000 | 03404nlm1a2200445 4500 | ||
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001 | 663571 | ||
005 | 20231030041859.0 | ||
035 | _a(RuTPU)RU\TPU\network\34741 | ||
090 | _a663571 | ||
100 | _a20210219a2019 k y0engy50 ba | ||
101 | 0 | _aeng | |
102 | _aUS | ||
135 | _adrcn ---uucaa | ||
181 | 0 | _ai | |
182 | 0 | _ab | |
200 | 1 |
_aMeasurement of the top quark polarization and t¯t spin correlations using dilepton final states in proton-proton collisions at √s=13 TeV _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: 81 tit.] | ||
330 | _aMeasurements of the top quark polarization and top quark pair (t¯t) spin correlations are presented using events containing two oppositely charged leptons (e+e−, e±μ∓, or μ+μ−) produced in proton-proton collisions at a center-of-mass energy of 13 TeV. The data were recorded by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb−1. A set of parton-level normalized differential cross sections, sensitive to each of the independent coefficients of the spin-dependent parts of the t¯t production density matrix, is measured for the first time at 13 TeV. The measured distributions and extracted coefficients are compared with standard model predictions from simulations at next-to-leading-order (NLO) accuracy in quantum chromodynamics (QCD), and from NLO QCD calculations including electroweak corrections. All measurements are found to be consistent with the expectations of the standard model. The normalized differential cross sections are used in fits to constrain the anomalous chromomagnetic and chromoelectric dipole moments of the top quark to −0.24<CtG/Λ2<0.07 TeV−2 and −0.33<CItG/Λ2<0.20 TeV−2, respectively, at the 95% confidence level. | ||
333 | _aРежим доступа: по договору с организацией-держателем ресурса | ||
461 |
_tPhysical Review D _oparticles, fields, gravitation, and cosmology _d1970- |
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463 |
_tVol. 100, iss. 7 _v[072002, 39 p.] _d2019 |
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610 | 1 | _aэлектронный ресурс | |
610 | 1 | _aтруды учёных ТПУ | |
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 |
_aZhokin _bA. S. _gAleksandr Sergeevich |
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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 |
_aYuzhakov _bA. D. _gAleksandr Dmitrievich |
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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 _c20211117 _gRCR |
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856 | 4 | _uhttps://doi.org/10.1103/PhysRevD.100.072002 | |
942 | _cCF |