Precise determination of the Bs0–B¯s0 oscillation frequency
Mesons comprising a beauty quark and strange quark can oscillate between particle ( B s 0 ) and antiparticle ( B ¯ s 0 ) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, Δ m s . Here we present a measurement of Δ m s using B s 0 → D s − π +...
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Published in: | Nature physics Vol. 18; no. 1; pp. 1 - 5 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Journal Article |
Language: | English |
Published: |
London
Nature Publishing Group UK
2022
Nature Publishing Group |
Subjects: | |
Online Access: | Get full text |
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Summary: | Mesons comprising a beauty quark and strange quark can oscillate between particle (
B
s
0
) and antiparticle (
B
¯
s
0
) flavour eigenstates, with a frequency given by the mass difference between heavy and light mass eigenstates, Δ
m
s
. Here we present a measurement of Δ
m
s
using
B
s
0
→
D
s
−
π
+
decays produced in proton–proton collisions collected with the LHCb detector at the Large Hadron Collider. The oscillation frequency is found to be Δ
m
s
= 17.7683 ± 0.0051 ± 0.0032 ps
−1
, where the first uncertainty is statistical and the second is systematic. This measurement improves on the current Δ
m
s
precision by a factor of two. We combine this result with previous LHCb measurements to determine Δ
m
s
= 17.7656 ± 0.0057 ps
−1
, which is the legacy measurement of the original LHCb detector.
The LHCb collaboration reports an improved measurement of the oscillation frequency of mesons consisting of a bottom quark and strange quark, which is then combined with previous results. |
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ISSN: | 1745-2473 1745-2481 |
DOI: | 10.1038/s41567-021-01394-x |