# Difference: LHCHXSWGFiducialAndSTXS (1 vs. 16)

#### Revision 162019-06-18 - NicolasBerger

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 58 to 58

#### Stage 1

Changed:
<
<
Stage 1 ggF bins
>
>
Stage 1 gg → H bins

Changed:
<
<
Stage 1 VBF bins
>
>
Stage 1 EW qqH bins
Stage 1 VH bins

#### Revision 152019-06-17 - NicolasBerger

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 70 to 70
This update follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings ( here and here).
Changed:
<
<
The Rivet tool that performs the STXS classification has also been updated to implement the Stage 1.1 scheme.
>
>
The Rivet tool that performs the STXS classification has also been updated to implement the Stage 1.1 scheme.

• gg → H (gluon-fusion and gg → (Z → qq) H)
Line: 89 to 89
>
>

## Code

The relevant code is hosted in the STXS gitlab area :

• Classification : Rivet routines that assign STXS bin labels to a given MC event.
• VBF Uncertainties : Code computing theory uncertainty values for events in the VBF categories.

## References

### Run 2 results

#### Revision 142019-05-11 - JasonNielsen

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 41 to 41

• Measure cross sections separated into production modes (or more generally kinematic templates)
• Allows different efficiencies/acceptances for different production modes without incurring a dependence on the SM production mode mix
• Currently, the main SM production processes act as kinematic templates, in the future more kinematic templates can be added (e.g. for a CP-odd Higgs)
Changed:
<
<
• Non-Higgs backgrounds are substracted
>
>
• Non-Higgs backgrounds are subtracted

• In the future, one could add templates for BSM sensitive backgrounds (e.g. for pp->WW)
• Simplified (idealized) bin definitions abstracted from the actual measurement categories
• Allows for some acceptance corrections

#### Revision 132019-02-09 - NicolasBerger

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 70 to 70
This update follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings ( here and here).
Changed:
<
<
An updated version of the Rivet tool that performs the STXS classification will be made available shortly.
>
>
The Rivet tool that performs the STXS classification has also been updated to implement the Stage 1.1 scheme.

• gg → H (gluon-fusion and gg → (Z → qq) H)

#### Revision 122019-01-28 - FrankTackmann

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 66 to 66

#### Stage 1.1

Changed:
<
<
This section describes an updated definition of the Stage 1 binning (Stage 1.1). This definition supersedes the one provided above, and should be used by new analyses performing STXS measurements. The changes with respect to Stage 1 are not backwards-compatible (due to the VBF process which required some reorganization).
>
>
This section describes an updated definition of the Stage 1 binning (Stage 1.1). This definition supersedes the one provided above, and should be used by new analyses performing STXS measurements. The changes with respect to Stage 1 are not backwards-compatible (due to the VBF process which required some reorganization). A note describing these new binnings in more detail is in preparation.

Changed:
<
<
The updates follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings ( here and here).
>
>
This update follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings ( here and here).
An updated version of the Rivet tool that performs the STXS classification will be made available shortly.
Line: 77 to 77
Changed:
<
<
NOTE: This process is defined as the usual gluon-fusion production including gg-induced EW corrections. This includes virtual EW corrections to the gg → H form factor as well as real EW corrections, corresponding to gg → ZH → qq H. (The latter are very small and are typically neglected at the present level of precision. Furthermore, the same binning should also be applied to the bbH process in analyses in which it is not distinguishable from gg → H, and the measurement of the total gg→H + bbH cross-section should be reported.
>
>
NOTE: This process is defined as the usual gluon-fusion production including gg-induced EW corrections. This includes virtual EW corrections to the gg → H form factor as well as real EW corrections, corresponding to gg → ZH → qq H. (The latter are very small and are typically neglected at the present level of precision.)
Furthermore, the same binning should also be applied to the bbH process in analyses in which it is not distinguishable from gg → H. In this case, measurements should report the sum of gg→H + bbH for each bin.

• EW qqH (VBF and qq → (V → qq) H)

#### Revision 112019-01-27 - NicolasBerger

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 77 to 77
Changed:
<
<
NOTE: This process is defined as the usual gluon-fusion production including gg-induced EW corrections. This includes virtual EW corrections to the gg->H form factor as well as real EW corrections, corresponding to gg → ZH → qq H. (The latter are very small and are typically neglected at the present level of precision. Furthermore, it includes the bb → H process which at present is not distinguishable from gg → H.
>
>
NOTE: This process is defined as the usual gluon-fusion production including gg-induced EW corrections. This includes virtual EW corrections to the gg → H form factor as well as real EW corrections, corresponding to gg → ZH → qq H. (The latter are very small and are typically neglected at the present level of precision. Furthermore, the same binning should also be applied to the bbH process in analyses in which it is not distinguishable from gg → H, and the measurement of the total gg→H + bbH cross-section should be reported.

• EW qqH (VBF and qq → (V → qq) H)
Line: 147 to 147

 META FILEATTACHMENT attachment="simplifiedXS_VBF.pdf" attr="" comment="" date="1494250055" name="simplifiedXS_VBF.pdf" path="simplifiedXS_VBF.pdf" size="13172" user="ftackman" version="1" attachment="simplifiedXS_VH.pdf" attr="" comment="" date="1494250063" name="simplifiedXS_VH.pdf" path="simplifiedXS_VH.pdf" size="12625" user="ftackman" version="1" attachment="simplifiedXS.pdf" attr="" comment="" date="1494250084" name="simplifiedXS.pdf" path="simplifiedXS.pdf" size="18613" user="ftackman" version="1"
Changed:
<
<
 META FILEATTACHMENT attachment="simplifiedXS_ggF_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_ggF_1.1.pdf" path="simplifiedXS_ggF_1.1.pdf" size="13540" user="thrynova" version="1" attachment="simplifiedXS_VBF_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_VBF_1.1.pdf" path="simplifiedXS_VBF_1.1.pdf" size="14128" user="thrynova" version="1" attachment="simplifiedXS_VH_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_VH_1.1.pdf" path="simplifiedXS_VH_1.1.pdf" size="12312" user="thrynova" version="1" attachment="simplifiedXS_ggF_1.1.png" attr="" comment="" date="1548548003" name="simplifiedXS_ggF_1.1.png" path="simplifiedXS_ggF_1.1.png" size="79420" user="thrynova" version="1" attachment="simplifiedXS_VBF_1.1.png" attr="" comment="" date="1548548006" name="simplifiedXS_VBF_1.1.png" path="simplifiedXS_VBF_1.1.png" size="82818" user="thrynova" version="1" attachment="simplifiedXS_VH_1.1.png" attr="" comment="" date="1548548008" name="simplifiedXS_VH_1.1.png" path="simplifiedXS_VH_1.1.png" size="65852" user="thrynova" version="1"
>
>
 META FILEATTACHMENT attachment="simplifiedXS_ggF_1.1.pdf" attr="" comment="" date="1548628586" name="simplifiedXS_ggF_1.1.pdf" path="simplifiedXS_ggF_1.1.pdf" size="13303" user="nberger" version="1" attachment="simplifiedXS_VBF_1.1.pdf" attr="" comment="" date="1548628586" name="simplifiedXS_VBF_1.1.pdf" path="simplifiedXS_VBF_1.1.pdf" size="14067" user="nberger" version="1" attachment="simplifiedXS_VH_1.1.pdf" attr="" comment="" date="1548628586" name="simplifiedXS_VH_1.1.pdf" path="simplifiedXS_VH_1.1.pdf" size="12193" user="nberger" version="1" attachment="simplifiedXS_VH_1.1.png" attr="" comment="" date="1548628613" name="simplifiedXS_VH_1.1.png" path="simplifiedXS_VH_1.1.png" size="61889" user="nberger" version="1" attachment="simplifiedXS_ggF_1.1.png" attr="" comment="" date="1548628613" name="simplifiedXS_ggF_1.1.png" path="simplifiedXS_ggF_1.1.png" size="77677" user="nberger" version="1" attachment="simplifiedXS_VBF_1.1.png" attr="" comment="" date="1548628614" name="simplifiedXS_VBF_1.1.png" path="simplifiedXS_VBF_1.1.png" size="80084" user="nberger" version="1"

#### Revision 102019-01-27 - FrankTackmann

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 66 to 66

#### Stage 1.1

Changed:
<
<
This section describes an updated definition of the Stage 1 binning (Stage 1.1). This definition supersedes the one provided above, and should be used by new analyses performing STXS measurements. The changes with respect to Stage 1 are not backwards-compatible.
>
>
This section describes an updated definition of the Stage 1 binning (Stage 1.1). This definition supersedes the one provided above, and should be used by new analyses performing STXS measurements. The changes with respect to Stage 1 are not backwards-compatible (due to the VBF process which required some reorganization).
The updates follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings (here and here).

An updated version of the Rivet tool that performs the STXS classification will be made available shortly.

Changed:
<
<
• gg→ H (gluon-fusion and gg → (Z → qq) H)
>
>
• gg → H (gluon-fusion and gg → (Z → qq) H)
Changed:
<
<
>
>

Changed:
<
<
• EW qqH (VBF and qq/gg → (V → qq) H)
>
>
NOTE: This process is defined as the usual gluon-fusion production including gg-induced EW corrections. This includes virtual EW corrections to the gg->H form factor as well as real EW corrections, corresponding to gg → ZH → qq H. (The latter are very small and are typically neglected at the present level of precision. Furthermore, it includes the bb → H process which at present is not distinguishable from gg → H.

>
>
• EW qqH (VBF and qq → (V → qq) H)
Changed:
<
<
>
>

Changed:
<
<
• VH→leptons
>
>
• VH (qq+gg → V(→ leptons) H)
Changed:
<
<
>
>

## References

### Run 2 results

Changed:
<
<
• Measurement of fiducial, differential and production cross sections in the H → γγ decay channel with 13.3 fb-1 of 13 TeV proton-proton collision data with the ATLAS detector, ATLAS-CONF-2016-067
• Study of the Higgs boson properties and search for high-mass scalar resonances in the $H→ ZZ^{*}→ 4\ell$ decay channel at √s = 13 TeV with the ATLAS detector, ATLAS-CONF-2016-079
• Combined measurements of the Higgs boson production and decay rates in H→ ZZ* → 4ℓ and H → γγ final states using pp collision data at √s = 13 TeV in the ATLAS experiment, ATLAS-CONF-2016-081
>
>
• Measurement of fiducial, differential and production cross sections in the H → γγ decay channel with 13.3 fb-1 of 13 TeV proton-proton collision data with the ATLAS detector, ATLAS-CONF-2016-067
• Study of the Higgs boson properties and search for high-mass scalar resonances in the $H→ ZZ^{*}→ 4\ell$ decay channel at √s = 13 TeV with the ATLAS detector, ATLAS-CONF-2016-079
• Combined measurements of the Higgs boson production and decay rates in H→ ZZ* → 4ℓ and H → γγ final states using pp collision data at √s = 13 TeV in the ATLAS experiment, ATLAS-CONF-2016-081

### Run 1 results

#### Revision 92019-01-27 - TetianaHrynova

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 62 to 63
Stage 1 VBF bins
>
>

#### Stage 1.1

This section describes an updated definition of the Stage 1 binning (Stage 1.1). This definition supersedes the one provided above, and should be used by new analyses performing STXS measurements. The changes with respect to Stage 1 are not backwards-compatible.

The updates follows from discussions at the 2018 LHCHXSWG workshop and dedicated fid/dif/STXS subgroup meetings (here and here).

An updated version of the Rivet tool that performs the STXS classification will be made available shortly.

• gg→ H (gluon-fusion and gg → (Z → qq) H)

• EW qqH (VBF and qq/gg → (V → qq) H)

• VH→leptons

## References

### Run 2 results

Line: 121 to 149

 META FILEATTACHMENT attachment="simplifiedXS_VBF.pdf" attr="" comment="" date="1494250055" name="simplifiedXS_VBF.pdf" path="simplifiedXS_VBF.pdf" size="13172" user="ftackman" version="1" attachment="simplifiedXS_VH.pdf" attr="" comment="" date="1494250063" name="simplifiedXS_VH.pdf" path="simplifiedXS_VH.pdf" size="12625" user="ftackman" version="1" attachment="simplifiedXS.pdf" attr="" comment="" date="1494250084" name="simplifiedXS.pdf" path="simplifiedXS.pdf" size="18613" user="ftackman" version="1"
>
>
 META FILEATTACHMENT attachment="simplifiedXS_ggF_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_ggF_1.1.pdf" path="simplifiedXS_ggF_1.1.pdf" size="13540" user="thrynova" version="1" attachment="simplifiedXS_VBF_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_VBF_1.1.pdf" path="simplifiedXS_VBF_1.1.pdf" size="14128" user="thrynova" version="1" attachment="simplifiedXS_VH_1.1.pdf" attr="" comment="" date="1548547714" name="simplifiedXS_VH_1.1.pdf" path="simplifiedXS_VH_1.1.pdf" size="12312" user="thrynova" version="1" attachment="simplifiedXS_ggF_1.1.png" attr="" comment="" date="1548548003" name="simplifiedXS_ggF_1.1.png" path="simplifiedXS_ggF_1.1.png" size="79420" user="thrynova" version="1" attachment="simplifiedXS_VBF_1.1.png" attr="" comment="" date="1548548006" name="simplifiedXS_VBF_1.1.png" path="simplifiedXS_VBF_1.1.png" size="82818" user="thrynova" version="1" attachment="simplifiedXS_VH_1.1.png" attr="" comment="" date="1548548008" name="simplifiedXS_VH_1.1.png" path="simplifiedXS_VH_1.1.png" size="65852" user="thrynova" version="1"

#### Revision 82019-01-25 - PredragMilenovic

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 6 to 6

## Conveners

• ATLAS: Nicolas Berger (LAPP)
Changed:
<
<
• CMS: Predrag Milenovic (CERN)
>
>
• CMS: Lorenzo Viliani (Firenze)

• Theory: Frank Tackmann (DESY)

## Communication and meetings

#### Revision 72017-05-16 - PredragMilenovic

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 10 to 10

• Theory: Frank Tackmann (DESY)

## Communication and meetings

Changed:
<
<
• Group discussions: lhc-higgs-prop-diSTXS[@]cern.ch
• Contact with conveners: lhc-higgs-diSTXS-convener[@]cern.ch
>
>
• Group discussions: lhc-higgs-prop-fidSTXS[@]cern.ch
• Contact with conveners: lhc-higgs-fidSTXS-convener[@]cern.ch

### Meetings

• Next meeting: TBD
Links to previous meetings on fiducial cross sections:

#### Revision 62017-05-11 - PredragMilenovic

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

#### Revision 52017-05-08 - NicolasBerger

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 65 to 65

### Run 2 results

>
>
• Measurement of fiducial, differential and production cross sections in the H → γγ decay channel with 13.3 fb-1 of 13 TeV proton-proton collision data with the ATLAS detector, ATLAS-CONF-2016-067
• Study of the Higgs boson properties and search for high-mass scalar resonances in the $H→ ZZ^{*}→ 4\ell$ decay channel at √s = 13 TeV with the ATLAS detector, ATLAS-CONF-2016-079
• Combined measurements of the Higgs boson production and decay rates in H→ ZZ* → 4ℓ and H → γγ final states using pp collision data at √s = 13 TeV in the ATLAS experiment, ATLAS-CONF-2016-081

### Run 1 results

• __Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s)=8 TeV using the H→WW

#### Revision 42017-05-08 - FrankTackmann

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"

# Fiducial/Differential and Simplified Template Cross Sections

Line: 13 to 12

• Group discussions: lhc-higgs-prop-diSTXS[@]cern.ch
• Contact with conveners: lhc-higgs-diSTXS-convener[@]cern.ch
Changed:
<
<
• Links to some of the previous meetings
>
>

### Meetings

• Next meeting: TBD
Links to previous meetings on fiducial cross sections:

Changed:
<
<
>
>
Links to previous meetings on STXS:

## Topics of the group

Goal of the group is to discuss and address the issues related to fiducial and differential cross sections as well as simplified template cross sections (STXS) within the WG2 structure.

Line: 27 to 29
In theories beyond the SM, the properties of the 125 GeV Higgs boson may not be determined only by a simple scaling of couplings. Instead, the kinematic distributions in the various Higgs production and decay channels may be sensitively modified by BSM (incl. EFT) effects. Fiducial cross sections (FXS), i.e. cross sections, whether total or differential, for specific states within the phase space de fined by experimental selection and acceptance cuts, provide a largely model-independent way to test for such deviations in kinematic distributions. In particular, differential FXS are a powerful for scrutinizing the SM Lagrangian structure of the Higgs boson interactions, including tests for new tensorial couplings, non-standard production modes, determination of effective form factors, etc.

### Simplified template cross sections (STXS)

Changed:
<
<
The Higgs boson coupling measurements during the LHC Run1 had as their main results measured signal strength and multiplicative coupling modifiers. Simplified template cross sections (STXS) were developed to provide a natural way to evolve these coupling measurements in the future. Compared to the Run1 measurements, the simplified template cross section framework aims to separate more cleanly measurement and interpretation steps in order to reduce in a systematic fashion the theory dependences that must be directly folded into the measurements (including both dependence on the theoretical uncertainties as well as on the underlying physics model). In addition, they provide more finely-grained measurements (and hence more information for theoretical interpretations), while at the same time allowing and benefiting from the global combination of the measurements in all decay channels.
>
>
The Higgs boson coupling measurements during the LHC Run1 had as their main results measured signal strength and multiplicative coupling modifiers. Simplified template cross sections (STXS) were developed to provide a natural way to evolve these coupling measurements in the future. Compared to the Run1 measurements, the STXS framework aims to separate more cleanly measurement and interpretation steps in order to reduce in a systematic fashion the theory dependencies that are folded into the measurements (including both the dependence on theoretical uncertainties and on the underlying physics model). In addition, they provide more finely-grained measurements (and hence more information for theoretical interpretations) while at the same time allowing and benefiting from the global combination of the measurements in all decay channels.

Here is a pictorial overview of the framework. The development was initiated at Les Houches 2015.
Details on the guiding principles, common object definitions, and specific bin definitions are documented in chapter III.2 of YR4 as well as the Les Houches 2015 proceedings.

The primary goals of the STXS framework are to maximize the sensitivity of the measurements while at the same time to minimize their theory dependence. Consequently, some of their defining features are:
• Inclusive over the Higgs decays
Line: 37 to 41

• Allows different efficiencies/acceptances for different production modes without incurring a dependence on the SM production mode mix
• Currently, the main SM production processes act as kinematic templates, in the future more kinematic templates can be added (e.g. for a CP-odd Higgs)
• Non-Higgs backgrounds are substracted
Changed:
<
<
• In the future, one could add templates for BSM sensitive backgrounds (e.g. for pp->WW)
>
>
• In the future, one could add templates for BSM sensitive backgrounds (e.g. for pp->WW)

• Simplified (idealized) bin definitions abstracted from the actual measurement categories
• Allows for some acceptance corrections
• Analyzes can use optimized selection at reconstruction level
The measured exclusive regions of phase space, called “bins” for simplicity, are specific to the different production modes. Their definitions are motivated by
• Minimizing the dependence on theoretical uncertainties that are directly folded into the measurements
• Maximizing experimental sensitivity
Changed:
<
<
• Isolation of possible BSM effects
>
>
• Isolation of possible BSM effects

• Minimizing the number of bins without loss of experimental sensitivity
Since these are competing requirements a nontrivial compromise has to be achieved. In particular, to account for the evolving experimental sensitivity the STXS bins are thus defined in stages (corresponding to increasingly fine granularity)
Changed:
<
<
• Stage 0
• Stage 1
Details on the guiding principles and specific bin definitions can be found in Chapter III.2 of YR4.
>
>

## References

### Run 2 results

Line: 97 to 108

• Probing the spin-parity of the Higgs boson via jet kinematics in vector boson fusion, A. Djouadi, R.M. Godbole, B. Mellado, K. Mohan, arXiv:1301.4965
Deleted:
<
<

-- NicolasBerger - 2017-05-05 \ No newline at end of file
>
>
 META FILEATTACHMENT attachment="simplifiedXS_stage0.pdf" attr="" comment="" date="1494249825" name="simplifiedXS_stage0.pdf" path="simplifiedXS_stage0.pdf" size="10700" user="ftackman" version="1" attachment="simplifiedXS_ggF.pdf" attr="" comment="" date="1494250047" name="simplifiedXS_ggF.pdf" path="simplifiedXS_ggF.pdf" size="13246" user="ftackman" version="1" attachment="simplifiedXS_VBF.pdf" attr="" comment="" date="1494250055" name="simplifiedXS_VBF.pdf" path="simplifiedXS_VBF.pdf" size="13172" user="ftackman" version="1" attachment="simplifiedXS_VH.pdf" attr="" comment="" date="1494250063" name="simplifiedXS_VH.pdf" path="simplifiedXS_VH.pdf" size="12625" user="ftackman" version="1" attachment="simplifiedXS.pdf" attr="" comment="" date="1494250084" name="simplifiedXS.pdf" path="simplifiedXS.pdf" size="18613" user="ftackman" version="1"

#### Revision 32017-05-08 - FrankTackmann

Line: 1 to 1

 META TOPICPARENT name="LHCHXSWG"
Changed:
<
<

>
>

# Fiducial/Differential and Simplified Template Cross Sections

Deleted:
<
<

## General

Goal of the group is to discuss and address the issues related to fiducial cross-sections, differential cross-sections, and simplified template cross-sections (STXS) within the WG2 structure.

## Conveners

• ATLAS: Nicolas Berger (LAPP)
Line: 26 to 21

## Topics of the group

>
>
Goal of the group is to discuss and address the issues related to fiducial and differential cross sections as well as simplified template cross sections (STXS) within the WG2 structure.

### Fiducial and differential cross sections

In theories beyond the SM, the properties of the 125 GeV Higgs boson may not be determined only by a simple scaling of couplings. Instead, the kinematic distributions in the various Higgs production and decay channels may be sensitively modified by BSM (incl. EFT) effects. Fiducial cross sections (FXS), i.e. cross sections, whether total or differential, for specific states within the phase space de fined by experimental selection and acceptance cuts, provide a largely model-independent way to test for such deviations in kinematic distributions. In particular, differential FXS are a powerful for scrutinizing the SM Lagrangian structure of the Higgs boson interactions, including tests for new tensorial couplings, non-standard production modes, determination of effective form factors, etc.

>
>

Changed:
<
<

### Simplified template cross-sections (STXS)

>
>
The Higgs boson coupling measurements during the LHC Run1 had as their main results measured signal strength and multiplicative coupling modifiers. Simplified template cross sections (STXS) were developed to provide a natural way to evolve these coupling measurements in the future. Compared to the Run1 measurements, the simplified template cross section framework aims to separate more cleanly measurement and interpretation steps in order to reduce in a systematic fashion the theory dependences that must be directly folded into the measurements (including both dependence on the theoretical uncertainties as well as on the underlying physics model). In addition, they provide more finely-grained measurements (and hence more information for theoretical interpretations), while at the same time allowing and benefiting from the global combination of the measurements in all decay channels.

>
>
The primary goals of the STXS framework are to maximize the sensitivity of the measurements while at the same time to minimize their theory dependence. Consequently, some of their defining features are:
• Inclusive over the Higgs decays
• This allows one to perform a global combination of all decay channels
• Measure cross sections (instead of signal strengths), in mutually exclusive regions of phase space
• Measure cross sections separated into production modes (or more generally kinematic templates)
• Allows different efficiencies/acceptances for different production modes without incurring a dependence on the SM production mode mix
• Currently, the main SM production processes act as kinematic templates, in the future more kinematic templates can be added (e.g. for a CP-odd Higgs)
• Non-Higgs backgrounds are substracted
• In the future, one could add templates for BSM sensitive backgrounds (e.g. for pp->WW)
• Simplified (idealized) bin definitions abstracted from the actual measurement categories
• Allows for some acceptance corrections
• Analyzes can use optimized selection at reconstruction level
The measured exclusive regions of phase space, called “bins” for simplicity, are specific to the different production modes. Their definitions are motivated by
• Minimizing the dependence on theoretical uncertainties that are directly folded into the measurements
• Maximizing experimental sensitivity
• Isolation of possible BSM effects
• Minimizing the number of bins without loss of experimental sensitivity
Since these are competing requirements a nontrivial compromise has to be achieved. In particular, to account for the evolving experimental sensitivity the STXS bins are thus defined in stages (corresponding to increasingly fine granularity)
• Stage 0
• Stage 1
Details on the guiding principles and specific bin definitions can be found in Chapter III.2 of YR4.

## References

### Run 1 results

Changed:
<
<
• __Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s)=8 TeV using the H→WW
>
>
• __Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s)=8 TeV using the H→WW
decays__, CMS Collaboration, CMS-PAS-HIG-15-010

• Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at sqrt(s)= 7 and 8 TeV, CMS Collaboration, arXiv:1512.08377

• Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at sqrt(s)=8 TeV, CMS Collaboration, arXiv:1508.07819
Changed:
<
<
• Constraints on non-Standard Model Higgs boson interactions in an effective field theory using differential cross sections measured in the H→γγ decay channel at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, arXiv:1508.02507
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• Constraints on non-Standard Model Higgs boson interactions in an effective field theory using differential cross sections measured in the H→γγ decay channel at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, arXiv:1508.02507

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• Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H→γγ and H→ZZ*→4ℓ Decay Channels at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Phys. Rev. Lett. 115, 091801 (2015)
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• Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H→γγ and H→ZZ*→4ℓ Decay Channels at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Phys. Rev. Lett. 115, 091801 (2015)

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• Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in pp collisions at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Physics Letters B 738 (2014) 234-253

• Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at √s=8 TeV with ATLAS, ATLAS Collaboration, JHEP09(2014)112
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• Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in pp collisions at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Physics Letters B 738 (2014) 234-253

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• Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at √s=8 TeV with ATLAS, ATLAS Collaboration, JHEP09(2014)112

### Theory: precision calculations, BSM effects, etc.

#### Revision 22017-05-08 - PredragMilenovic

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# Fiducial/differential and simplified template cross section measurements

## General

Goal of the group is to discuss and address the issues related to fiducial cross-sections, differential cross-sections, and simplified template cross-sections (STXS) within the WG2 structure.

## Conveners

• ATLAS: Nicolas Berger (LAPP)
• CMS: Predrag Milenovic (CERN)
• Theory: Frank Tackmann (DESY)

## Communication and meetings

• Group discussions: lhc-higgs-prop-diSTXS[@]cern.ch
• Contact with conveners: lhc-higgs-diSTXS-convener[@]cern.ch

## Topics of the group

### Fiducial and differential cross sections

In theories beyond the SM, the properties of the 125 GeV Higgs boson may not be determined only by a simple scaling of couplings. Instead, the kinematic distributions in the various Higgs production and decay channels may be sensitively modified by BSM (incl. EFT) effects. Fiducial cross sections (FXS), i.e. cross sections, whether total or differential, for specific states within the phase space de fined by experimental selection and acceptance cuts, provide a largely model-independent way to test for such deviations in kinematic distributions. In particular, differential FXS are a powerful for scrutinizing the SM Lagrangian structure of the Higgs boson interactions, including tests for new tensorial couplings, non-standard production modes, determination of effective form factors, etc.

## References

### Run 1 results

• Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at sqrt(s)=8 TeV using the H→WW decays, CMS Collaboration, CMS-PAS-HIG-15-010

• Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at sqrt(s)= 7 and 8 TeV, CMS Collaboration, arXiv:1512.08377

• Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at sqrt(s)=8 TeV, CMS Collaboration, arXiv:1508.07819

• Constraints on non-Standard Model Higgs boson interactions in an effective field theory using differential cross sections measured in the H→γγ decay channel at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, arXiv:1508.02507

• Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H→γγ and H→ZZ*→4ℓ Decay Channels at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Phys. Rev. Lett. 115, 091801 (2015)

• Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in pp collisions at √s=8 TeV with the ATLAS detector, ATLAS Collaboration, Physics Letters B 738 (2014) 234-253

• Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at √s=8 TeV with ATLAS, ATLAS Collaboration, JHEP09(2014)112

### Theory: precision calculations, BSM effects, etc.

Selected references, certainly incomplete. Let us know to add your paper.

• High energy resummation of transverse momentum distributions:Higgs in gluon fusion, Stefano Forte, Claudio Muselli, arXiv:1511.05561

• Resummation ambiguities in the Higgs transverse-momentum spectrum in the Standard Model and beyond, Emanuele Bagnaschi, Robert V. Harlander, Hendrik Mantler, Alessandro Vicini, Marius Wiesemann, arXiv:1510.08850

• Pushing Higgs Effective Theory to its Limits, Johann Brehmer, Ayres Freitas, David Lopez-Val, Tilman Plehn, arXiv:1510.03443

• Fiducial cross sections for Higgs boson production in association with a jet at next-to-next-to-leading order in QCD, Fabrizio Caola, Kirill Melnikov, Markus Schulze arXiv:1508.02684

• Benchmarks for Higgs Effective Theory: Extended Higgs Sectors, Martin Gorbahn, Jose Miguel No, Veronica Sanz, arXiv:1502.07352

• Mass Effects in the Higgs-Gluon Coupling: Boosted vs Off-Shell Production, Malte Buschmann, Dorival Goncalves, Silvan Kuttimalai, Marek Schonherr, Frank Krauss, Tilman Plehn, arXiv:1410.5806

• Resolving the Higgs-Gluon Coupling with Jets, Malte Buschman, Christoph Englert, Dorival Goncalves, Tilman Plehn, Michael Spannowsky, arXiv:1405.7651

• Complete Higgs Sector Constraints on Dimension-6 Operators, John Ellis, Veronica Sanz, Tevong You, arXiv:1404.3667

• Probing Higgs couplings with high pT Higgs production, Aleksandr Azatov, Ayan Paul, arXiv:1309.5273

• Probing top-partners in Higgs+jets, Andrea Banfi, Adam Martin, Veronica Sanz, arXiv:1308.4771

• Probing the spin-parity of the Higgs boson via jet kinematics in vector boson fusion, A. Djouadi, R.M. Godbole, B. Mellado, K. Mohan, arXiv:1301.4965

-- NicolasBerger - 2017-05-05

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