| 000 | 03148nlm1a2200409 4500 | ||
|---|---|---|---|
| 001 | 663687 | ||
| 005 | 20231030041903.0 | ||
| 035 | _a(RuTPU)RU\TPU\network\34857 | ||
| 035 | _aRU\TPU\network\33945 | ||
| 090 | _a663687 | ||
| 100 | _a20210226a2019 k y0engy50 ba | ||
| 101 | 0 | _aeng | |
| 135 | _adrcn ---uucaa | ||
| 181 | 0 | _ai | |
| 182 | 0 | _ab | |
| 200 | 1 |
_aSearch for a heavy resonance decaying to a top quark and a vector-like top quark in the lepton + jets final state in pp collisions at s√=13TeV _fA. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.] |
|
| 203 |
_aText _celectronic |
||
| 300 | _aTitle screen | ||
| 320 | _a[References: 73 tit.] | ||
| 330 | _aA search is presented for a heavy spin-1 resonance Z′Z′ decaying to a top quark and a vector-like top quark partner TT in the lepton + jets final state. The search is performed using a data set of pp pp collisions at a centre-of-mass energy of 13TeVTeV corresponding to an integrated luminosity of 35.9fb−135.9fb−1 as recorded by the CMS experiment at the CERN LHC in the year 2016. The analysis is optimised for final states arising from the TT decay modes to a top quark and a Higgs or ZZ boson (T→Ht,ZtT→Ht,Zt). The event selection makes use of resolved and merged top quark decay products, as well as decays of boosted Higgs bosons and ZZ and WW bosons using jet substructure techniques. No significant deviation from the standard model background expectation is observed. Exclusion limits on the product of the cross section and branching fraction for Z′→tT,T→Ht,Zt,WbZ′→tT,T→Ht,Zt,Wb are presented for various combinations of the Z′Z′ resonance mass and the vector-like TT quark mass. These results represent the most stringent limits to date for the decay mode Z′→tT→tHtZ′→tT→tHt. In a benchmark model with extra dimensions, invoking a heavy spin-1 resonance G∗G∗, masses of the G∗G∗ between 1.5 and 2.3TeVTeV and between 2.0 and 2.4TeVTeV are excluded for TT masses of 1.2 and 1.5TeVTeV, respectively. | ||
| 461 | _tEuropean Physical Journal C | ||
| 463 |
_tVol. 79, iss. 3 _v[208, 32 p.] _d2019 |
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| 610 | 1 | _aэлектронный ресурс | |
| 610 | 1 | _aтруды учёных ТПУ | |
| 610 | 1 | _aкварки | |
| 610 | 1 | _aпротон-протонные соударения | |
| 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 |
|
| 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 _c20210226 _gRCR |
|
| 856 | 4 | _uhttps://doi.org/10.1140/epjc/s10052-019-6688-5 | |
| 942 | _cCF | ||