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000645822 0247_ $$2doi$$a10.21468/SciPostPhysCommRep.15
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000645822 0247_ $$2inspire$$ainspire:1738820
000645822 0247_ $$2arXiv$$aarXiv:1906.02754
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000645822 041__ $$aEnglish
000645822 088__ $$2arXiv$$aarXiv:1906.02754
000645822 088__ $$2Other$$aLHCHXSWG-2019-003
000645822 088__ $$2DESY$$aDESY 19-070
000645822 088__ $$2Other$$aLHCHWG-INT-2025-001
000645822 088__ $$2DESY$$aDESY-19-070
000645822 1001_ $$aBerger, Nicolas$$b0
000645822 245__ $$aSimplified template cross sections – Stage 1.1 and 1.2
000645822 260__ $$c2026
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000645822 500__ $$aSciPost Phys. Comm. Rep. 15 (2026). 14 pages, 4 figures; v2: added stage 1.2 / Missing Journal: SciPost Physics Community Reports (SciPost Phys. Comm. Rep.) = 3051-3197 (import from CrossRef, INSPIRE, Journals: bib-pubdb1.desy.de)
000645822 520__ $$aSimplified Template Cross Sections (STXS) have been adopted by the LHC experiments as a common framework for Higgs measurements. Their purpose is to reduce the theoretical uncertainties that are directly folded into the measurements as much as possible, while at the same time allowing for the combination of the measurements between different decay channels as well as between experiments. We report the complete, revised definition of the STXS kinematic bins (stage 1.1 and stage 1.2), which have been used for the measurements by the ATLAS and CMS experiments using the full LHC Run 2 datasets. The main focus is on the four dominant Higgs production processes, namely gluon-fusion, vector-boson fusion, production in association with a vector boson and in association with a $t\bar t$ pair. We also comment briefly on the treatment of other production modes.
000645822 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0
000645822 536__ $$0G:(GEPRIS)390833306$$aDFG project G:(GEPRIS)390833306 - EXC 2121: Das Quantisierte Universum II (390833306)$$c390833306$$x1
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000645822 650_7 $$2INSPIRE$$avector boson: fusion
000645822 650_7 $$2INSPIRE$$aCERN LHC Coll
000645822 650_7 $$2INSPIRE$$akinematics
000645822 650_7 $$2INSPIRE$$aATLAS
000645822 650_7 $$2INSPIRE$$aCMS
000645822 650_7 $$2INSPIRE$$aHiggs particle: production
000645822 650_7 $$2INSPIRE$$agluon: fusion
000645822 650_7 $$2INSPIRE$$avector boson: associated production
000645822 650_7 $$2INSPIRE$$across section
000645822 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000645822 7001_ $$aBertella, Claudia$$b1
000645822 7001_ $$aBonanomi, Matteo$$b2
000645822 7001_ $$aBrahimi, Nihal$$b3
000645822 7001_ $$aCalvet, Thomas P.$$b4
000645822 7001_ $$aCalvetti, Milene$$b5
000645822 7001_ $$aDao, Valerio$$b6
000645822 7001_ $$aDelmastro, Marco$$b7
000645822 7001_ $$aDuehrssen-Debling, Michael$$b8
000645822 7001_ $$aFrancavilla, Paolo$$b9
000645822 7001_ $$aHaddad, Yacine$$b10
000645822 7001_ $$aHeim, Sarah$$b11
000645822 7001_ $$aJovicevic, Jelena$$b12
000645822 7001_ $$aKivernyk, Oleh$$b13
000645822 7001_ $$aMoreno Llacer, Maria$$b14
000645822 7001_ $$aLangford, Jonathon M.$$b15
000645822 7001_ $$aLi, Changqiao$$b16
000645822 7001_ $$aMarchiori, Giovanni$$b17
000645822 7001_ $$aMcFayden, Josh A.$$b18
000645822 7001_ $$aMichel, Johannes K. L.$$b19
000645822 7001_ $$aMilenovic, Predrag$$b20
000645822 7001_ $$aPandini, Carlo E.$$b21
000645822 7001_ $$aScott, Edward$$b22
000645822 7001_ $$0P:(DE-H253)PIP1015356$$aTackmann, Frank J.$$b23$$udesy
000645822 7001_ $$0P:(DE-H253)PIP1013754$$aTackmann, Kerstin$$b24$$udesy
000645822 7001_ $$aViliani, Lorenzo$$b25
000645822 7001_ $$aXiao, Meng$$b26
000645822 7001_ $$aYang, Hongtao$$b27
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