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005 20231030041853.0
035 _a(RuTPU)RU\TPU\network\34573
090 _a663404
100 _a20210210a2019 k y0engy50 ba
101 0 _aeng
102 _aUS
135 _adrcn ---uucaa
181 0 _ai
182 0 _ab
200 1 _aAmplitude analysis of the B0(s)→K∗0K¯∗0B(s)0→K∗0K¯∗0 decays and measurement of the branching fraction of the B0→K∗0K¯∗0B0→K∗0K¯∗0 decay
_fR. Aaij, C. A. Beteta, B. Adeva [et al.]
203 _aText
_celectronic
300 _aTitle screen
320 _a[References: 44 tit.]
330 _aThe B0→K∗0K¯∗0B0→K∗0K¯∗0 and B0s→K∗0K¯∗0Bs0→K∗0K¯∗0 decays are studied using proton-proton collision data corresponding to an integrated luminosity of 3 fb−1. An untagged and timeintegrated amplitude analysis of B0(s) → (K+π−)(K−π+) decays in two-body invariant mass regions of 150 MeV/c2 around the K∗0 mass is performed. A stronger longitudinal polarisation fraction in the B0→K∗0K¯∗0B0→K∗0K¯∗0 decay, fL = 0.724 ± 0.051 (stat) ± 0.016 (syst), is observed as compared to fL = 0.240 ± 0.031 (stat) ± 0.025 (syst) in the B0s→K∗0K¯∗0Bs0→K∗0K¯∗0 decay. The ratio of branching fractions of the two decays is measured and used to determine B(B0→K∗0K¯∗0)=(8.0±0.9(stat)±0.4(syst))×10−7B(B0→K∗0K¯∗0)=(8.0±0.9(stat)±0.4(syst))×10−7.
461 _tJournal of High Energy Physics
463 _tVol. 2019, iss. 7
_v[32, 30 p.]
_d2019
610 1 _aэлектронный ресурс
610 1 _aтруды учёных ТПУ
610 1 _aB physics
610 1 _aHadron-Hadron scattering (experiments)
701 1 _aAaij
_bR.
_gRoel
701 1 _aBeteta
_bC. A.
_gCarlos Abellan
701 1 _aAdeva
_bB.
_gBernardo
701 1 _aEydelman
_bS. I.
_gSemen Isaakovich
701 1 _aKharisova
_bA. E.
_cnuclear technology specialist
_cengineer of Tomsk Polytechnic University
_f1994-
_gAnastasiya Evgenjevna
_2stltpush
_3(RuTPU)RU\TPU\pers\46775
701 1 _aPanshin
_bG. L.
_cspecialist in the field of informatics and computer technology
_cAssistant of the Department of Tomsk Polytechnic University
_f1987-
_gGennady Leonidovich
_2stltpush
_3(RuTPU)RU\TPU\pers\40978
701 1 _aStrokov
_bS. A.
_cphysicist
_cengineer of Tomsk Polytechnic University
_f1977-
_gSergey Aleksandrovich
_2stltpush
_3(RuTPU)RU\TPU\pers\37442
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 информационных технологий и робототехники
_bОтделение автоматизации и робототехники (ОАР)
_h7952
_2stltpush
_3(RuTPU)RU\TPU\col\23553
801 2 _aRU
_b63413507
_c20210226
_gRCR
856 4 _uhttps://doi.org/10.1007/JHEP07(2019)032
942 _cCF