Studies of B∗s2(5840)0Bs2∗(5840)0 and Bs1(5830)0Bs1(5830)0 mesons including the observation of the B∗s2(5840)0→B0K0SBs2∗(5840)0→B0KS0 decay in proton-proton collisions at s√=8TeV

Bibliographic Details
Parent link:The European Physical Journal C: Scientific Journal
Vol. 78, iss. 11.— 2018.— [939, 26 р.,]
Corporate Authors: 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"
Other Authors: Sirunyan А. М., Tumasyan A. R., Adam W. Wolfgang, Ambrogi F. Federico, Babaev A. A. Anton Anatoljevich, Okhotnikov V. V. Vitaly Vladimirovich, Baydali S. A. Sergey Anatolievich
Summary:Title screen
Measurements of B∗s2(5840)0Bs2∗(5840)0 and Bs1(5830)0Bs1(5830)0 mesons are performed using a data sample of proton-proton collisions corresponding to an integrated luminosity of Open image in new window, collected with the CMS detector at the LHC at a centre-of-mass energy of 8TeV8TeV. The analysis studies P-wave B0sBs0 meson decays into B(∗)+K−B(∗)+K− and B(∗)0K0SB(∗)0KS0, where the B+B+ and B0B0 mesons are identified using the decays B+→J/ψK+B+→J/ψK+ and B0→J/ψK∗(892)0B0→J/ψK∗(892)0. The masses of the P-wave B0sBs0 meson states are measured and the natural width of the B∗s2(5840)0Bs2∗(5840)0 state is determined. The first measurement of the mass difference between the charged and neutral B∗B∗ mesons is also presented. The B∗s2(5840)0Bs2∗(5840)0 decay to B0K0SB0KS0 is observed, together with a measurement of its branching fraction relative to the B∗s2(5840)0→B+K−Bs2∗(5840)0→B+K− decay
Published: 2018
Subjects:
Online Access:https://doi.org/10.1140/epjc/s10052-018-6390-z
Format: Electronic Book Chapter
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=659051