000 | 03150nlm1a2200421 4500 | ||
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001 | 662512 | ||
005 | 20231030041823.0 | ||
035 | _a(RuTPU)RU\TPU\network\33667 | ||
090 | _a662512 | ||
100 | _a20200827a2019 k y0engy50 ba | ||
101 | 0 | _aeng | |
135 | _adrcn ---uucaa | ||
181 | 0 | _ai | |
182 | 0 | _ab | |
200 | 1 |
_aCombined measurements of Higgs boson couplings in proton–proton collisions at √s=13TeV _fA. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.] |
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203 |
_aText _celectronic |
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300 | _aTitle screen | ||
320 | _a[References: 131 tit.] | ||
330 | _aCombined measurements of the production and decay rates of the Higgs boson, as well as its couplings to vector bosons and fermions, are presented. The analysis uses the LHC proton-proton collision data set recorded with the CMS detector in 2016 at s√=13TeVs=13TeV, corresponding to an integrated luminosity of 35.9fb−1fb−1. The combination is based on analyses targeting the five main Higgs boson production mechanisms (gluon fusion, vector boson fusion, and associated production with a WW or ZZ boson, or a top quark-antiquark pair) and the following decay modes: H→γγH→γγ, ZZZZ, WWWW, ττττ, bbbb, and μμμμ. Searches for invisible Higgs boson decays are also considered. The best-fit ratio of the signal yield to the standard model expectation is measured to be μ=1.17±0.10μ=1.17±0.10, assuming a Higgs boson mass of 125.09GeV125.09GeV. Additional results are given for various assumptions on the scaling behavior of the production and decay modes, including generic parametrizations based on ratios of cross sections and branching fractions or couplings. The results are compatible with the standard model predictions in all parametrizations considered. In addition, constraints are placed on various two Higgs doublet models. | ||
461 | _tEuropean Physical Journal C | ||
463 |
_tVol. 79, iss. 5 _v[421, 44 p.] _d2019 |
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610 | 1 | _aэлектронный ресурс | |
610 | 1 | _aтруды учёных ТПУ | |
610 | 1 | _aбозон Хиггса | |
610 | 1 | _aZ-бозоны | |
610 | 1 | _aпротон-протонные соударения | |
701 | 1 |
_aSirunyan _bA. M. |
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701 | 1 |
_aTumasyan _bA. R. |
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701 | 1 |
_aAdam _bW. _gWolfgang |
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701 | 1 |
_aAmbrogi _bF. _gFederico |
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701 | 1 |
_aAsilar _bE. _gEce |
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701 | 1 |
_aBergauer _bT. _gThomas |
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701 | 1 |
_aBabaev _bA. A. _cphysicist _cengineer-issledovatelskogo Polytechnic University, candidate of physical and mathematical Sciences _f1981- _gAnton Anatoljevich _2stltpush _3(RuTPU)RU\TPU\pers\35154 |
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701 | 1 |
_aOkhotnikov _bV. V. _cphysicist _cengineer of Tomsk Polytechnic University _f1992- _gVitaly Vladimirovich _2stltpush _3(RuTPU)RU\TPU\pers\36453 |
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712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИсследовательская школа физики высокоэнергетических процессов _c(2017- ) _h8118 _2stltpush _3(RuTPU)RU\TPU\col\23551 |
801 | 2 |
_aRU _b63413507 _c20201012 _gRCR |
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856 | 4 | _uhttps://doi.org/10.1140/epjc/s10052-019-6909-y | |
942 | _cCF |