Measurement of τL using the B0s→ J/ψη decay mode
Using a proton–proton collision data sample collected by the LHCb detector and corresponding to an integrated luminosity of 5.7 fb−1, the lifetime of the light B0s mass eigenstate, τL , is measured using the B0s→ J/ψη decay mode to be τL = 1.445 ± 0.016(stat) ± 0.008(syst) ps. A combination of this...
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| Main Authors: | , , , , , , , , , , , , , , , , , , , , |
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| Corporate Author: | |
| Format: | Article (Journal) |
| Language: | English |
| Published: |
17 July 2023
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| In: |
The European physical journal. C, Particles and fields
Year: 2023, Volume: 83, Issue: 7, Pages: 1-13 |
| ISSN: | 1434-6052 |
| DOI: | 10.1140/epjc/s10052-023-11634-4 |
| Online Access: | Verlag, kostenfrei, Volltext: https://doi.org/10.1140/epjc/s10052-023-11634-4 |
| Author Notes: | LHCb collaboration* |
MARC
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| 245 | 1 | 0 | |a Measurement of τL using the B0s→ J/ψη decay mode |c LHCb collaboration* |
| 246 | 3 | 3 | |a Measurement of tau L using the B 0 s → J / Psi eta decay mode |
| 264 | 1 | |c 17 July 2023 | |
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| 500 | |a *LHCb collaboration: R. Aaij, F. Archilli, S. Bachmann, D. Berninghoff, M. Borsato, R. Caspary, G. Frau, D. Gerick, J.P. Grabowski, P.A. Günther, X. Han, S. Hansmann-Menzemer, J. Hu, R. Kopecna, B. Leverington, P. Li, J. Marks, D.J. Unverzagt, U. Uwer, C. Witola, A. Zhelezov (und sehr viele weitere Personen) | ||
| 500 | |a Im Titel ist die Zahl 0 hochgestellt und der Buchstabe s tiefgestellt | ||
| 500 | |a Gesehen am 21.05.2024 | ||
| 520 | |a Using a proton–proton collision data sample collected by the LHCb detector and corresponding to an integrated luminosity of 5.7 fb−1, the lifetime of the light B0s mass eigenstate, τL , is measured using the B0s→ J/ψη decay mode to be τL = 1.445 ± 0.016(stat) ± 0.008(syst) ps. A combination of this result with a previous LHCb analysis using an independent dataset corresponding to 3 fb−1 of integrated luminosity gives τL = 1.452 ± 0.014 ± 0.007 ± 0.002 ps, where the first uncertainty is statistical, the second due to the uncorrelated part of the systematic uncertainty and the third due to the correlated part of the systematic uncertainty. | ||
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