Search for resonant tt¯tt¯ production in proton-proton collisions at √s=13 TeV; Journal of High Energy Physics; Vol. 2019, iss. 4

Bibliographische Detailangaben
Parent link:Journal of High Energy Physics
Vol. 2019, iss. 4.— 2019.— [31, 54 p.]
Körperschaften: Национальный исследовательский Томский политехнический университет Исследовательская школа физики высокоэнергетических процессов, Национальный исследовательский Томский политехнический университет Инженерная школа новых производственных технологий Научно-производственная лаборатория "Импульсно-пучковых, электроразрядных и плазменных технологий"
Weitere Verfasser: Sirunyan A. M., Tumasyan A. R., Adam W. Wolfgang, Ambrogi F. Federico, Asilar E. Ece, Bergauer T. Thomas, Babaev A. A. Anton Anatoljevich, Okhotnikov V. V. Vitaly Vladimirovich
Zusammenfassung:Title screen
A search for a heavy resonance decaying into a top quark and antiquark (tt¯)(tt¯) pair is performed using proton-proton collisions at s√=13s=13 TeV. The search uses the data set collected with the CMS detector in 2016, which corresponds to an integrated luminosity of 35.9 fb−1. The analysis considers three exclusive final states and uses reconstruction techniques that are optimized for top quarks with high Lorentz boosts, which requires the use of nonisolated leptons and jet substructure techniques. No significant excess of events relative to the expected yield from standard model processes is observed. Upper limits on the production cross section of heavy resonances decaying to a tt¯tt¯ pair are calculated. Limits are derived for a leptophobic topcolor Z′ resonance with widths of 1, 10, and 30%, relative to the mass of the resonance, and exclude masses up to 3.80, 5.25, and 6.65 TeV, respectively. Kaluza-Klein excitations of the gluon in the Randall-Sundrum model are excluded up to 4.55 TeV. To date, these are the most stringent limits on tt¯tt¯ resonances.
Режим доступа: по договору с организацией-держателем ресурса
Sprache:Englisch
Veröffentlicht: 2019
Schlagworte:
Online-Zugang:https://doi.org/10.1007/JHEP04(2019)031
Format: xMaterials Elektronisch Buchkapitel
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=662610

MARC

LEADER 00000naa0a2200000 4500
001 662610
005 20250409124613.0
035 |a (RuTPU)RU\TPU\network\33765 
090 |a 662610 
100 |a 20200910d2019 k||y0rusy50 ba 
101 0 |a eng 
135 |a drcn ---uucaa 
181 0 |a i  
182 0 |a b 
200 1 |a Search for resonant tt¯tt¯ production in proton-proton collisions at √s=13 TeV  |f A. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.] 
203 |a Text  |c electronic 
300 |a Title screen 
320 |a [References: 88 tit.] 
330 |a A search for a heavy resonance decaying into a top quark and antiquark (tt¯)(tt¯) pair is performed using proton-proton collisions at s√=13s=13 TeV. The search uses the data set collected with the CMS detector in 2016, which corresponds to an integrated luminosity of 35.9 fb−1. The analysis considers three exclusive final states and uses reconstruction techniques that are optimized for top quarks with high Lorentz boosts, which requires the use of nonisolated leptons and jet substructure techniques. No significant excess of events relative to the expected yield from standard model processes is observed. Upper limits on the production cross section of heavy resonances decaying to a tt¯tt¯ pair are calculated. Limits are derived for a leptophobic topcolor Z′ resonance with widths of 1, 10, and 30%, relative to the mass of the resonance, and exclude masses up to 3.80, 5.25, and 6.65 TeV, respectively. Kaluza-Klein excitations of the gluon in the Randall-Sundrum model are excluded up to 4.55 TeV. To date, these are the most stringent limits on tt¯tt¯ resonances. 
333 |a Режим доступа: по договору с организацией-держателем ресурса 
461 |t Journal of High Energy Physics 
463 |t Vol. 2019, iss. 4  |v [31, 54 p.]  |d 2019 
610 1 |a электронный ресурс 
610 1 |a труды учёных ТПУ 
610 1 |a Hadron-Hadron scattering (experiments) 
610 1 |a Beyond Standard Model 
610 1 |a адрон-адронное рассеяние 
701 1 |a Sirunyan  |b A. M. 
701 1 |a Tumasyan  |b A. R. 
701 1 |a Adam  |b W.  |g Wolfgang 
701 1 |a Ambrogi  |b F.  |g Federico 
701 1 |a Asilar  |b E.  |g Ece 
701 1 |a Bergauer  |b T.  |g Thomas 
701 1 |a Babaev  |b A. A.  |c physicist  |c engineer-issledovatelskogo Polytechnic University, candidate of physical and mathematical Sciences  |f 1981-  |g Anton Anatoljevich  |3 (RuTPU)RU\TPU\pers\35154  |9 18420 
701 1 |a Okhotnikov  |b V. V.  |c physicist  |c engineer of Tomsk Polytechnic University  |f 1992-  |g Vitaly Vladimirovich  |3 (RuTPU)RU\TPU\pers\36453  |9 19502 
712 0 2 |a Национальный исследовательский Томский политехнический университет  |b Исследовательская школа физики высокоэнергетических процессов  |c (2017- )  |3 (RuTPU)RU\TPU\col\23551  |9 28348 
712 0 2 |a Национальный исследовательский Томский политехнический университет  |b Инженерная школа новых производственных технологий  |b Научно-производственная лаборатория "Импульсно-пучковых, электроразрядных и плазменных технологий"  |3 (RuTPU)RU\TPU\col\23502  |9 28318 
801 2 |a RU  |b 63413507  |c 20201012  |g RCR 
856 4 |u https://doi.org/10.1007/JHEP04(2019)031 
942 |c CF