000 | 03829nlm1a2200469 4500 | ||
---|---|---|---|
001 | 662583 | ||
005 | 20231030041826.0 | ||
035 | _a(RuTPU)RU\TPU\network\33738 | ||
090 | _a662583 | ||
100 | _a20200907a2019 k y0engy50 ba | ||
101 | 0 | _aeng | |
135 | _adrcn ---uucaa | ||
181 | 0 | _ai | |
182 | 0 | _ab | |
200 | 1 |
_aSearch for supersymmetry in proton-proton collisions at 13 TeV in final states with jets and missing transverse momentum _fA. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.] |
|
203 |
_aText _celectronic |
||
300 | _aTitle screen | ||
320 | _a[References: 102 tit.] | ||
330 | _aResults are reported from a search for supersymmetric particles in the final state with multiple jets and large missing transverse momentum. The search uses a sample of proton-proton collisions at sv = 13 TeV collected with the CMS detector in 2016–2018, corresponding to an integrated luminosity of 137 fb-1, representing essentially the full LHC Run 2 data sample. The analysis is performed in a four-dimensional search region defined in terms of the number of jets, the number of tagged bottom quark jets, the scalar sum of jet transverse momenta, and the magnitude of the vector sum of jet transverse momenta. No significant excess in the event yield is observed relative to the expected background contributions from standard model processes. Limits on the pair production of gluinos and squarks are obtained in the framework of simplified models for supersymmetric particle production and decay processes. Assuming the lightest supersymmetric particle to be a neutralino, lower limits on the gluino mass as large as 2000 to 2310 GeV are obtained at 95% confidence level, while lower limits on the squark mass as large as 1190 to 1630 GeV are obtained, depending on the production scenario. | ||
333 | _aРежим доступа: по договору с организацией-держателем ресурса | ||
461 | _tJournal of High Energy Physics | ||
463 |
_tVol. 2019, iss. 10 _v[244, 60 p.] _d2019 |
||
610 | 1 | _aэлектронный ресурс | |
610 | 1 | _aтруды учёных ТПУ | |
610 | 1 | _aHadron-Hadron scattering (experiments) | |
610 | 1 | _asupersymmetry | |
610 | 1 | _aадрон-адронное рассеяние | |
610 | 1 | _aсуперсимметрии | |
701 | 1 |
_aSirunyan _bA. M. |
|
701 | 1 |
_aTumasyan _bA. R. |
|
701 | 1 |
_aAdam _bW. _gWolfgang |
|
701 | 1 |
_aAmbrogi _bF. _gFederico |
|
701 | 1 |
_aAsilar _bE. _gEce |
|
701 | 1 |
_aBergauer _bT. _gThomas |
|
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 |
|
701 | 1 |
_aYuzhakov _bA. D. _gAleksandr Dmitrievich |
|
701 | 1 |
_aOkhotnikov _bV. V. _cphysicist _cengineer of Tomsk Polytechnic University _f1992- _gVitaly Vladimirovich _2stltpush _3(RuTPU)RU\TPU\pers\36453 |
|
712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИсследовательская школа физики высокоэнергетических процессов _c(2017- ) _h8118 _2stltpush _3(RuTPU)RU\TPU\col\23551 |
712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИнженерная школа новых производственных технологий _bНаучно-производственная лаборатория "Импульсно-пучковых, электроразрядных и плазменных технологий" _h7882 _2stltpush _3(RuTPU)RU\TPU\col\23502 |
801 | 2 |
_aRU _b63413507 _c20200907 _gRCR |
|
856 | 4 | _uhttps://doi.org/10.1007/JHEP10(2019)244 | |
942 | _cCF |