B meson
Composition

  • B+
    :
    u

    b

  • B0
    :
    d

    b

  • B0
    s    :
    s

    b

  • B+
    c    :
    c

    b
StatisticsBosonic
FamilyMesons
InteractionsStrong, Weak, Gravitational, Electromagnetic
Symbol
B+
,
B−
,
B0
,
B0
,
B0
s,
B0
s,
B+
c,
B−
c
Antiparticle

  • B+
    :
    B−

  • B0
    :
    B0

  • B0
    s    :
    B0
    s

  • B+
    c    :
    B−
    c
Mass

  • B+
    : 5279.34±0.12 MeV/c2

  • B0
    : 5279.65±0.12 MeV/c2

  • B0
    s    : 5366.88±0.14 MeV/c2

  • B+
    c    : 6274.9±0.8 MeV/c2
Mean lifetime

  • B+
    : (1.638±0.004)×10−12 s

  • B0
    : (1.519±0.004)×10−12 s

  • B0
    s    : (1.515±0.004)×10−12 s

  • B+
    c    : (0.510±0.009)×10−12 s
Electric charge

  • B±
    ,
    B±
    c    : ±1 e

  • B0
    ,
    B0
    s    : 0 e
Spin0
Strangeness
B0
s: −1
Charm
B+
c: +1
Bottomness+1
Isospin

  • B+
    : +1⁄2

  • B0
    : −1⁄2

  • B0
    s    ,
    B+
    c    : 0
Parity−1

In particle physics, B mesons are mesons composed of a bottom antiquark and either an up (
B+
), down (
B0
), strange (
B0
s) or charm quark (
B+
c). The combination of a bottom antiquark and a top quark is not thought to be possible because of the top quark's short lifetime. The combination of a bottom antiquark and a bottom quark is not a B meson, but rather bottomonium, which is something else entirely.

Each B meson has an antiparticle that is composed of a bottom quark and an up (
B−
), down (
B0
), strange (
B0
s) or charm (
B−
c) antiquark respectively.

List of B mesons

B mesons
Particle Symbol Anti-
particle 		Quark
content 		Charge Isospin
(I) 		Spin and parity,
(JP) 		Rest mass
(MeV/c2) 		S C B' Mean lifetime (s) Commonly decays to
Charged
B meson
B+
B−
u

b
 		+1 1/2 0− 5279.34±0.12 0 0 +1 (1.638±0.004)×10−12 See
B±
 decay modes
Neutral
B meson
B0
B0
d

b
 		0 1/2 0− 5279.65±0.12 0 0 +1 (1.519±0.004)×10−12 See
B0
 decay modes
Strange B meson
B0
s
B0
s
s

b
 		0 0 0− 5366.88±0.14 −1 0 +1 (1.515±0.004)×10−12 See
B0
s decay modes
Charmed B meson
B+
c
B−
c
c

b
 		+1 0 0− 6274.9±0.8 0 +1 +1 (0.510±0.009)×10−12 See
B±
c decay modes


B0
–
B0
 oscillations

Main article:
B
–
B
 oscillation

The neutral B mesons,
B0
 and
B0
s, spontaneously transform into their own antiparticles and back. This phenomenon is called flavor oscillation. The existence of neutral B meson oscillations is a fundamental prediction of the Standard Model of particle physics. It has been measured in the
B0
–
B0
 system to be about 0.496 / picoseconds,[1] and in the
B0
s–
B0
s system to be Δms = 17.77 ± 0.10 (stat) ± 0.07 (syst) / picosecond measured by CDF experiment at Fermilab.[2] A first estimation of the lower and upper limit of the
B0
s–
B0
s system value have been made by the DØ experiment also at Fermilab.[3]

On 25 September 2006, Fermilab announced that they had claimed discovery of previously-only-theorized Bs meson oscillation.[4] According to Fermilab's press release:

This first major discovery of Run 2 continues the tradition of particle physics discoveries at Fermilab, where the bottom (1977) and top (1995) quarks were discovered. Surprisingly, the bizarre behavior of the Bs (pronounced "B sub s") mesons is actually predicted by the Standard Model of fundamental particles and forces. The discovery of this oscillatory behavior is thus another reinforcement of the Standard Model's durability ...

CDF physicists have previously measured the rate of the matter-antimatter transitions for the Bs meson, which consists of the heavy bottom quark bound by the strong nuclear interaction to a strange antiquark. Now they have achieved the standard for a discovery in the field of particle physics, where the probability for a false observation must be proven to be less than about 5 in 10 million (5⁄10,000,000). For CDF's result the probability is even smaller, at 8 in 100 million (8⁄100,000,000).

Ronald Kotulak, writing for the Chicago Tribune, called the particle "bizarre" and stated that the meson "may open the door to a new era of physics" with its proven interactions with the "spooky realm of antimatter".[5]

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.[6] However, more recent results at LHCb with larger data samples have suggested no significant deviation from the Standard Model.[7]

Rare decays

B mesons are an important probe for exploring quantum chromodynamics.[8] Various uncommon decay paths of the B mesons are sensitive to physics processes outside the standard model. Measuring these rare branching fractions sets limits on new particles. The LHCb experiment has observed and searched for several of these decays such as Bs → µ+ µ−.[9]

On 21 February 2017, the LHCb collaboration announced that the rare decay of a neutral B meson into two oppositely charged kaons had been observed to a statistical significance of 5σ.[10]

See also

References

  1. ^ "[no title cited]". repository.ubn.ru.nl. 2066/26242.
  2. ^ Abulencia, A.; et al. (CDF Collaboration) (2006). "Observation of
    B0
    s    –
    B0
    s     Oscillations". Physical Review Letters. 97 (24): 242003. arXiv:hep-ex/0609040. Bibcode:2006PhRvL..97x2003A. doi:10.1103/PhysRevLett.97.242003. PMID 17280271.
  3. ^ Abazov, V. M.; et al. (D0 Collaboration) (2006). "Direct Limits on the B0
    s     Oscillation Frequency"     (PDF). Physical Review Letters. 97 (2): 021802. arXiv:hep-ex/0603029. Bibcode:2006PhRvL..97b1802A. doi:10.1103/PhysRevLett.97.021802. hdl:10211.3/194397. PMID 16907434. S2CID 11632404.
  4. ^ "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. Retrieved 8 December 2007.
  5. ^ Kotulak, R. (26 September 2006). "Antimatter discovery could alter physics: Particle tracked between real world, spooky realm". Deseret News. Archived from the original on 29 November 2007. Retrieved 8 December 2007.
  6. ^ Overbye, D. (17 May 2010). "From Fermilab, a New Clue to Explain Human Existence?". The New York Times. Retrieved 26 December 2016.
  7. ^ Timmer, J. (29 August 2011). "LHCb detector causes trouble for supersymmetry theory". Ars Technica. Retrieved 26 December 2012.
  8. ^ CMS Collaboration; LHCb Collaboration (4 June 2015). "Observation of the rare B0
    s     → µ+ µ−     decay from the combined analysis of CMS and LHCb data". Nature. 522 (7554): 68–72. arXiv:1411.4413. Bibcode:2015Natur.522...68C. doi:10.1038/nature14474. PMID 26047778. S2CID 4394036.
  9. ^ Aaij, R.; Beteta, C. Abellán; Adeva, B.; Adinolfi, M.; Affolder, A.; Ajaltouni, Z.; Akar, S.; Albrecht, J. (16 October 2015). "Search for the rare decays B0 → J/ψ γ and B0
    s     → J/ψ γ     ". Physical Review D. 92 (11): 112002. arXiv:1510.04866. Bibcode:2015PhRvD..92k2002A. doi:10.1103/PhysRevD.92.112002. S2CID 118320485.
  10. ^ Aaij, R.; et al. (21 February 2017). "Observation of the annihilation decay mode B0 → K+ K− ". Physical Review Letters. 118 (8): 47–50. arXiv:1610.08288. Bibcode:2017PhRvL.118h1801A. doi:10.1103/PhysRevLett.118.081801. PMID 2828221. S2CID 27186492.

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