Amplitude analysis of the Bs0 → K∗0K[bar]∗0 decays and measurement of the branching fraction of the B0 → K∗0K[bar]∗0 decay
The B0→K∗0K¯∗0$$ {B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ and Bs0→K∗0K¯∗0$$ {B}_s^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ decays are studied using proton-proton collision data corresponding to an integrated luminosity of 3 fb−1. An untagged and timeintegrated amplitude analysis of B(s)0 →...
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
July 5, 2019
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| In: |
Journal of high energy physics
Year: 2019, Heft: 7 |
| ISSN: | 1029-8479 |
| DOI: | 10.1007/JHEP07(2019)032 |
| Online-Zugang: | Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1007/JHEP07(2019)032
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| Verfasserangaben: | the LHCb collaboration |
MARC
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| 245 | 1 | 0 | |a Amplitude analysis of the Bs0 → K∗0K[bar]∗0 decays and measurement of the branching fraction of the B0 → K∗0K[bar]∗0 decay |c the LHCb collaboration |
| 246 | 3 | 3 | |a Amplitude analysis of the B s 0 → K ∗ 0 K bar ∗ 0 decays and measurement of the branching fraction of the B 0 → K ∗ 0 K bar ∗ 0 decay |
| 264 | 1 | |c July 5, 2019 | |
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| 500 | |a Im Titel ist die "0" bei den Buchstaben B und K hochgestellt, "s" tiefgestellt und in Klammern | ||
| 500 | |a Im Titel ist beim ersten und dritten K "∗" hochgestellt | ||
| 500 | |a Im Titel ist das zweite und vierte "K" mit einem Oberstrich dargestellt, "∗" und "0" stehen rechts neben dem Oberstrich | ||
| 500 | |a The LHCb Collaboration: R. Aaij, S. Bachmann, D. Berninghoff, M. Borsato, S. Braun, A. Comerma-Montells, P. d’Argent, M. Dziewiecki, D. Gerick, J.P. Grabowski, X. Han, S. Hansmann-Menzemer, M. Heß, J. Hu, M. Kecke, M. Kolpin, R. Kopecna, B. Leverington, H. Malygina, J. Marks, D.S. Mitzel, S. Neubert, A. Piucci, M. Schmelling, N. Skidmore, M. Stahl, S. Stemmle, U. Uwer, R. Waldi, A. Zhelezov [und viele weitere] | ||
| 500 | |a Gesehen am 12.05.2020 | ||
| 520 | |a The B0→K∗0K¯∗0$$ {B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ and Bs0→K∗0K¯∗0$$ {B}_s^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ decays are studied using proton-proton collision data corresponding to an integrated luminosity of 3 fb−1. An untagged and timeintegrated amplitude analysis of B(s)0 → (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¯∗0$$ {B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ 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 Bs0→K∗0K¯∗0$$ {B}_s^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0} $$ decay. The ratio of branching fractions of the two decays is measured and used to determine ℬB0→K∗0K¯∗0=8.0±0.9stat±0.4syst×10−7$$ \mathrm{\mathcal{B}}\left({B}^0\to {K}^{\ast 0}{\overline{K}}^{\ast 0}\right)=\left(8.0\pm 0.9\left(\mathrm{stat}\right)\pm 0.4\left(\mathrm{syst}\right)\right)\times {10}^{-7} $$. | ||
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