REVIEW 2 minor 93 references
Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\gamma\gamma$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV
T0 review · 0 major / 2 minor · reviewed 2026-05-15 · grok-4.3
Pith's one-line read Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.
desk verdict CMS reports updated constraints on anomalous Higgs couplings from the full Run 2 diphoton data, consistent with the Standard Model. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
Extended reading notes
Core claim
The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.
Load-bearing premise
The matrix element techniques and multivariate discriminants correctly categorize events and separate signal from background without significant bias from unmodeled effects.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript reports constraints on anomalous Higgs boson couplings to vector bosons and fermions using the diphoton decay channel in 138 fb^{-1} of 13 TeV proton-proton collision data collected by CMS. Events are categorized into gluon-fusion, vector-boson-fusion, and associated-production modes via matrix-element techniques and multivariate discriminants; the CP properties of the gluon couplings and the tensor structure of the electroweak couplings are examined. Results are presented as fractional contributions of anomalous couplings to each production cross section and found consistent with Standard Model expectations.
Significance. If the central results hold, the work supplies competitive, data-driven limits on dimension-6 operator contributions to Higgs production, exploiting the clean diphoton final state and a large dataset. The combination of matrix-element discriminants, BDT categorization, and a binned likelihood fit to the diphoton mass plus discriminant outputs constitutes a standard yet robust EFT-style analysis whose consistency checks (closure tests, control-region validation) support the reported SM agreement.
minor comments (2)
- [Abstract] The abstract states consistency with SM expectations but omits any quantitative indication of the fit uncertainties or the dominant systematic sources; adding a single sentence summarizing the leading uncertainties would improve readability without altering the technical content.
- [Signal modeling] Section describing the signal reweighting procedure should explicitly state the range of anomalous coupling values used to generate the templates and confirm that the reweighting preserves the normalization of the SM component.
Simulated Author's Rebuttal
We thank the referee for the careful reading and positive assessment of the manuscript. The analysis provides updated constraints on anomalous Higgs boson couplings to vector bosons and fermions in the diphoton channel using the full Run 2 dataset of 138 fb^{-1}. The results remain consistent with Standard Model expectations across gluon-fusion, vector-boson-fusion, and associated-production modes. No major comments were raised in the report.
Assumptions & free parameters
assumptions (1)
- domain assumption Standard model predictions for Higgs production cross sections and decay branching ratios are accurate enough for background subtraction and signal modeling.
Cite this review
Pith. "Pith review of Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\gamma\gamma$ final state in proton-proton collisions at $\sqrt{s}$ = 13 TeV." pith.science (2026). https://pith.science/paper/KOITDP7P
@misc{pith2026260514245,
author = {Pith},
title = {Pith review of: Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\gamma\gamma$ final state in proton-proton collisions at $\sqrts$ = 13 TeV},
year = {2026},
howpublished = {\url{https://pith.science/paper/KOITDP7P}},
note = {Machine review of arXiv:2605.14245}
}
abstract
Possible anomalous couplings of the Higgs boson to vector bosons and fermions are studied using Higgs boson candidates decaying to a pair of photons. The study is based on proton-proton collision data at $\sqrt{s}$ = 13 TeV collected by the CMS experiment, corresponding to an integrated luminosity of 138 fb$^{-1}$. Events with Higgs boson candidates produced via gluon fusion, electroweak vector boson fusion and in association with a vector boson, are categorized using matrix element techniques and multivariate discriminants. The $CP$ properties of the Higgs boson couplings to gluons through loops of heavy particles, as well as the tensor structure of its interactions with two electroweak bosons, are investigated. The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.
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unclearRelation between the paper passage and the cited Recognition theorem.
The results are interpreted in terms of the fractional contributions of anomalous Higgs boson couplings to the total production cross section of each process and are found to be consistent with the standard model expectations.
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IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Events ... are categorized using matrix element techniques and multivariate discriminants.
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Reference graph
Works this paper leans on
-
[1]
ATLAS Collaboration, “Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC”,Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214
work page Pith review arXiv doi:10.1016/j.physletb.2012.08.020 2012
-
[2]
Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC
CMS Collaboration, “Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC”,Phys. Lett. B716(2012) 30, doi:10.1016/j.physletb.2012.08.021,arXiv:1207.7235
work page Pith review arXiv doi:10.1016/j.physletb.2012.08.021 2012
-
[3]
Observation of a new boson with mass near 125 GeV in pp collisions at sqrt(s) = 7 and 8 TeV
CMS Collaboration, “Observation of a new boson with mass near 125 GeV in pp collisions at √s= 7 and 8 TeV”,JHEP06(2013) 081, doi:10.1007/JHEP06(2013)081,arXiv:1303.4571
work page Pith review arXiv doi:10.1007/jhep06(2013)081 2013
-
[4]
doi: 10.1016/0029-5582(61)90469-2
S. L. Glashow, “Partial-symmetries of weak interactions”,Nucl. Phys.22(1961) 579, doi:10.1016/0029-5582(61)90469-2
-
[5]
F. Englert and R. Brout, “Broken symmetry and the mass of gauge vector mesons”,Phys. Rev. Lett.13(1964) 321,doi:10.1103/PhysRevLett.13.321
-
[6]
Broken symmetries, massless particles and gauge fields
P . W. Higgs, “Broken symmetries, massless particles and gauge fields”,Phys. Lett.12 (1964) 132,doi:10.1016/0031-9163(64)91136-9
-
[7]
Broken Symmetries and the Masses of Gauge Bosons
P . W. Higgs, “Broken symmetries and the masses of gauge bosons”,Phys. Rev. Lett.13 (1964) 508,doi:10.1103/PhysRevLett.13.508
-
[8]
Global conservation laws and massless particles
G. S. Guralnik, C. R. Hagen, and T. W. B. Kibble, “Global conservation laws and massless particles”,Phys. Rev. Lett.13(1964) 585,doi:10.1103/PhysRevLett.13.585
Show all 93 references
-
[9]
A model of leptons
S. Weinberg, “A model of leptons”,Phys. Rev. Lett.19(1967) 1264, doi:10.1103/PhysRevLett.19.1264
1967 doi
-
[10]
Weak and electromagnetic interactions
A. Salam, “Weak and electromagnetic interactions”,Conf. Proc. C680519(1968) 367, doi:10.1142/9789812795915_0034
1968 doi
-
[11]
Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV
CMS Collaboration, “Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV”,Phys. Rev. D92(2015) 012004, doi:10.1103/PhysRevD.92.012004,arXiv:1411.3441
-
[12]
Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector
ATLAS Collaboration, “Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector”,Eur. Phys. J. C75(2015) 476, doi:10.1140/epjc/s10052-015-3685-1,arXiv:1506.05669. 34
-
[13]
Study of the mass and spin-parity of the Higgs boson candidate via its decays to Z boson pairs
CMS Collaboration, “Study of the mass and spin-parity of the Higgs boson candidate via its decays to Z boson pairs”,Phys. Rev. Lett.110(2013) 081803, doi:10.1103/PhysRevLett.110.081803,arXiv:1212.6639
- [14]
- [15]
- [16]
-
[17]
Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state
CMS Collaboration, “Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state”,Phys. Lett. B775(2017) 1, doi:10.1016/j.physletb.2017.10.021,arXiv:1707.00541
-
[18]
Measurements of the Higgs boson width and anomalous HVV couplings from on-shell and off-shell production in the four-lepton final state
CMS Collaboration, “Measurements of the Higgs boson width and anomalous HVV couplings from on-shell and off-shell production in the four-lepton final state”,Phys. Rev. D99(2019) 112003,doi:10.1103/PhysRevD.99.112003,arXiv:1901.00174
-
[19]
Constraints on anomalous HVV couplings from the production of Higgs bosons decaying toτlepton pairs
CMS Collaboration, “Constraints on anomalous HVV couplings from the production of Higgs bosons decaying toτlepton pairs”,Phys. Rev. D100(2019) 112002, doi:10.1103/PhysRevD.100.112002,arXiv:1903.06973
2019 doi
-
[20]
Measurements of t ¯tH production and theCPstructure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel
CMS Collaboration, “Measurements of t ¯tH production and theCPstructure of the Yukawa interaction between the Higgs boson and top quark in the diphoton decay channel”,Phys. Rev. Lett.125(2020) 061801, doi:10.1103/PhysRevLett.125.061801,arXiv:2003.10866
2020 doi
-
[21]
Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state
CMS Collaboration, “Constraints on anomalous Higgs boson couplings to vector bosons and fermions in its production and decay using the four-lepton final state”,Phys. Rev. D 104(2021) 052004,doi:10.1103/PhysRevD.104.052004,arXiv:2104.12152
2021 doi
-
[22]
Analysis of theCPstructure of the Yukawa coupling between the Higgs boson andτleptons in proton-proton collisions at √s=13 TeV
CMS Collaboration, “Analysis of theCPstructure of the Yukawa coupling between the Higgs boson andτleptons in proton-proton collisions at √s=13 TeV”,JHEP06(2022) 012,doi:10.1007/jhep06(2022)012,arXiv:2110.04836
2022 doi
-
[23]
Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
CMS Collaboration, “Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production”,Nature Phys.18(2022) 1329, doi:10.1038/s41567-022-01682-0,arXiv:2202.06923
2022 doi
- [24]
-
[25]
Test of CP invariance in vector-boson fusion production of the Higgs boson using the optimal observable method in the ditau decay channel with the ATLAS detector
ATLAS Collaboration, “Test of CP invariance in vector-boson fusion production of the Higgs boson using the optimal observable method in the ditau decay channel with the ATLAS detector”,Eur. Phys. J. C76(2016) 658, doi:10.1140/epjc/s10052-016-4499-5,arXiv:1602.04516. References 35
-
[26]
Measurement of inclusive and differential cross sections in the H→ZZ ∗ →4ℓdecay channel in pp collisions at √s=13 TeV with the ATLAS detector
ATLAS Collaboration, “Measurement of inclusive and differential cross sections in the H→ZZ ∗ →4ℓdecay channel in pp collisions at √s=13 TeV with the ATLAS detector”, JHEP10(2017) 132,doi:10.1007/JHEP10(2017)132,arXiv:1708.02810
-
[27]
Measurement of the Higgs boson coupling properties in the H→ZZ ∗ →4ℓdecay channel at √s=13 TeV with the ATLAS detector
ATLAS Collaboration, “Measurement of the Higgs boson coupling properties in the H→ZZ ∗ →4ℓdecay channel at √s=13 TeV with the ATLAS detector”,JHEP03 (2018) 095,doi:10.1007/JHEP03(2018)095,arXiv:1712.02304
-
[28]
Measurements of Higgs boson properties in the diphoton decay channel with 36 fb−1 of pp collision data at √s=13 TeV with the ATLAS detector
ATLAS Collaboration, “Measurements of Higgs boson properties in the diphoton decay channel with 36 fb−1 of pp collision data at √s=13 TeV with the ATLAS detector”,Phys. Rev. D98(2018) 052005,doi:10.1103/PhysRevD.98.052005,arXiv:1802.04146
-
[29]
Test of CP invariance in vector-boson fusion production of the Higgs boson in the H→ττchannel in proton-proton collisions at √s=13 TeV with the ATLAS detector
ATLAS Collaboration, “Test of CP invariance in vector-boson fusion production of the Higgs boson in the H→ττchannel in proton-proton collisions at √s=13 TeV with the ATLAS detector”,Phys. Lett. B805(2020) 135426, doi:10.1016/j.physletb.2020.135426,arXiv:2002.05315
2020 doi
-
[30]
CPproperties of Higgs boson interactions with top quarks in the ttH and tH processes using H→γγwith the ATLAS detector
ATLAS Collaboration, “CPproperties of Higgs boson interactions with top quarks in the ttH and tH processes using H→γγwith the ATLAS detector”,Phys. Rev. Lett.125 (2020) 061802,doi:10.1103/PhysRevLett.125.061802,arXiv:2004.04545
2020 doi
-
[31]
Constraints on Higgs boson properties using WW ∗(→eνµν)jj production in 36.1 fb−1 of √s=13 TeV pp collisions with the ATLAS detector
ATLAS Collaboration, “Constraints on Higgs boson properties using WW ∗(→eνµν)jj production in 36.1 fb−1 of √s=13 TeV pp collisions with the ATLAS detector”, 2022. arXiv:2109.13808. Published inEur. Phys. J. C
2022
-
[32]
Determining the cp nature of a neutral higgs boson at the cern large hadron collider
J. F. Gunion and X.-G. He, “Determining the cp nature of a neutral higgs boson at the cern large hadron collider”,Phys. Rev. Lett.76(Jun, 1996) 4468, doi:10.1103/PhysRevLett.76.4468
1996 doi
-
[33]
The CMS experiment at the CERN LHC
CMS Collaboration, “The CMS experiment at the CERN LHC”,JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004
2008 doi
-
[34]
Development of the CMS detector for the CERN LHC Run 3
CMS Collaboration, “Development of the CMS detector for the CERN LHC Run 3”, JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466
2024 doi
-
[35]
Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at√s=13 TeV
CMS Collaboration, “Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at√s=13 TeV”,Eur. Phys. J. C84(2024) 779, doi:10.1140/epjc/s10052-024-12925-0,arXiv:2403.00657
2024 doi
-
[36]
Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using theττfinal state
CMS Collaboration, “Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using theττfinal state”,Phys. Rev. D 108(2023) 032013,doi:10.1103/PhysRevD.108.032013,arXiv:2205.05120
2023 doi
-
[37]
HEPData record for this analysis, 2026.doi:10.17182/hepdata.169546
2026 doi
- [38]
- [39]
-
[40]
Proceedings of the Workshop on CP studies and non-standard Higgs physics
S. Kraml et al., “Proceedings of the Workshop on CP studies and non-standard Higgs physics”, inProc. Workshop on CP studies and non-standard Higgs physics. 2006. arXiv:hep-ph/0608079.doi:10.5170/CERN-2006-009
2006 doi
- [41]
- [42]
- [43]
- [44]
- [45]
- [46]
- [47]
- [48]
- [49]
-
[50]
Constraining anomalous Higgs boson couplings to the heavy flavor fermions using matrix element techniques
A. V . Gritsan, R. R¨ontsch, M. Schulze, and M. Xiao, “Constraining anomalous Higgs boson couplings to the heavy flavor fermions using matrix element techniques”,Phys. Rev. D94(2016) 055023,doi:10.1103/PhysRevD.94.055023,arXiv:1606.03107
2016 doi
-
[51]
Constraining anomalous Higgs boson couplings to virtual photons
J. Davis et al., “Constraining anomalous Higgs boson couplings to virtual photons”, Phys. Rev. D105(2022) 096027,doi:10.1103/PhysRevD.105.096027, arXiv:2109.13363
2022 doi
-
[52]
New features in the JHU generator framework: constraining Higgs boson properties from on-shell and off-shell production
A. V . Gritsan et al., “New features in the JHU generator framework: constraining Higgs boson properties from on-shell and off-shell production”,Phys. Rev. D102(2020) 056022, doi:10.1103/PhysRevD.102.056022,arXiv:2002.09888
2020 doi
- [53]
-
[54]
Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV
CMS Collaboration, “Measurements of Higgs boson production cross sections and couplings in the diphoton decay channel at √s = 13 TeV”,JHEP07(2021) 027, doi:10.1007/JHEP07(2021)027,arXiv:2103.06956. References 37
2021 doi
-
[55]
Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV
CMS Collaboration, “Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV”,JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165
2020 doi
- [56]
-
[57]
Performance of the CMS high-level trigger during LHC Run 2
CMS Collaboration, “Performance of the CMS high-level trigger during LHC Run 2”, JINST19(2024) P11021,doi:10.1088/1748-0221/19/11/P11021, arXiv:2410.17038
2024 doi
-
[58]
Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS
CMS Collaboration, “Precision luminosity measurement in proton-proton collisions at√s=13 TeV in 2015 and 2016 at CMS”,Eur. Phys. J. C81(2021) 800, doi:10.1140/epjc/s10052-021-09538-2,arXiv:2104.01927
2015 doi
-
[59]
CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV
CMS Collaboration, “CMS luminosity measurement for the 2017 data-taking period at√s=13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-17-004, 2018
2017
-
[60]
CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV
CMS Collaboration, “CMS luminosity measurement for the 2018 data-taking period at√s=13 TeV”, CMS Physics Analysis Summary CMS-PAS-LUM-18-002, 2019
2018
-
[61]
Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at √s=7 TeV
CMS Collaboration, “Measurement of the Inclusive W and Z Production Cross Sections in pp Collisions at √s=7 TeV”,JHEP10(2011) 132,doi:10.1007/JHEP10(2011)132
2011 doi
- [62]
-
[63]
Event generator tunes obtained from underlying event and multiparton scattering measurements
CMS Collaboration, “Event generator tunes obtained from underlying event and multiparton scattering measurements”,Eur. Phys. J. C76(2016) 155, doi:10.1140/epjc/s10052-016-3988-x,arXiv:1512.00815
-
[64]
Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements
CMS Collaboration, “Extraction and validation of a new set of CMS PYTHIA8 tunes from underlying-event measurements”,Eur. Phys. J. C80(2020) 4, doi:10.1140/epjc/s10052-019-7499-4,arXiv:1903.12179
2020 doi
- [65]
- [66]
-
[67]
Handbook of LHC Higgs Cross Sections: 4. Deciphering the nature of the Higgs sector
LHC Higgs Cross Section Working Group, “Handbook of LHC Higgs Cross Sections: 4. Deciphering the nature of the Higgs sector”,CERN Y ellow Rep. Monogr.2(2017) doi:10.23731/CYRM-2017-002,arXiv:1610.07922
-
[68]
GEANT4—a simulation toolkit
GEANT4 Collaboration, “GEANT4—a simulation toolkit”,Nucl. Instrum. Meth. A506 (2003) 250,doi:10.1016/S0168-9002(03)01368-8
2003 doi
-
[69]
The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
J. Alwall et al., “The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations”,JHEP07 (2014) 079,doi:10.1007/JHEP07(2014)079,arXiv:1405.0301
- [70]
- [71]
- [72]
- [73]
-
[74]
A general framework for implementing NLO calculations in shower Monte Carlo programs: thePOWHEGBOX
S. Alioli, P . Nason, C. Oleari, and E. Re, “A general framework for implementing NLO calculations in shower Monte Carlo programs: thePOWHEGBOX”,JHEP06(2010) 043, doi:10.1007/JHEP06(2010)043,arXiv:1002.2581
- [75]
-
[76]
An interface between thePOWHEG BOXand MADGRAPH5 aMC@NLO
P . Nason, C. Oleari, M. Rocco, and M. Zaro, “An interface between thePOWHEG BOXand MADGRAPH5 aMC@NLO”,Eur. Phys. J. C80(2020) 10, doi:10.1140/epjc/s10052-020-08559-7,arXiv:2008.06364
2020 doi
- [77]
- [78]
-
[79]
Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC
A. M. Sirunyan et al., “Electron and photon reconstruction and identification with the CMS experiment at the CERN LHC”,Journal of Instrumentation16(2021) doi:10.1088/1748-0221/16/05/p05014
2021 doi
- [80]
- [81]
- [82]
-
[83]
Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector
CMS Collaboration, “Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector”,JINST14(2019) P07004,doi:10.1088/1748-0221/14/07/P07004,arXiv:1903.06078
-
[84]
A measurement of the Higgs boson mass in the diphoton decay channel
CMS Collaboration, “A measurement of the Higgs boson mass in the diphoton decay channel”,Phys. Lett. B805(2020) 135425,doi:10.1016/j.physletb.2020.135425, arXiv:2002.06398. References 39
2020 doi
-
[85]
Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV
CMS Collaboration, “Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV”,Eur. Phys. J. C75(2015) 212, doi:10.1140/epjc/s10052-015-3351-7,arXiv:1412.8662
-
[86]
The CMS statistical analysis and combination tool: COMBINE
CMS Collaboration, “The CMS statistical analysis and combination tool: COMBINE”, Comput. Softw. Big Sci.8(2024) 19,doi:10.1007/s41781-024-00121-4, arXiv:2404.06614
2024 doi
-
[87]
Extended maximum likelihood
R. J. Barlow, “Extended maximum likelihood”,Nucl. Instrum. Meth. A297(1990) 496, doi:10.1016/0168-9002(90)91334-8
1990 doi
-
[88]
The large-sample distribution of the likelihood ratio for testing composite hypotheses
S. S. Wilks, “The large-sample distribution of the likelihood ratio for testing composite hypotheses”,Ann. Math. Stat.9(1938) 60,doi:10.1214/aoms/1177732360
1938 doi
-
[89]
Cover your bases: asymptotic distributions of the profile likelihood ratio when constraining effective field theories in high-energy physics
F. U. Bernlochner, D. C. Fry, S. B. Menary, and E. Persson, “Cover your bases: asymptotic distributions of the profile likelihood ratio when constraining effective field theories in high-energy physics”,SciPost Phys. Core6(2023) 013, doi:10.21468/SciPostPhysCore.6.1.013,arXiv:...
2023 doi
-
[90]
Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements
CMS Collaboration, “Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements”, 2025. arXiv:2504.02958. Submitted toEur. Phys. J. C
2025 arXiv
-
[91]
On the interpretation ofχ 2 from contingency tables, and the calculation of p
R. A. Fisher, “On the interpretation ofχ 2 from contingency tables, and the calculation of p”,J. Royal Stat. Soc.85(1922) 87,doi:10.2307/2340521
1922 doi
- [92]
-
[93]
Observation of the diphoton decay of the Higgs boson and measurement of its properties
CMS Collaboration, “Observation of the diphoton decay of the Higgs boson and measurement of its properties”,Eur. Phys. J. C74(2014) 3076, doi:10.1140/epjc/s10052-014-3076-z,arXiv:1407.0558. 40 41 A The CMS Collaboration Yerevan Physics Institute, Yerevan, Armenia A. Hayrapetya...
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