="mhmodp_mu-200_8TeV.root" size="11704522" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-500_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-500_8TeV.root" path="mhmodp_mu-500_8TeV.root" size="11708284" user="sliebler" version="1"
META FILEATTACHMENT attachment="mhmodp_mu-1000_8TeV.root" attr="" comment="mhmodp scenario for 8TeV with different values of mu" date="1429875787" name="mhmodp_mu-1000_8TeV.root" path="mhmodp_mu-1000_8TeV.root" size="8579361" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 702015-02-24 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 195 to 195
  To read these files please use the old tool (v4): header file and implementation file.
Added:
>
>

Discussion of MSSM scenarios with low tan(beta) and Heavy SUSY

See dedicated twiki page here.

 

Some consideration on h/H/A ->tau tau (xs * BR)

This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.

Revision 692015-01-05 - TrevorVickey

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 8 to 8
  In case of questions or problems, please report them to all the conveners.
Changed:
<
<
>
>
 

Revision 682014-12-24 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 128 to 128
 
Changed:
<
<
    • The tauphobic scenario with A_τ=0 and μ=2000GeV is on the way.
>
>
 
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed):
Line: 349 to 351
 
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332561" name="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" path="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" size="1415400" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332561" name="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" path="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" size="14362150" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332562" name="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" path="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" size="1414511" user="sliebler" version="1"
Added:
>
>
META FILEATTACHMENT attachment="tauphobic_7TeV_ataueq0_mu2000.root" attr="" comment="tauphobic scenario with A_tau=0 and mu=2000GeV" date="1419432988" name="tauphobic_7TeV_ataueq0_mu2000.root" path="tauphobic_7TeV_ataueq0_mu2000.root" size="14292492" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_ataueq0_mu2000.root" attr="" comment="tauphobic scenario with A_tau=0 and mu=2000GeV" date="1419433114" name="tauphobic_8TeV_ataueq0_mu2000.root" path="tauphobic_8TeV_ataueq0_mu2000.root" size="14283291" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 672014-12-22 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Revision 662014-11-18 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 123 to 123
 

  • tauphobic
Changed:
<
<
    • Please find subsequently the tauphobic scenario with A_τ=A_t and μ=2000GeV, available since 18.11.2014:
>
>
    • Please find below the tauphobic scenario with A_τ=A_t and μ=2000GeV, available since 18.11.2014:
 
Changed:
<
<
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Subsequently you may find the inconsistent(!) ROOT histograms for comparison, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed.):
>
>
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Below you can find for comparison the inconsistent (!) ROOT histograms, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed):
 

Revision 652014-11-18 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 122 to 122
 
Changed:
<
<
  • tauphobic (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed.)
>
>
  • tauphobic
 
    • Please find subsequently the tauphobic scenario with A_τ=A_t and μ=2000GeV, available since 18.11.2014:
Changed:
<
<
>
>
 
    • The tauphobic scenario with A_τ=0 and μ=2000GeV is on the way.
Changed:
<
<
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Subsequently you may find the inconsistent(!) ROOT histograms for comparison, which include the official numbers for the tauphobic scenario between March and November 2014:
>
>
    • The tauphobic scenario originally suffered from an inconsistent choice of μ between cross sections (μ=2000GeV) and branching ratios (μ=500GeV). Subsequently you may find the inconsistent(!) ROOT histograms for comparison, which include the official numbers for the tauphobic scenario between March and November 2014 (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed.):
 
Line: 345 to 345
 
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149989" name="tauphobic_7TeV_tanbLow.root" path="tauphobic_7TeV_tanbLow.root" size="1437590" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149988" name="tauphobic_8TeV_tanbHigh.root" path="tauphobic_8TeV_tanbHigh.root" size="15643285" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149968" name="tauphobic_8TeV_tanbLow.root" path="tauphobic_8TeV_tanbLow.root" size="1437001" user="monicava" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" path="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" size="14550697" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" path="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" size="1415400" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" path="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" size="14362150" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" path="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" size="1414511" user="sliebler" version="1"
>
>
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332561" name="tauphobic_7TeV_tanbHigh_ataueqat_mu2000.root" path="tauphobic_7TeV_tanbHigh_ataueqat_mu2000.root" size="14550697" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332561" name="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" path="tauphobic_7TeV_tanbLow_ataueqat_mu2000.root" size="1415400" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332561" name="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" path="tauphobic_8TeV_tanbHigh_ataueqat_mu2000.root" size="14362150" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416332562" name="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" path="tauphobic_8TeV_tanbLow_ataueqat_mu2000.root" size="1414511" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 642014-11-18 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 122 to 122
 
Changed:
<
<
  • tauphobic (BRs at tan(β)=7 and tan(β)=8 have a numerical instability. Interpolation needed.
    Due to confusion with the choice of μ updates are on the way. Stay tuned.)
>
>
 
Line: 335 to 341
 
META FILEATTACHMENT attachment="out.lightstopmod-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634071" name="out.lightstopmod-7TeV-tanbLow-nnlo.root" path="out.lightstopmod-7TeV-tanbLow-nnlo.root" size="1218162" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1394634070" name="out.lightstopmod-8TeV-tanbHigh-nnlo.root" path="out.lightstopmod-8TeV-tanbHigh-nnlo.root" size="17265776" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634047" name="out.lightstopmod-8TeV-tanbLow-nnlo.root" path="out.lightstopmod-8TeV-tanbLow-nnlo.root" size="1217313" user="monicava" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh.root" attr="" comment="" date="1395150012" name="tauphobic_7TeV_tanbHigh.root" path="tauphobic_7TeV_tanbHigh.root" size="15899280" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow.root" attr="" comment="" date="1395149989" name="tauphobic_7TeV_tanbLow.root" path="tauphobic_7TeV_tanbLow.root" size="1437590" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh.root" attr="" comment="" date="1395149988" name="tauphobic_8TeV_tanbHigh.root" path="tauphobic_8TeV_tanbHigh.root" size="15643285" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow.root" attr="" comment="" date="1395149968" name="tauphobic_8TeV_tanbLow.root" path="tauphobic_8TeV_tanbLow.root" size="1437001" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395150012" name="tauphobic_7TeV_tanbHigh.root" path="tauphobic_7TeV_tanbHigh.root" size="15899280" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149989" name="tauphobic_7TeV_tanbLow.root" path="tauphobic_7TeV_tanbLow.root" size="1437590" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149988" name="tauphobic_8TeV_tanbHigh.root" path="tauphobic_8TeV_tanbHigh.root" size="15643285" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow.root" attr="" comment="inconsistent tauphobic scenario with mu=2000GeV in XS and mu=500GeV in BRs, A_tau=A_top, used until 18.11.2014" date="1395149968" name="tauphobic_8TeV_tanbLow.root" path="tauphobic_8TeV_tanbLow.root" size="1437001" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" path="tauphobic_7TeV_tanbHigh_atabatau_mu2000.root" size="14550697" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" path="tauphobic_7TeV_tanbLow_atabatau_mu2000.root" size="1415400" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" path="tauphobic_8TeV_tanbHigh_atabatau_mu2000.root" size="14362150" user="sliebler" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" attr="" comment="tauphobic scenario with A_tau=A_top and mu=2000GeV" date="1416318569" name="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" path="tauphobic_8TeV_tanbLow_atabatau_mu2000.root" size="1414511" user="sliebler" version="1"
 
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 632014-11-17 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 10 to 10
 
Changed:
<
<
>
>
  Don't forget to remove 'SPAMNOT' in the email addresses before sending.

Revision 622014-11-14 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 90 to 90
 M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
arXiv:1302.7033
Added:
>
>
The scans in the m_A-tan(β)-plane have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60. For lower values of tan(β) between 0.5 and 0.9 seperate ROOT histograms are available. Differences with respect to this procedure are highlighted.
 ROOT histograms for 13 and 14 TeV as well as for a scenario with high SUSY masses in combination with low tan(β) are on the way.

  • mhmodm
Line: 160 to 161
 μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tan(β) plane.
Changed:
<
<
Two complete scans (for 7 TeV and for 14 TeV) of the m_A-tan(β) plane are available. The scans have been made between m_A=90 GeV and m_A=1000 GeV in steps of 1 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan) in steps of 1. For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. The quantities available in these are:
>
>
We present the ROOT histograms produced by the MSSM subgroup at an early stage in the m_A-tan(β)-plane for 7 TeV and for 14 TeV. The scans have been made between m_A=90 GeV and m_A=1000 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan). For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. They are kept for documentation:
 
Changed:
<
<
  • masses of the scalar bosons h and H (calculated using FeynHiggs 2.7.4)
  • Cross sections for b-associated h/H/A production in the 5 flavour scheme (NNLO QCD), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4.
  • Cross sections for b-associated h/H/A production in the 4 flavour scheme (NLO QCD) and scale uncertainties using MSTW2008. PDF uncertainties are not available. ( not yet for 14 TeV; Please note that as a consequence, the Santander-matching member function from the mssm_xs_tools.C macro will NOT return meaningful 14 TeV cross section numbers!)
  • Cross sections for gluon-gluon-fusion h/H/production (NLO QCD (HIGLU) for b-loop and t-b-interference, top-loop only is corrected to NNLO QCD (ggh@nnlo)), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above). ( * PDF uncertainties not yet for 14 TeV.*) Renormalization and Factorization scale: m_Phi
    Scale uncertainty: variation by a factor 2
  • PRELIMINARY AND SUBJECT TO BR subgroup approval: Branching fractions of h/H/A to bottom quarks, tau leptons and muons from FeynHiggs 2.7.4.

The ROOT files can be downloaded here for 7 TeV and here for 14 TeV.

>
>
FeynHiggs 2.7.4 with default flags + HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
  • out.mhmax_7.root: mhmax, 7 TeV
  • out.mhmax_7.root: mhmax, 14 TeV (no bbh 4FS and thus no Santander-matched XS and no PDF uncertainties! You obtain unreasonable results by the access tool!)
 
Changed:
<
<
  • HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
    ggH scale: μ_R=μ_F=m_Phi. Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
    bbH 5FS scale: μ_R= m_Phi; μ_F=0.25*m_Phi. Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
>
>
For 7 and 8 TeV please make use of the subsequent ROOT histograms:
HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
  • bbH (5FS) scale choices:
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
 
Changed:
<
<
>
>
 
Added:
>
>
The scenario is availabe for other (negative) values of μ as well, see attachments!
 To read these files please use the old tool (v4): header file and implementation file.

Some consideration on h/H/A ->tau tau (xs * BR)

Revision 612014-11-10 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 6 to 6
 

Group Members

Added:
>
>
In case of questions or problems, please report them to all the conveners.
 
Added:
>
>
Don't forget to remove 'SPAMNOT' in the email addresses before sending.
 

Bibliography

If you use numbers provided on this webpage you must cite the following papers:
  • HIGLU program

Revision 602014-11-10 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 12 to 12
 

Bibliography

If you use numbers provided on this webpage you must cite the following papers:
Changed:
<
<
  • Higlu program
>
>
  • HIGLU program
 
    • Spira:1995mt
  • SusHi program
    • Harlander:2012pb
Line: 57 to 57
 Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
santandermatching-hks.pdf: Description of Santander matching procedure for inclusive pp-->H(bb) cross-section
Changed:
<
<
The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Download the header file and the implementation file. For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. The current version of the access tool is v5.
>
>
The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Download the header file and the implementation file. For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. The current version of the access tool is v5 provided by Monica Vazquez Acosta, Trevor Vickey, Markus Warsinsky and Felix Frensch.
 

Start the access tool

Line: 199 to 199
  4b) SUSY-QCD corrections:
Changed:
<
<
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Delta_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Delta_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)
>
>
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Δ_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Δ_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)
 
Changed:
<
<
5) Delta_b: We know exactly where to place Delta_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)
>
>
5) Δ_b: We know exactly where to place Δ_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)
  6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)
Line: 219 to 219
 

Choice of input parameters

Added:
>
>
All SusHi runs make use of the naive Δ_b resummation (Y_b -> Y_b/(1+ Δ_b)) using the Δ_b from FeynHiggs for gluon fusion and the full resummation for bottom-quark annihilation (5FS) (see SusHi manual). They include NLO squark contributions expanded in heavy SUSY masses and electroweak corrections by light quarks.

 
HIGLU Standard Model parameters
Changed:
<
<
aS (MZ) 0.12018, 2 loop
>
>
α_S(MZ) 0.12018, 2 loop
 
Lambda_QCD^(5) 226 MeV
PDF MSTW2008nlo68cl
Mcharm 1.40 GeV
Line: 237 to 240
 
Mtop 172.5 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
Added:
>
>
   
SusHi 1.0.6 Standard Model parameters
α_S(MZ) 0.119 / PDF value
PDF (NLO) MSTW2008nlo68cl
PDF (NNLO) MSTW2008nnlo68cl
Mcharm 1.40 GeV
Mbottom 4.75 GeV
Mtop 172.5 GeV
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
 
FeynHiggs 2.7.4 and 2.8.6 with default flags
Standard Model parameters
Mtop 172.5 GeV
mb(mb) MSbar 4.213 GeV
Changed:
<
<
aS(MZ) 0.119
>
>
α_S(MZ) 0.119
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"

Revision 592014-11-08 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 47 to 47
 
  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • cross sections for b-associated h/H/A production in the 4 flavour scheme (4FS) (NLO QCD) including scale uncertainties.
Changed:
<
<
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with squark (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons.
>
>
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with SUSY QCD (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons, see also BR subgroup.
  The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available:
Line: 80 to 80
 

ROOT histograms: new MSSM benchmark scenarios

Changed:
<
<
Subsequently you find root files for the MSSM benchmark scenarios defined in:
>
>
Subsequently you find ROOT histograms for the MSSM benchmark scenarios defined in:
 "MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the Discovery of a Higgs-like Particle"
M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
Line: 89 to 89
 ROOT histograms for 13 and 14 TeV as well as for a scenario with high SUSY masses in combination with low tan(β) are on the way.

  • mhmodm
Changed:
<
<
>
>
 
  • mhmodp
Changed:
<
<

>
>

 
  • lightstau
Changed:
<
<

>
>

 
  • mhmax
Changed:
<
<
>
>
  Scenarios named in red are obtained with the following setup:
FeynHiggs 2.8.6 with default flags + SusHi 1.0.6 + bbH (4FS) scans
  • ggH scale choices:
Changed:
<
<
    • muR=muF=m_Phi.
    • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • bbH (5FS) scale choices:
Changed:
<
<
    • muR= m_Phi, muF=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
  Scenarios named in blue are obtained with the following setup:
HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
Changed:
<
<
    • muR=muF=m_Phi.
    • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
>
>
    • μ_R=μ_F=m_Phi.
    • Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
 
  • bbH (5FS) scale choices:
Changed:
<
<
    • muR= m_Phi, muF=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
    • μ_R= m_Phi, μ_F=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
  Please use v5 of the access tool: header file and implementation file.
Line: 166 to 167
  The ROOT files can be downloaded here for 7 TeV and here for 14 TeV.
Changed:
<
<
  • HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
  • HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
    ggH scale: μ_R=μ_F=m_Phi. Scale variation: 0.5*m_Phi < μ_R, μ_F < 2*m_Phi
    bbH 5FS scale: μ_R= m_Phi; μ_F=0.25*m_Phi. Scale variation: 0.2*m_Phi < μ_R < 5*m_Phi ; 0.1*m_Phi < μ_F < 0.7*m_Phi
 

Revision 582014-11-07 - StefanLiebler

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Group Members

Changed:
<
<
>
>
 

Bibliography

Changed:
<
<
If you use these numbers you must cite the following papers:
>
>
If you use numbers provided on this webpage you must cite the following papers:
 
  • Higlu program
    • Spira:1995mt
  • SusHi program
    • Harlander:2012pb
Changed:
<
<
  • FeynHiggs:
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi
    • Frank:2006yh
>
>
  • FeynHiggs program
    • Heinemeyer:1998yj, Heinemeyer:1998np, Degrassi:2002fi, Frank:2006yh
 
  • ggH@NNLO program
    • Harlander:2002wh
Changed:
<
<
  • ggH: NLO massive
    • Spira:1995rr
  • ggH NNLO: Scalar Higgs
    • Anastasiou:2002yz
    • Ravindran:2003um
  • ggH NNLO: Pseudoscalar Higgs
    • Harlander:2002vv
    • Anastasiou:2002wq
  • bbh@nnlo 5FS program
>
>
  • bbh@nnlo (5FS) program
 
    • Harlander:2003ai
Changed:
<
<
  • NLO bbH 4FS
    • Dittmaier:2003ej
    • Dawson:2003kb
  • Electroweak corrections by light fermions:
    • Aglietti:2004nj
    • Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A:
>
>
  • bbH NLO (4FS)
    • Dittmaier:2003ej, Dawson:2003kb
  • ggH NLO massive
    • Spira:1995rr
  • ggH NNLO for scalar Higgs
    • Anastasiou:2002yz, Ravindran:2003um
  • ggH NNLO for pseudoscalar Higgs
    • Harlander:2002vv, Anastasiou:2002wq
  • Electroweak corrections by light fermions
    • Aglietti:2004nj, Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A
 
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
Line: 46 to 40
 
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH != 0)
Changed:
<
<

Available Xsection scans

>
>

Available benchmark scenarios

 
Changed:
<
<
Two complete scans (for 7 TeV and for 14 TeV) of the mA-tan(beta) plane in the mhmax scenario are available with the numbers produced for the CERN Yellow Report that will soon be published. The scans have been made between mA=90 GeV and mA=1000 GeV in steps of 1 GeV and between tan(beta)=1 and 60 (5 and 70 for the 14 TeV scan) in steps of 1. For very low tan(beta), the scan is done between tan(beta)=0.5 and 0.9 in steps of 0.1. The scanned quantities are available in form of 2 dimensional ROOT histograms. The quantities available in these are:
>
>
Higgs masses, cross sections (including uncertainties) and branching ratios for different MSSM benchmark scenarios are provided in terms of 2 dimensional ROOT histograms usually scanning over the m_A-tan(β) plane. In detail the histograms contain:
 
Changed:
<
<
  • masses of the scalar bosons h and H (calculated using FeynHiggs 2.7.4 with Mtop=172.5 GeV, mb(mb)=4.213 GeV, alphas(MZ)=0.119, MSUSY=1000 GeV, Xt=2000 GeV, M2=200 GeV, mu=200 GeV, M3=800 GeV)
  • Cross sections for b-associated h/H/A production in the 5 flavour scheme (NNLO QCD), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above).
  • Cross sections for b-associated h/H/A production in the 4 flavour scheme (NLO QCD) and scale uncertainties using MSTW2008. PDF uncertainties are not available. ( not yet for 14 TeV; Please note that as a consequence, the Santander-matching member function from the mssm_xs_tools.C macro will NOT return meaningful 14 TeV cross section numbers!)
  • Cross sections for gluon-gluon-fusion h/H/production (NLO QCD (HIGLU) for b-loop and t-b-interference, top-loop only is corrected to NNLO QCD (ggh@nnlo)), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above). ( !PDF uncertainties not yet for 14 TeV.)
  • PRELIMINARY AND SUBJECT TO BR subgroup approval: Branching fractions of h/H/A to bottom quarks, tau leptons and muons from FeynHiggs 2.7.4.
The ROOT files can be downloaded here for 7 TeV and here for 14 TeV. The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Download the header file and the implementation file. For infomation about the usage , please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4.
>
>
  • masses of the scalar bosons h and H (The pseudoscalar mass is fixed by m_A).
  • cross sections for b-associated h/H/A production in the 5 flavour scheme (5FS) (NNLO QCD) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • cross sections for b-associated h/H/A production in the 4 flavour scheme (4FS) (NLO QCD) including scale uncertainties.
  • cross sections for gluon-gluon fusion h/H/A production (top at NNLO QCD, bottom and top-bottom interference at NLO QCD, partially with squark (SQCD) and electroweak (EW) contributions) including scale and PDF(+α_s) uncertainties using MSTW2008.
  • branching ratios of h/H/A to bottom quarks, tau leptons and muons.

The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available:
"Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach"
R. Harlander, M. Krämer, and M. Schumacher
Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.

santandermatching-hks.pdf: Description of Santander matching procedure for inclusive pp-->H(bb) cross-section

 
Changed:
<
<

How to run the tool

>
>
The structure of the histograms is rather complicated. To ensure that the numbers are extracted properly, a simple C++ class is provided. Download the header file and the implementation file. For infomation about the usage, please consult the header file, or use the help() method of the class, which will explain all available methods. On initialization with an input file, some information on the used MSSM parameters is also printed out on screen. The accessor tool has been tested with ROOT stand-alone and was tested to be compiled stand-alone GCC4.4. The current version of the access tool is v5.
 
Changed:
<
<
Example on how to run the tool
>
>

Start the access tool

To work with the access tool you have to include the corresponding C++ class. help() gives you a list of the available commands.

 
root -l
.L mssm_xs_tools.C
Line: 76 to 78
 
Changed:
<
<

Xsection scan files: new scenarios

>
>

ROOT histograms: new MSSM benchmark scenarios

 
Added:
>
>
Subsequently you find root files for the MSSM benchmark scenarios defined in:
"MSSM Higgs Boson Searches at the LHC: Benchmark Scenarios after the Discovery of a Higgs-like Particle"
M. Carena, S. Heinemeyer, O. Stål, C.E.M. Wagner, G. Weiglein
arXiv:1302.7033

ROOT histograms for 13 and 14 TeV as well as for a scenario with high SUSY masses in combination with low tan(β) are on the way.

 
Added:
>
>

Scenarios named in red are obtained with the following setup:
FeynHiggs 2.8.6 with default flags + SusHi 1.0.6 + bbH (4FS) scans

  • ggH scale choices:
    • muR=muF=m_Phi.
    • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
  • bbH (5FS) scale choices:
    • muR= m_Phi, muF=0.25*m_Phi.
    • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
 
Changed:
<
<
  • SuSHi + 4FS bbH scans
    • ggH scale:
>
>
Scenarios named in blue are obtained with the following setup:
HIGLU + ggH@NNLO + bbH@NNLO (5FS) + bbH (4FS) scans
  • ggH scale choices:
 
      • muR=muF=m_Phi.
      • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
Changed:
<
<
    • bbH 5FS scale:
>
>
  • bbH (5FS) scale choices:
 
      • muR= m_Phi, muF=0.25*m_Phi.
      • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
Changed:
<
<

>
>
Please use v5 of the access tool: header file and implementation file.
 
Changed:
<
<

The access tool has been updated (v5) to provide functions to query the combined cross section, pdf and scale errors for the new SusHi scan files.

The new tool is in Download the header file and the implementation file

The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available: "Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach" by R. Harlander, M. Krämer, and M. Schumacher, Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.

Xsection scan files: traditional mhmax

>
>

ROOT histograms: 'traditional mhmax' benchmark scenario

Subsequently you may find the numbers for the 'traditional mhmax' scenario, which is defined by the parameter choice:
μ = 200GeV, M_Susy = 1000GeV, X_t = 2000GeV, M_2 = 200GeV, M_3 = 800GeV
It is known to provide a light Higgs with m_h>126GeV in large parts of the m_A-tan(β) plane.

Two complete scans (for 7 TeV and for 14 TeV) of the m_A-tan(β) plane are available. The scans have been made between m_A=90 GeV and m_A=1000 GeV in steps of 1 GeV and between tan(β)=1 and 60 (5 and 70 for the 14 TeV scan) in steps of 1. For very low tan(β), the scan is done between tan(β)=0.5 and 0.9 in steps of 0.1. The quantities available in these are:

  • masses of the scalar bosons h and H (calculated using FeynHiggs 2.7.4)
  • Cross sections for b-associated h/H/A production in the 5 flavour scheme (NNLO QCD), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4.
  • Cross sections for b-associated h/H/A production in the 4 flavour scheme (NLO QCD) and scale uncertainties using MSTW2008. PDF uncertainties are not available. ( not yet for 14 TeV; Please note that as a consequence, the Santander-matching member function from the mssm_xs_tools.C macro will NOT return meaningful 14 TeV cross section numbers!)
  • Cross sections for gluon-gluon-fusion h/H/production (NLO QCD (HIGLU) for b-loop and t-b-interference, top-loop only is corrected to NNLO QCD (ggh@nnlo)), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above). ( * PDF uncertainties not yet for 14 TeV.*) Renormalization and Factorization scale: m_Phi
    Scale uncertainty: variation by a factor 2
  • PRELIMINARY AND SUBJECT TO BR subgroup approval: Branching fractions of h/H/A to bottom quarks, tau leptons and muons from FeynHiggs 2.7.4.
 
Changed:
<
<
To read these files please use the old tool Download the header file and the implementation file
>
>
The ROOT files can be downloaded here for 7 TeV and here for 14 TeV.

To read these files please use the old tool (v4): header file and implementation file.

 

Some consideration on h/H/A ->tau tau (xs * BR)

This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.

Changed:
<
<
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(beta)) points (which is not so useful).
>
>
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(β)) points (which is not so useful).
  That being said, we recommend the following:
Line: 177 to 205
 6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)

Tools and Programs

Changed:
<
<
>
>
If you aim to get cross sections and branching ratios for other scenarios than the ones on this webpage, you may use the following codes, which were also used to calculate the provided numbers:

  • Higgs mass calculation and branching ratios: FeynHiggs:
  • Gluon fusion cross section: ggh@nnlo
  • Gluon fusion cross section: HIGLU
  • Bottom-quark annihilation (5FS) cross section: bbh@nnlo
  • Gluon fusion (incl. SQCD and EW) and bottom-quark annihilation (5FS) cross section: SusHi
 

Meetings

Changed:
<
<

ggH: Input Parameters

Renormalization and Factorization scale: M_Higgs
Scale uncertainty: variation by a factor 2

>
>

Choice of input parameters

 
HIGLU Standard Model parameters
aS (MZ) 0.12018, 2 loop
Line: 208 to 237
 
GF 1.16637 10-5 GeV-2
MZ 91.1876 GeV
Changed:
<
<
FeynHiggs 2.8.6
  • Default flags
  • Standard Model parameters
>
>
FeynHiggs 2.7.4 and 2.8.6 with default flags
Standard Model parameters
 
Mtop 172.5 GeV
mb(mb) MSbar 4.213 GeV
aS(MZ) 0.119
Deleted:
<
<
  • Scenarios
    • mhmax
MT 172.5
MB 4.213
AlfasMZ 0.119
Abs(MUE) 200
Arg(MUE) 0
MSusy 1000
Abs(Xt) 2000
Arg(Xt) 0
Abs(M_2) 200
Arg(M_2) 0
Abs(M_3) 800.0
Arg(M_3) 0
MA0 XXX_mA
TB XXX_tanb
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"

Revision 572014-11-04 - ReiTanaka

Line: 1 to 1
 
META TOPICPARENT name="LHCHXSWG3"

MSSM Neutral Higgs

Line: 299 to 299
 
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow.root" attr="" comment="" date="1395149989" name="tauphobic_7TeV_tanbLow.root" path="tauphobic_7TeV_tanbLow.root" size="1437590" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh.root" attr="" comment="" date="1395149988" name="tauphobic_8TeV_tanbHigh.root" path="tauphobic_8TeV_tanbHigh.root" size="15643285" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow.root" attr="" comment="" date="1395149968" name="tauphobic_8TeV_tanbLow.root" path="tauphobic_8TeV_tanbLow.root" size="1437001" user="monicava" version="1"
Changed:
<
<
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"
>
>
META TOPICMOVED by="tanaka" date="1415123449" from="LHCPhysics.LHXHXSWGMSSMNeutral" to="LHCPhysics.LHCHXSWGMSSMNeutral"

Revision 552014-08-17 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 181 to 181
 
Added:
>
>
 

Meetings

Revision 542014-07-04 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 262 to 262
 
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=-200, 7 TeV, lowest tanbeta=1" date="1328106516" name="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" path="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" size="29800667" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[1,70]; Note no BRs for WW or gamma-gamma" date="1343391609" name="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" path="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" size="31624335" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[0.5,0.9]; Note no BRs for WW or gamma-gamma" date="1350290547" name="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" path="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" size="2414466" user="tvickey" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169782" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169781" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169781" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169779" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169779" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169776" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="" date="1404470880" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17522635" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="" date="1404470848" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1564278" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="" date="1404470845" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17509100" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="" date="1404470826" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1563821" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="" date="1404470825" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17542756" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="" date="1404470805" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1562873" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="" date="1404470775" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1562344" user="monicava" version="2"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="" date="1404470802" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17530955" user="monicava" version="2"
 
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027113" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027079" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027143" name="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" size="29890978" user="monicava" version="1"

Revision 532014-06-10 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 110 to 110
 
Changed:
<
<
  • lightstopmod ( Note: tanbeta below 0.7 is not used due to problematic two-loop stop mas corrections)
>
>
  • lightstopmod ( Note: tanbeta below 0.7 is not used due to problematic two-loop stop mas corrections
    SUSY QCD corrections above MA> 600 GeV are not reliable)
 
Line: 279 to 280
 
META FILEATTACHMENT attachment="out.lightstau1-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027227" name="out.lightstau1-7TeV-tanbLow-nnlo.root" path="out.lightstau1-7TeV-tanbLow-nnlo.root" size="1543459" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstau1-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027226" name="out.lightstau1-8TeV-tanbHigh-nnlo.root" path="out.lightstau1-8TeV-tanbHigh-nnlo.root" size="17335195" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstau1-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027206" name="out.lightstau1-8TeV-tanbLow-nnlo.root" path="out.lightstau1-8TeV-tanbLow-nnlo.root" size="1542840" user="monicava" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="out.lowmH-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027343" name="out.lowmH-7TeV-tanbHigh-nnlo.root" path="out.lowmH-7TeV-tanbHigh-nnlo.root" size="3587603" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lowmH-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027340" name="out.lowmH-8TeV-tanbHigh-nnlo.root" path="out.lowmH-8TeV-tanbHigh-nnlo.root" size="3583786" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="out.lowmH-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1402409316" name="out.lowmH-7TeV-tanbHigh-nnlo.root" path="out.lowmH-7TeV-tanbHigh-nnlo.root" size="3586100" user="monicava" version="2"
META FILEATTACHMENT attachment="out.lowmH-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1402409316" name="out.lowmH-8TeV-tanbHigh-nnlo.root" path="out.lowmH-8TeV-tanbHigh-nnlo.root" size="3582579" user="monicava" version="2"
 
META FILEATTACHMENT attachment="out.mhmodm-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027338" name="out.mhmodm-7TeV-tanbHigh-nnlo.root" path="out.mhmodm-7TeV-tanbHigh-nnlo.root" size="17353727" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027321" name="out.mhmodm-7TeV-tanbLow-nnlo.root" path="out.mhmodm-7TeV-tanbLow-nnlo.root" size="1545329" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027320" name="out.mhmodm-8TeV-tanbHigh-nnlo.root" path="out.mhmodm-8TeV-tanbHigh-nnlo.root" size="17340182" user="monicava" version="1"

Revision 522014-04-29 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Revision 512014-04-29 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 42 to 42
 
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
Changed:
<
<
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0)
>
>
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA !=0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH !=0)
 

Available Xsection scans

Revision 502014-04-29 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 9 to 9
 
Added:
>
>

Bibliography

If you use these numbers you must cite the following papers:
  • Higlu program
    • Spira:1995mt
  • SusHi program
    • Harlander:2012pb
  • FeynHiggs:
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi
    • Frank:2006yh
  • ggH@NNLO program
    • Harlander:2002wh
  • ggH: NLO massive
    • Spira:1995rr
  • ggH NNLO: Scalar Higgs
    • Anastasiou:2002yz
    • Ravindran:2003um
  • ggH NNLO: Pseudoscalar Higgs
    • Harlander:2002vv
    • Anastasiou:2002wq
  • bbh@nnlo 5FS program
    • Harlander:2003ai
  • NLO bbH 4FS
    • Dittmaier:2003ej
    • Dawson:2003kb
  • Electroweak corrections by light fermions:
    • Aglietti:2004nj
    • Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A:
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0)
 

Available Xsection scans

Two complete scans (for 7 TeV and for 14 TeV) of the mA-tan(beta) plane in the mhmax scenario are available with the numbers produced for the CERN Yellow Report that will soon be published. The scans have been made between mA=90 GeV and mA=1000 GeV in steps of 1 GeV and between tan(beta)=1 and 60 (5 and 70 for the 14 TeV scan) in steps of 1. For very low tan(beta), the scan is done between tan(beta)=0.5 and 0.9 in steps of 0.1. The scanned quantities are available in form of 2 dimensional ROOT histograms. The quantities available in these are:

Line: 39 to 76
 
Changed:
<
<

Xsection scan files

>
>

Xsection scan files: new scenarios

 
Deleted:
<
<
If you use these numbers you must cite the following papers: link
  • SusHi:
    • Harlander:2012pb
  • ggh@nnlo:
    • Harlander:2002wh
  • bbh@nnlo:
    • Harlander:2003ai
  • Electroweak corrections by light fermions:
    • Aglietti:2004nj
    • Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A:
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top/bottom)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0)
  • FeynHiggs:
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi
    • Frank:2006yh
 
  • SuSHi + 4FS bbH scans
    • ggH scale:
Line: 118 to 135
 
Added:
>
>

Xsection scan files: traditional mhmax

To read these files please use the old tool Download the header file and the implementation file

 

Some consideration on h/H/A ->tau tau (xs * BR)

This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.

Revision 492014-03-23 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 57 to 57
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0)
Changed:
<
<
>
>
  • FeynHiggs:
 
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi

Revision 482014-03-23 - PietroSlavich

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 52 to 53
 
    • Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A:
    • Harlander:2004tp (NLO-stop scalar mh=0)
Changed:
<
<
    • Harlander:2005rq (NLO-top)
>
>
    • Harlander:2005rq (NLO-top/bottom)
 
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
Changed:
<
<
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0) ---FeynHiggs:
>
>
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0)
  • FeynHiggs:
 
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi
Line: 65 to 66
 
  • SuSHi + 4FS bbH scans
    • ggH scale:
      • muR=muF=m_Phi.
Changed:
<
<
      • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
>
>
      • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
 
    • bbH 5FS scale:
      • muR= m_Phi, muF=0.25*m_Phi.
Changed:
<
<
      • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
      • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
 
Line: 104 to 105
 
Changed:
<
<
  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
 
Line: 118 to 114
  The new tool is in Download the header file and the implementation file
Changed:
<
<
The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available: "Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach" by R. Harlander, M. Krämer, and M. Schumacher, Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
>
>
The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting). The write-up of the Santander-Macthing is available: "Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach" by R. Harlander, M. Krämer, and M. Schumacher, Please refer to CERN-PH-TH/2011-134 – FR-PHENO-2011-009 – TTK-11-17 – WUB/11-04 and this webpage.
 
Changed:
<
<
 
H(bb) cross-section
>
>
 
Added:
>
>

Some consideration on h/H/A ->tau tau (xs * BR)

 
Added:
>
>
This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.
 
Added:
>
>
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(beta)) points (which is not so useful).
 
Changed:
<
<

Some consideration on h/H/A ->tau tau (xs * BR)

>
>
That being said, we recommend the following:
 
Changed:
<
<
This is a typical case where the YR does not give the answer in terms of explicit numbers, but in the form of a procedure that should be followed: input, central values, THU and PU and scale errors with combinations.
>
>
2a) As far as the PDF error is concerned, the simplest way out is to determine the PDF error on the sum of different production mechanisms (in the usual way), rather than on each of the cross sections separately. Then the correlation is automatically taken into account. (comment by S. Forte)
 
Changed:
<
<
We do not think that there is a case for tabulating all XS*BR, users can do that. It is practically impossible to tabulate the full set of results in MSSM, unless one represents typical (M_A, tan(beta)) points (which is not so useful).
>
>
2b) Therefore, in combining ggF and bbH one has to take into full account one caveat: since the b-PDFs so far are only contructed as being purely perturbative, i.e. fully generated by g -> bb spitting at LL level, a sum of the PDF uncertainties - linear as well as quadratic - seems to double count the gluon PDF uncertainties. Thus, one would prefer a scheme in which the PDF uncertainties of the sum ggF+bbH are computed as those to a single observable. The situation will only become different once there are data on b-PDFs... Noone knows until now if there is a non-perturbative intrinsic b contribution or not, i.e. whether the non-perturbative component is sizeable or not. We believe that 4-5 GeV as the input scale is deep in the perturbative regime. (comment by M. Spira)
 
Changed:
<
<
That being said, we recommend the following:
>
>
2b) To summarize: we recommend to do once the check 2a) and compare the result with the simple addition in quadrature: it could well be that even though in principles the g and b are correlated, in practice the simple sum in quadrature works well. (comment by S. Forte)

3) Typically we vary scales in some range (like M_H/2 to 2M_H), but we never start thinking about it as if that represents the true uncertainty. It only represents `the best we can do'. But this should be clear from the YR.

The scale variation follows the recommendation of Harlander/Kilgore. It serves as a conservative estimate of the scale dependence for this process. (comment by M. Spira and M. Warsinsky)

4a) SUSY-QCD corrections: Statements that SUSY-QCD corrections are just of this and that size cannot be made, because they strongly depend a) on the scenario, b) on the details how LO is defined.

 
Changed:
<
<
2a) As far as the PDF error is concerned, the simplest way out is to determine the PDF error on the sum of different production mechanisms (in the usual way), rather than on each of the cross sections separately. Then the correlation is automatically taken into account. (comment by S. Forte)

2b) Therefore, in combining ggF and bbH one has to take into full account one caveat: since the b-PDFs so far are only contructed as being purely perturbative, i.e. fully generated by g -> bb spitting at LL level, a sum of the PDF uncertainties - linear as well as quadratic - seems to double count the gluon PDF uncertainties. Thus, one would prefer a scheme in which the PDF uncertainties of the sum ggF+bbH are computed as those to a single observable. The situation will only become different once there are data on b-PDFs... Noone knows until now if there is a non-perturbative intrinsic b contribution or not, i.e. whether the non-perturbative component is sizeable or not. We believe that 4-5 GeV as the input scale is deep in the perturbative regime. (comment by M. Spira)

2b) To summarize: we recommend to do once the check 2a) and compare the result with the simple addition in quadrature: it could well be that even though in principles the g and b are correlated, in practice the simple sum in quadrature works well. (comment by S. Forte)

3) Typically we vary scales in some range (like M_H/2 to 2M_H), but we never start thinking about it as if that represents the true uncertainty. It only represents `the best we can do'. But this should be clear from the YR.

The scale variation follows the recommendation of Harlander/Kilgore. It serves as a conservative estimate of the scale dependence for this process. (comment by M. Spira and M. Warsinsky)

4a) SUSY-QCD corrections: Statements that SUSY-QCD corrections are just of this and that size cannot be made, because they strongly depend a) on the scenario, b) on the details how LO is defined.

To a): The variety of all scenarios is too large and rich for overall statements in the YR. To b): residual corrections typically are small (not like 30% or so) if LO is based on loop-corrected masses of the external Higgs particles and appropriate effective couplings.

>
>
To a): The variety of all scenarios is too large and rich for overall statements in the YR. To b): residual corrections typically are small (not like 30% or so) if LO is based on loop-corrected masses of the external Higgs particles and appropriate effective couplings.
  4b) SUSY-QCD corrections:
Changed:
<
<
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Delta_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Delta_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)

5) Delta_b: We know exactly where to place Delta_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)

6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)

>
>
Concerning the SUSY-QCD corrections to bbH: They are fully accounted for by the Delta_b terms (up to the per-cent level for the remainder). The situation is not completely clear for the 5FS. In the 4FS the residual corrections beyond the Delta_b terms are tiny so that the same should be expected in the 5FS, too. (comment by M. Spira)
 
Added:
>
>
5) Delta_b: We know exactly where to place Delta_b, so there is no uncertainty. Switching it on and off does not quantify any uncertainty. (comment by S. Dittmaier)

6) We do not quote large tables with all uncertainties in the YR since it would require a 2D-scan (and probably produced hundreds of pages). Instead we have put everything in root-files on the Twiki pages. The uncertainties can be accessed easily from there. In addition we had added the BRs to bbbar, tautau and mumu, so xsec*BR is accessible from there. (comment by M. Warsinsky)

 

Tools and Programs

Line: 211 to 156
 

Meetings

Deleted:
<
<
 

ggH: Input Parameters

Changed:
<
<
Renormalization and Factorization scale: M_Higgs
Scale uncertainty: variation by a factor 2
>
>
Renormalization and Factorization scale: M_Higgs
Scale uncertainty: variation by a factor 2
 
HIGLU Standard Model parameters
aS (MZ) 0.12018, 2 loop

Revision 472014-03-23 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 40 to 40
 

Xsection scan files

Added:
>
>
If you use these numbers you must cite the following papers: link
  • SusHi:
    • Harlander:2012pb
  • ggh@nnlo:
    • Harlander:2002wh
  • bbh@nnlo:
    • Harlander:2003ai
  • Electroweak corrections by light fermions:
    • Aglietti:2004nj
    • Bonciani:2010ms
  • (N)NLO (S)QCD corrections for h/H/A:
    • Harlander:2004tp (NLO-stop scalar mh=0)
    • Harlander:2005rq (NLO-top)
    • Degrassi:2010eu (NLO-sbottom scalar)
    • Degrassi:2011vq (NLO-stop/sbottom pseudo mA =0)
    • Degrassi:2012vt (NLO-stop/sbottom scalar mH =0) ---FeynHiggs:
    • Heinemeyer:1998yj
    • Heinemeyer:1998np
    • Degrassi:2002fi
    • Frank:2006yh
 
  • SuSHi + 4FS bbH scans
    • ggH scale:
      • muR=muF=m_Phi.

Revision 462014-03-18 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 38 to 38
 
Changed:
<
<

Available Xsection scans

>
>

Xsection scan files

 
  • SuSHi + 4FS bbH scans
    • ggH scale:
Line: 76 to 76
 
Added:
>
>
 

  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
Line: 239 to 244
 
Deleted:
<
<
 
Deleted:
<
<

 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"

Revision 452014-03-18 - MonicaVazquezAcosta

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META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 239 to 239
 
Added:
>
>

 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools.h" attr="" comment="Access tool: version 0.5" date="1386172658" name="mssm_xs_tools.h" path="mssm_xs_tools.h" size="11337" user="monicava" version="4"
Line: 303 to 311
 
META FILEATTACHMENT attachment="out.lightstopmod-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634071" name="out.lightstopmod-7TeV-tanbLow-nnlo.root" path="out.lightstopmod-7TeV-tanbLow-nnlo.root" size="1218162" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1394634070" name="out.lightstopmod-8TeV-tanbHigh-nnlo.root" path="out.lightstopmod-8TeV-tanbHigh-nnlo.root" size="17265776" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634047" name="out.lightstopmod-8TeV-tanbLow-nnlo.root" path="out.lightstopmod-8TeV-tanbLow-nnlo.root" size="1217313" user="monicava" version="1"
Added:
>
>
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbHigh.root" attr="" comment="" date="1395150012" name="tauphobic_7TeV_tanbHigh.root" path="tauphobic_7TeV_tanbHigh.root" size="15899280" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_7TeV_tanbLow.root" attr="" comment="" date="1395149989" name="tauphobic_7TeV_tanbLow.root" path="tauphobic_7TeV_tanbLow.root" size="1437590" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbHigh.root" attr="" comment="" date="1395149988" name="tauphobic_8TeV_tanbHigh.root" path="tauphobic_8TeV_tanbHigh.root" size="15643285" user="monicava" version="1"
META FILEATTACHMENT attachment="tauphobic_8TeV_tanbLow.root" attr="" comment="" date="1395149968" name="tauphobic_8TeV_tanbLow.root" path="tauphobic_8TeV_tanbLow.root" size="1437001" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 442014-03-13 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 70 to 70
 
Changed:
<
<
  • lightstopmod
>
>
  • lightstopmod ( Note: tanbeta below 0.7 is not used due to problematic two-loop stop mas corrections)
 
Changed:
<
<
>
>
 
Changed:
<
<
>
>
 

Revision 432014-03-13 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 41 to 41
 

Available Xsection scans

  • SuSHi + 4FS bbH scans
Changed:
<
<
ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
>
>
    • ggH scale:
      • muR=muF=m_Phi.
      • Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    • bbH 5FS scale:
      • muR= m_Phi, muF=0.25*m_Phi.
      • Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
 

Revision 422014-03-12 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 66 to 66
 
Added:
>
>

 
  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
Line: 287 to 295
 
META FILEATTACHMENT attachment="out.mhmodp-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027416" name="out.mhmodp-7TeV-tanbLow-nnlo.root" path="out.mhmodp-7TeV-tanbLow-nnlo.root" size="1544001" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027415" name="out.mhmodp-8TeV-tanbHigh-nnlo.root" path="out.mhmodp-8TeV-tanbHigh-nnlo.root" size="17362382" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027398" name="out.mhmodp-8TeV-tanbLow-nnlo.root" path="out.mhmodp-8TeV-tanbLow-nnlo.root" size="1543466" user="monicava" version="1"
Added:
>
>
META FILEATTACHMENT attachment="out.lightstopmod-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1394634094" name="out.lightstopmod-7TeV-tanbHigh-nnlo.root" path="out.lightstopmod-7TeV-tanbHigh-nnlo.root" size="17268387" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634071" name="out.lightstopmod-7TeV-tanbLow-nnlo.root" path="out.lightstopmod-7TeV-tanbLow-nnlo.root" size="1218162" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1394634070" name="out.lightstopmod-8TeV-tanbHigh-nnlo.root" path="out.lightstopmod-8TeV-tanbHigh-nnlo.root" size="17265776" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstopmod-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1394634047" name="out.lightstopmod-8TeV-tanbLow-nnlo.root" path="out.lightstopmod-8TeV-tanbLow-nnlo.root" size="1217313" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 412014-02-10 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 40 to 40
 

Available Xsection scans

Changed:
<
<
  • SuSHi + 4FS bbH scans
>
>
  • SuSHi + 4FS bbH scans
  ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
Changed:
<
<
bbH 5FS scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
>
>
bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi

 
Changed:
<
<
>
>
  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
  ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
Line: 252 to 267
 
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169776" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170168" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170165" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170171" name="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" size="29890978" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170168" name="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" size="31611343" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027113" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027079" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027143" name="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" size="29890978" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027111" name="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" size="31611343" user="monicava" version="1"
 
META FILEATTACHMENT attachment="mssm_xs_tools_v0.4.C" attr="" comment="Access tool: version 0.4" date="1386172522" name="mssm_xs_tools_v0.4.C" path="mssm_xs_tools_v0.4.C" size="39898" user="monicava" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v0.4.h" attr="" comment="Access tool: version 0.4" date="1386172522" name="mssm_xs_tools_v0.4.h" path="mssm_xs_tools_v0.4.h" size="17158" user="monicava" version="1"
Added:
>
>
META FILEATTACHMENT attachment="out.lightstau1-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027245" name="out.lightstau1-7TeV-tanbHigh-nnlo.root" path="out.lightstau1-7TeV-tanbHigh-nnlo.root" size="17350034" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstau1-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027227" name="out.lightstau1-7TeV-tanbLow-nnlo.root" path="out.lightstau1-7TeV-tanbLow-nnlo.root" size="1543459" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstau1-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027226" name="out.lightstau1-8TeV-tanbHigh-nnlo.root" path="out.lightstau1-8TeV-tanbHigh-nnlo.root" size="17335195" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lightstau1-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027206" name="out.lightstau1-8TeV-tanbLow-nnlo.root" path="out.lightstau1-8TeV-tanbLow-nnlo.root" size="1542840" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lowmH-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027343" name="out.lowmH-7TeV-tanbHigh-nnlo.root" path="out.lowmH-7TeV-tanbHigh-nnlo.root" size="3587603" user="monicava" version="1"
META FILEATTACHMENT attachment="out.lowmH-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027340" name="out.lowmH-8TeV-tanbHigh-nnlo.root" path="out.lowmH-8TeV-tanbHigh-nnlo.root" size="3583786" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027338" name="out.mhmodm-7TeV-tanbHigh-nnlo.root" path="out.mhmodm-7TeV-tanbHigh-nnlo.root" size="17353727" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027321" name="out.mhmodm-7TeV-tanbLow-nnlo.root" path="out.mhmodm-7TeV-tanbLow-nnlo.root" size="1545329" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027320" name="out.mhmodm-8TeV-tanbHigh-nnlo.root" path="out.mhmodm-8TeV-tanbHigh-nnlo.root" size="17340182" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodm-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027303" name="out.mhmodm-8TeV-tanbLow-nnlo.root" path="out.mhmodm-8TeV-tanbLow-nnlo.root" size="1544857" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-7TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027433" name="out.mhmodp-7TeV-tanbHigh-nnlo.root" path="out.mhmodp-7TeV-tanbHigh-nnlo.root" size="17374182" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-7TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027416" name="out.mhmodp-7TeV-tanbLow-nnlo.root" path="out.mhmodp-7TeV-tanbLow-nnlo.root" size="1544001" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-8TeV-tanbHigh-nnlo.root" attr="" comment="" date="1392027415" name="out.mhmodp-8TeV-tanbHigh-nnlo.root" path="out.mhmodp-8TeV-tanbHigh-nnlo.root" size="17362382" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmodp-8TeV-tanbLow-nnlo.root" attr="" comment="" date="1392027398" name="out.mhmodp-8TeV-tanbLow-nnlo.root" path="out.mhmodp-8TeV-tanbLow-nnlo.root" size="1543466" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 402013-12-11 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 40 to 40
 

Available Xsection scans

Changed:
<
<
  • SuSHi + 4FS bbH scans
>
>
  • SuSHi + 4FS bbH scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
 
Line: 50 to 52
 
Changed:
<
<
>
>
  • HIGLU+ggH@NNLO + bbH@NNLO 5FS + 4FS bbH scans
    ggH scale: muR=muF=m_Phi. Scale variation: 0.5*m_Phi < mR, muF < 2*m_Phi
    bbH 5FS scale: muR= m_Phi muF=0.25*m_Phi. Scale variation: 0.2*m_Phi < muR < 5*m_Phi ; 0.1*m_Phi < muF < 0.7*m_Phi
 

Revision 392013-12-04 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 38 to 38
 
Changed:
<
<

Available Xsection scans: SuSHi + 4FS bbH scans

>
>

Available Xsection scans

 
Added:
>
>
  • SuSHi + 4FS bbH scans
 
Line: 49 to 50
 
Added:
>
>
 
Deleted:
<
<

Available Xsection scans: latest root files

NEW!
New grids exist for 7 TeV in the mhmax scenario with different values of mu = 200, 400, 800, -200, -400 GeV and the no mixing scenario for a value of mu=200 GeV

SCAN with tanbeta value as low as tanbeta=1

Scan in the low tanbeta region between 0.5-0.9

NEW!
A new grid is available in 7 TeV grid, which contains the pdf error for the combined ggF+bbH5f cross section. The access tool has also been updated (v2) to provide functions to query the combined cross section, pdf and scale errors. The new tool is in Download the header file and the implementation file
-----------------------------------------------------------------

NEW!
The access tool has been updated (v3) to provide functions to get the Santander matched b-associated production cross sections (see this meeting).
-----------------------------------------------------------------

 
Changed:
<
<
NEW!
>
>
The access tool has been updated (v5) to provide functions to query the combined cross section, pdf and scale errors for the new SusHi scan files.

The new tool is in Download the header file and the implementation file

The access tool provides functions to get the Santander matched b-associated production cross sections (see this meeting).

 The write-up of the Santander-Macthing is available: "Bottom-quark associated Higgs-boson production: reconciling the four- and five-flavour scheme approach" by R. Harlander, M. Krämer, and M. Schumacher,
Line: 94 to 69
 
 
H(bb) cross-section
Deleted:
<
<
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Deleted:
<
<
A generalized tool to perform such a scan in the mA-tam(beta) plane is currently being prepared. Since this is not yet available for general usage, please contact the MSSM neutral Higgs contact persons if you need an additional scan. Please be aware that the provided cross sections are only valid for the case of heavy squarks!
 

Some consideration on h/H/A ->tau tau (xs * BR)

Line: 233 to 206
 
Added:
>
>
 
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools.h" attr="" comment="Version 3 of the tool to read the new grid" date="1302686618" name="mssm_xs_tools.h" path="mssm_xs_tools.h" size="17158" stream="mssm_xs_tools.h" tmpFilename="/usr/tmp/CGItemp15369" user="78a51471b6627bd81779" version="3"
META FILEATTACHMENT attachment="mssm_xs_tools.C" attr="" comment="New version of the tool V5: linear errors in the Santander matching methods and fixed sign for negative variations of MSSM xsections" date="1313937936" name="mssm_xs_tools.C" path="mssm_xs_tools.C" size="39898" user="78a51471b6627bd81779" version="9"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.h" attr="" comment="Access tool: version 0.5" date="1386172658" name="mssm_xs_tools.h" path="mssm_xs_tools.h" size="11337" user="monicava" version="4"
META FILEATTACHMENT attachment="mssm_xs_tools.C" attr="" comment="Access tool: version 0.5" date="1386172658" name="mssm_xs_tools.C" path="mssm_xs_tools.C" size="27175" user="monicava" version="10"
 


META FILEATTACHMENT attachment="out.mhmax_7_nnlo.root" attr="" comment="Scan which include the ggF+bbH combined PDF uncertainty" date="1296827611" name="out.mhmax_7_nnlo.root" path="out.mhmax_7_nnlo.root" size="28151505" user="monicava" version="1"
META FILEATTACHMENT attachment="santandermatching-hks.pdf" attr="" comment="Description of Santander matching procedure for inclusive pp-->H(bb) cross-section" date="1307193388" name="santandermatching-hks.pdf" path="santandermatching-hks.pdf" size="181607" stream="santandermatching-hks.pdf" tmpFilename="/usr/tmp/CGItemp52250" user="schumach" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_7_nnlo.root" attr="" comment="mhmax mu=200, 7 TeV" date="1321004712" name="out.mhmax_mu200_7_nnlo.root" path="out.mhmax_mu200_7_nnlo.root" size="28151505" user="monicava" version="1"
Line: 265 to 240
 
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=-200, 7 TeV, lowest tanbeta=1" date="1328106516" name="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" path="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" size="29800667" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[1,70]; Note no BRs for WW or gamma-gamma" date="1343391609" name="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" path="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" size="31624335" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[0.5,0.9]; Note no BRs for WW or gamma-gamma" date="1350290547" name="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" path="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" size="2414466" user="tvickey" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047341" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047729" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans (in pb)" date="1385586730" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans (in pb)" date="1385586811" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169782" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169781" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169781" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169779" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169779" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="New scans with SusHi" date="1386169776" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="New scans with SusHi" date="1386169777" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170168" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170165" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170171" name="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-7TeV-tanbHigh-nnlo.root" size="29890978" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" attr="" comment="mhmax scans with fixed cross sections (all in pb)" date="1386170168" name="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" path="out.mhmax-mu200-8TeV-tanbHigh-nnlo.root" size="31611343" user="monicava" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v0.4.C" attr="" comment="Access tool: version 0.4" date="1386172522" name="mssm_xs_tools_v0.4.C" path="mssm_xs_tools_v0.4.C" size="39898" user="monicava" version="1"
META FILEATTACHMENT attachment="mssm_xs_tools_v0.4.h" attr="" comment="Access tool: version 0.4" date="1386172522" name="mssm_xs_tools_v0.4.h" path="mssm_xs_tools_v0.4.h" size="17158" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 382013-11-27 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 273 to 273
 
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047729" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
Added:
>
>
META FILEATTACHMENT attachment="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans (in pb)" date="1385586730" name="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-7TeV-tanbLow-nnlo.root" size="2275552" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" attr="" comment="mhmax scans (in pb)" date="1385586811" name="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" path="out.mhmax-mu200-8TeV-tanbLow-nnlo.root" size="2405097" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 372013-11-27 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 265 to 265
 
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=-200, 7 TeV, lowest tanbeta=1" date="1328106516" name="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" path="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" size="29800667" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[1,70]; Note no BRs for WW or gamma-gamma" date="1343391609" name="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" path="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" size="31624335" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[0.5,0.9]; Note no BRs for WW or gamma-gamma" date="1350290547" name="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" path="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" size="2414466" user="tvickey" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047341" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047341" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
 
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047729" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"

Revision 362013-11-21 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 38 to 38
 
Changed:
<
<

Available Xsection scans: SuSHi + 4FS bbH scans

>
>

Available Xsection scans: SuSHi + 4FS bbH scans

 

Available Xsection scans: latest root files

Line: 255 to 265
 
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=-200, 7 TeV, lowest tanbeta=1" date="1328106516" name="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" path="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" size="29800667" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[1,70]; Note no BRs for WW or gamma-gamma" date="1343391609" name="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" path="out.mhmax_mu200_8_nnlo.tanBeta_gte1_FHv274.root" size="31624335" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" attr="" comment="!FeynHiggs 2.7.4: 8 TeV MSSM Neutral Higgs scans in the mhmax and nomixing scenarios for mA=[90 GeV,1000 GeV] and tanB=[0.5,0.9]; Note no BRs for WW or gamma-gamma" date="1350290547" name="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" path="out.mhmax_mu200_8_nnlo.low_tanBeta_FHv274.root" size="2414466" user="tvickey" version="1"
Added:
>
>
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047341" name="mhmodm_7TeV_tanbHigh.root" path="mhmodm_7TeV_tanbHigh.root" size="17570365" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_7TeV_tanbLow.root" path="mhmodm_7TeV_tanbLow.root" size="1364375" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047340" name="mhmodm_8TeV_tanbHigh.root" path="mhmodm_8TeV_tanbHigh.root" size="17549852" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodm_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodm_8TeV_tanbLow.root" path="mhmodm_8TeV_tanbLow.root" size="1361800" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbHigh.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047339" name="mhmodp_7TeV_tanbHigh.root" path="mhmodp_7TeV_tanbHigh.root" size="17590748" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_7TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_7TeV_tanbLow.root" path="mhmodp_7TeV_tanbLow.root" size="1364222" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbLow.root" attr="" comment="SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047338" name="mhmodp_8TeV_tanbLow.root" path="mhmodp_8TeV_tanbLow.root" size="1357773" user="monicava" version="1"
META FILEATTACHMENT attachment="mhmodp_8TeV_tanbHigh.root" attr="" comment="!SusHi+ 4FSbbH scans: new scenarios mhmod" date="1385047729" name="mhmodp_8TeV_tanbHigh.root" path="mhmodp_8TeV_tanbHigh.root" size="17571295" user="monicava" version="1"
 
META TOPICMOVED by="tanaka" date="1265555699" from="LHCPhysics.HiggsMSSMNeutral" to="LHCPhysics.MSSMNeutral"

Revision 352013-11-13 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 38 to 38
 
Added:
>
>

Available Xsection scans: SuSHi + 4FS bbH scans

 

Available Xsection scans: latest root files

NEW!
New grids exist for 7 TeV in the mhmax scenario with different values of mu = 200, 400, 800, -200, -400 GeV and the no mixing scenario for a value of mu=200 GeV

Revision 342013-06-26 - TrevorVickey

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 14 to 14
 
  • masses of the scalar bosons h and H (calculated using FeynHiggs 2.7.4 with Mtop=172.5 GeV, mb(mb)=4.213 GeV, alphas(MZ)=0.119, MSUSY=1000 GeV, Xt=2000 GeV, M2=200 GeV, mu=200 GeV, M3=800 GeV)
  • Cross sections for b-associated h/H/A production in the 5 flavour scheme (NNLO QCD), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above).
Changed:
<
<
  • Cross sections for b-associated h/H/A production in the 4 flavour scheme (NLO QCD) and scale uncertainties using MSTW2008. PDF uncertainties are not available. (not yet for 14 TeV)
>
>
  • Cross sections for b-associated h/H/A production in the 4 flavour scheme (NLO QCD) and scale uncertainties using MSTW2008. PDF uncertainties are not available. (not yet for 14 TeV; Please note that as a consequence, the Santander-matching member function from the mssm_xs_tools.C macro will NOT return meaningful 14 TeV cross section numbers!)
 
  • Cross sections for gluon-gluon-fusion h/H/production (NLO QCD (HIGLU) for b-loop and t-b-interference, top-loop only is corrected to NNLO QCD (ggh@nnlo)), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above). (!PDF uncertainties not yet for 14 TeV.)
  • PRELIMINARY AND SUBJECT TO BR subgroup approval: Branching fractions of h/H/A to bottom quarks, tau leptons and muons from FeynHiggs 2.7.4.

Revision 332013-02-19 - TrevorVickey

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"

MSSM Neutral Higgs

Line: 10 to 10
 

Available Xsection scans

Changed:
<
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Two complete scans (for 7 TeV and for 14 TeV) of the mA-tan(beta) plane in the mhmax scenario are available with the numbers produced for the CERN Yellow Report that will soon be published. The scans have been made between mA=90 GeV and mA=1000 GeV in steps of 1 GeV and between tan(beta)=5 and 60 (70 for the 14 TeV scan) in steps of 1. The scanned quantities are available in form of 2 dimensional ROOT histograms. The quantities available in these are:
>
>
Two complete scans (for 7 TeV and for 14 TeV) of the mA-tan(beta) plane in the mhmax scenario are available with the numbers produced for the CERN Yellow Report that will soon be published. The scans have been made between mA=90 GeV and mA=1000 GeV in steps of 1 GeV and between tan(beta)=1 and 60 (5 and 70 for the 14 TeV scan) in steps of 1. For very low tan(beta), the scan is done between tan(beta)=0.5 and 0.9 in steps of 0.1. The scanned quantities are available in form of 2 dimensional ROOT histograms. The quantities available in these are:
 
  • masses of the scalar bosons h and H (calculated using FeynHiggs 2.7.4 with Mtop=172.5 GeV, mb(mb)=4.213 GeV, alphas(MZ)=0.119, MSUSY=1000 GeV, Xt=2000 GeV, M2=200 GeV, mu=200 GeV, M3=800 GeV)
  • Cross sections for b-associated h/H/A production in the 5 flavour scheme (NNLO QCD), and scale and PDF(+alphas) uncertainties of these using MSTW2008. The rescaling to MSSM couplings was done with FeynHiggs 2.7.4 (same input parameters as above).

Revision 322012-11-26 - MonicaVazquezAcosta

Line: 1 to 1
 
META TOPICPARENT name="CrossSections"
Changed:
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MSSM Neutral Higgs

>
>

MSSM Neutral Higgs

 
Line: 220 to 220
 
Changed:
<
<
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" stream="out.mhmax_7.root" tmpFilename="/usr/tmp/CGItemp47951" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" stream="out.mhmax_14.root" tmpFilename="/usr/tmp/CGItemp41784" user="78a51471b6627bd81779" version="1"
>
>
META FILEATTACHMENT attachment="out.mhmax_7.root" attr="" comment="mhmax scan results for 7 TeV" date="1292323092" name="out.mhmax_7.root" path="out.mhmax_7.root" size="22026890" user="tvickey" version="2"
META FILEATTACHMENT attachment="out.mhmax_14.root" attr="" comment="mhmax scan results for 14 TeV,bbh 4f results and PDF uncertainties for ggF missing at the moment." date="1290196237" name="out.mhmax_14.root" path="out.mhmax_14.root" size="15128192" user="78a51471b6627bd81779" version="1"
 
META FILEATTACHMENT attachment="mssm_xs_tools.h" attr="" comment="Version 3 of the tool to read the new grid" date="1302686618" name="mssm_xs_tools.h" path="mssm_xs_tools.h" size="17158" stream="mssm_xs_tools.h" tmpFilename="/usr/tmp/CGItemp15369" user="78a51471b6627bd81779" version="3"
Changed:
<
<
META FILEATTACHMENT attachment="mssm_xs_tools.C" attr="" comment="New version of the tool V5: linear errors in the Santander matching methods and fixed sign for negative variations of MSSM xsections" date="1313937936" name="mssm_xs_tools.C" path="mssm_xs_tools.C" size="39898" stream="mssm_xs_tools.C" tmpFilename="/usr/tmp/CGItemp10593" user="78a51471b6627bd81779" version="9"
META FILEATTACHMENT attachment="out.mhmax_7_nnlo.root" attr="" comment="Scan which include the ggF+bbH combined PDF uncertainty" date="1296827611" name="out.mhmax_7_nnlo.root" path="out.mhmax_7_nnlo.root" size="28151505" stream="out.mhmax_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp4969" user="monicava" version="1"
>
>
META FILEATTACHMENT attachment="mssm_xs_tools.C" attr="" comment="New version of the tool V5: linear errors in the Santander matching methods and fixed sign for negative variations of MSSM xsections" date="1313937936" name="mssm_xs_tools.C" path="mssm_xs_tools.C" size="39898" user="78a51471b6627bd81779" version="9"
META FILEATTACHMENT attachment="out.mhmax_7_nnlo.root" attr="" comment="Scan which include the ggF+bbH combined PDF uncertainty" date="1296827611" name="out.mhmax_7_nnlo.root" path="out.mhmax_7_nnlo.root" size="28151505" user="monicava" version="1"
 
META FILEATTACHMENT attachment="santandermatching-hks.pdf" attr="" comment="Description of Santander matching procedure for inclusive pp-->H(bb) cross-section" date="1307193388" name="santandermatching-hks.pdf" path="santandermatching-hks.pdf" size="181607" stream="santandermatching-hks.pdf" tmpFilename="/usr/tmp/CGItemp52250" user="schumach" version="1"
Changed:
<
<
META FILEATTACHMENT attachment="out.mhmax_mu200_7_nnlo.root" attr="" comment="mhmax mu=200, 7 TeV" date="1321004712" name="out.mhmax_mu200_7_nnlo.root" path="out.mhmax_mu200_7_nnlo.root" size="28151505" stream="out.mhmax_mu200_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp53891" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu400_7_nnlo.root" attr="" comment="mhmax mu=400, 7 TeV" date="1321004741" name="out.mhmax_mu400_7_nnlo.root" path="out.mhmax_mu400_7_nnlo.root" size="28303378" stream="out.mhmax_mu400_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp54001" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu600_7_nnlo.root" attr="" comment="mhmax mu=600, 7 TeV" date="1321004768" name="out.mhmax_mu600_7_nnlo.root" path="out.mhmax_mu600_7_nnlo.root" size="28120186" stream="out.mhmax_mu600_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp53926" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu800_7_nnlo.root" attr="" comment="mhmax mu=800, 7 TeV" date="1321004793" name="out.mhmax_mu800_7_nnlo.root" path="out.mhmax_mu800_7_nnlo.root" size="27992004" stream="out.mhmax_mu800_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp54009" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-200_7_nnlo.root" attr="" comment="mhmax mu=-200, 7 TeV" date="1321004846" name="out.mhmax_mu-200_7_nnlo.root" path="out.mhmax_mu-200_7_nnlo.root" size="28351718" stream="out.mhmax_mu-200_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp53990" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-400_7_nnlo.root" attr="" comment="mhmax mu=-400, 7 TeV" date="1321004908" name="out.mhmax_mu-400_7_nnlo.root" path="out.mhmax_mu-400_7_nnlo.root" size="28426988" stream="out.mhmax_mu-400_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp54005" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu200_7_nnlo.root" attr="" comment="nomix mu=200, 7 TeV" date="1321004960" name="out.nomix_mu200_7_nnlo.root" path="out.nomix_mu200_7_nnlo.root" size="28135687" stream="out.nomix_mu200_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp54051" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.root" attr="" comment="nomix mu=-200, 7 TeV" date="1321363605" name="out.nomix_mu-200_7_nnlo.root" path="out.nomix_mu-200_7_nnlo.root" size="28217597" stream="out.nomix_mu-200_7_nnlo.root" tmpFilename="/usr/tmp/CGItemp53231" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-200_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=-200, 7 TeV, tanbeta between 0.5 & 0.9" date="1328106056" name="out.mhmax_mu-200_7_nnlo.low_tanBeta.root" path="out.mhmax_mu-200_7_nnlo.low_tanBeta.root" size="2289091" stream="out.mhmax_mu-200_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13159" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu400_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=400, 7 TeV, tanbeta between 0.5 & 0.9" date="1328105927" name="out.mhmax_mu400_7_nnlo.low_tanBeta.root" path="out.mhmax_mu400_7_nnlo.low_tanBeta.root" size="2289329" stream="out.mhmax_mu400_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13231" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu600_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=600, 7 TeV, tanbeta between 0.5 & 0.9" date="1328105953" name="out.mhmax_mu600_7_nnlo.low_tanBeta.root" path="out.mhmax_mu600_7_nnlo.low_tanBeta.root" size="2290792" stream="out.mhmax_mu600_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13100" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=200, 7 TeV, tanbeta between 0.5 & 0.9" date="1328105975" name="out.mhmax_mu200_7_nnlo.low_tanBeta.root" path="out.mhmax_mu200_7_nnlo.low_tanBeta.root" size="2289050" stream="out.mhmax_mu200_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13238" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu800_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=800, 7 TeV, tanbeta between 0.5 & 0.9" date="1328106001" name="out.mhmax_mu800_7_nnlo.low_tanBeta.root" path="out.mhmax_mu800_7_nnlo.low_tanBeta.root" size="2291681" stream="out.mhmax_mu800_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13097" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-400_7_nnlo.low_tanBeta.root" attr="" comment="mhmax mu=-400, 7 TeV, tanbeta between 0.5 & 0.9" date="1328106082" name="out.mhmax_mu-400_7_nnlo.low_tanBeta.root" path="out.mhmax_mu-400_7_nnlo.low_tanBeta.root" size="2290701" stream="out.mhmax_mu-400_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13139" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu200_7_nnlo.low_tanBeta.root" attr="" comment="nomix mu=200, 7 TeV, tanbeta between 0.5 & 0.9" date="1328106148" name="out.nomix_mu200_7_nnlo.low_tanBeta.root" path="out.nomix_mu200_7_nnlo.low_tanBeta.root" size="2271037" stream="out.nomix_mu200_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13205" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.low_tanBeta.root" attr="" comment="nomix mu=-200, 7 TeV, tanbeta between 0.5 & 0.9" date="1328106213" name="out.nomix_mu-200_7_nnlo.low_tanBeta.root" path="out.nomix_mu-200_7_nnlo.low_tanBeta.root" size="2272449" stream="out.nomix_mu-200_7_nnlo.low_tanBeta.root" tmpFilename="/usr/tmp/CGItemp13230" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu200_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=200, 7 TeV, lowest tanbeta=1" date="1328106256" name="out.mhmax_mu200_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu200_7_nnlo.tanBeta_gte1.root" size="29906249" stream="out.mhmax_mu200_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13245" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu400_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=400, 7 TeV, lowest tanbeta=1" date="1328106288" name="out.mhmax_mu400_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu400_7_nnlo.tanBeta_gte1.root" size="30046026" stream="out.mhmax_mu400_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13222" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu600_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=600, 7 TeV, lowest tanbeta=1" date="1328106319" name="out.mhmax_mu600_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu600_7_nnlo.tanBeta_gte1.root" size="29862988" stream="out.mhmax_mu600_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13283" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu800_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=800, 7 TeV, lowest tanbeta=1" date="1328106356" name="out.mhmax_mu800_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu800_7_nnlo.tanBeta_gte1.root" size="29735031" stream="out.mhmax_mu800_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13323" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=-200, 7 TeV, lowest tanbeta=1" date="1328106382" name="out.mhmax_mu-200_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu-200_7_nnlo.tanBeta_gte1.root" size="30093726" stream="out.mhmax_mu-200_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13256" user="monicava" version="1"
META FILEATTACHMENT attachment="out.mhmax_mu-400_7_nnlo.tanBeta_gte1.root" attr="" comment="mhmax mu=-400, 7 TeV, lowest tanbeta=1" date="1328106442" name="out.mhmax_mu-400_7_nnlo.tanBeta_gte1.root" path="out.mhmax_mu-400_7_nnlo.tanBeta_gte1.root" size="30168396" stream="out.mhmax_mu-400_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13243" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=200, 7 TeV, lowest tanbeta=1" date="1328106478" name="out.nomix_mu200_7_nnlo.tanBeta_gte1.root" path="out.nomix_mu200_7_nnlo.tanBeta_gte1.root" size="29717948" stream="out.nomix_mu200_7_nnlo.tanBeta_gte1.root" tmpFilename="/usr/tmp/CGItemp13266" user="monicava" version="1"
META FILEATTACHMENT attachment="out.nomix_mu-200_7_nnlo.tanBeta_gte1.root" attr="" comment="nomix mu=-200, 7 TeV, lowest tanbe