B–Bbar oscillation
Neutral B meson oscillations (or
B
–
B
oscillations) are one of the manifestations of the neutral particle oscillation, a fundamental prediction of the Standard Model of particle physics. It is the phenomenon of B mesons changing (or oscillating) between their matter and antimatter forms before their decay. The
B
s meson can exist as either a bound state of a strange antiquark and a bottom quark, or a strange quark and bottom antiquark. The oscillations in the neutral B sector are analogous to the phenomena that produce long and short-lived neutral kaons.
B
s–
B
s mixing was observed by the CDF experiment at Fermilab in 2006 and by LHCb at CERN in 2011 and 2021.
Excess of matter over antimatter
[edit]The Standard Model predicts that regular matter
B
s mesons are slightly favored in these oscillations over their antimatter counterpart, making strange B mesons of special interest to particle physicists. The observation of the
B
–
B
mixing phenomena led physicists to propose the construction of the so-named "B factories" in the early 1990s. They realized that a precise
B
–
B
oscillation measure could pin down the unitarity triangle and perhaps explain the excess of matter over antimatter in the universe. To this end construction began on two "B factories" in the late nineties, one at the Stanford Linear Accelerator Center (SLAC) in California and one at KEK in Japan.
B
s–
B
s mesons, they act as short lived virtual particles
These B factories, BaBar and Belle, were set at the
ϒ
(4S) resonance which is just above the threshold for decay into two B mesons.
On 14 May 2010, physicists at the Fermi National Accelerator Laboratory reported that the oscillations decayed into matter 1% more often than into antimatter, which may help explain the abundance of matter over antimatter in the observed Universe.[1] However, more recent results at LHCb in 2011, 2012, and 2021 with larger data samples have demonstrated no significant deviation from the Standard Model prediction of very nearly zero asymmetry.[2][3][4]
See also
[edit]References
[edit]- ^ "A new clue to explain existence". The New York Times. 2010-05-18.
- ^ "LHCb detector causes trouble for supersymmetry theory". Ars Technica. 29 August 2011.
- ^ Aaij, R.; et al. (LHCb collaboration) (2014). "Measurement of the flavour-specific CP-violating asymmetry as
sl in B0
s decays". Physics Letters B. 728: 607–615. arXiv:1308.1048. Bibcode:2014PhLB..728..607A. doi:10.1016/j.physletb.2013.12.030. S2CID 73647030. - ^ Aaij, R.; Beteta, C. Abellán; Ackernley, T.; Adeva, B.; Adinolfi, M.; Afsharnia, H.; et al. (6 January 2022). "Precise determination of the B0
s–B0
s oscillation frequency". Nature Physics. 18: 1–5. arXiv:2104.04421. doi:10.1038/s41567-021-01394-x. ISSN 1745-2481. S2CID 245809087.
Further reading
[edit]- Albrecht, H.; et al. (ARGUS collaboration) (1987). "Observation of B0
–B0
mixing". Physics Letters B. 192 (1–2): 245–252. doi:10.1016/0370-2693(87)91177-4. — paper describing the discovery of B-meson mixing by the ARGUS collaboration - "Fermilab's CDF scientists present a precision measurement of a subtle dance between matter and antimatter" (Press release). Fermilab. 11 April 2006.
- "Fermilab's CDF scientists make it official: They have discovered the quick-change behavior of the B-sub-s meson, which switches between matter and antimatter 3 trillion times a second" (Press release). Fermilab. 25 September 2006. — announcement of the 5 sigma discovery
External links
[edit] | This particle physics–related article is a stub. You can help Wikipedia by expanding it. |