par Khachatryan, Vardan;Barria, Patrizia
;Caillol, Cécile
;Clerbaux, Barbara
;De Lentdecker, Gilles
;Delannoy, Hugo
;Fasanella, Giuseppe
;Favart, Laurent
;Gay, Arnaud
;Grebenyuk, Anastasia
;Karapostoli, Georgia
;Lenzi, Thomas
;Maerschalk, Thierry
;Marinov, Audrey
;Pernie, Luca
;Randle-Conde, Aidan Sean
;Reis, Thomas
;Seva, Tomislav
;Vander Velde, Catherine
;Vanlaer, Pascal
;Yonamine, Ryo
;Zenoni, Florian
;Zhang, Fengwangdong
; [et al.]
Référence The Journal of high energy physics, 2016, 1, 166
Publication Publié, 2016
;Caillol, Cécile
;Clerbaux, Barbara
;De Lentdecker, Gilles
;Delannoy, Hugo
;Fasanella, Giuseppe
;Favart, Laurent
;Gay, Arnaud
;Grebenyuk, Anastasia
;Karapostoli, Georgia
;Lenzi, Thomas
;Maerschalk, Thierry
;Marinov, Audrey
;Pernie, Luca
;Randle-Conde, Aidan Sean
;Reis, Thomas
;Seva, Tomislav
;Vander Velde, Catherine
;Vanlaer, Pascal
;Yonamine, Ryo
;Zenoni, Florian
;Zhang, Fengwangdong
; [et al.]Référence The Journal of high energy physics, 2016, 1, 166
Publication Publié, 2016
Article révisé par les pairs
| Résumé : | A search is presented for a singly produced excited bottom quark (b*) decaying to a top quark and a W boson in the all-hadronic, lepton+jets, and dilepton final states in proton-proton collisions at s=8(Formula Presented.)TeV recorded by the CMS experiment at the CERN LHC. Data corresponding to an integrated luminosity of 19.7 fb−1 are used. No significant excess of events is observed with respect to standard model expectations. We set limits at 95% confidence on the product of the b* quark production cross section and its branching fraction to tW. The cross section limits are interpreted for scenarios including left-handed, right-handed, and vector-like couplings of the b* quark and are presented in the two-dimensional coupling plane based on the production and decay coupling constants. The masses of the left-handed, right-handed, and vector-like b* quark states are excluded at 95% confidence below 1390, 1430, and 1530 GeV, respectively, for benchmark couplings. This analysis gives the most stringent limits on the mass of the b∗ quark to date. |



