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Rho meson

From Wikipedia, the free encyclopedia
Short-lived hadronic particle that is an isospin triplet
Rho meson
StatisticsBosonic
FamilyMesons
InteractionsStrong,Weak,Gravitational andElectromagnetic
Symbolρ+
,ρ0
, andρ
Antiparticle
  • ρ+
    :ρ
  • ρ0
    : self
Types3
Mass~770 MeV/c2[1][a]
Mean lifetime~4.5×10−24 s[b][a]
Decays into
  • ρ±
    :π±
    +π0
  • ρ0
    :π+
    +π
Electric charge
  • ρ±
    :±1e
  • ρ0
    : 0 e
Color charge0
Spin1
Isospin
  • ρ±
    :±1
  • ρ0
    : 0
Hypercharge0
Parity−1
C parity−1

Inparticle physics, arho meson is a short-livedhadronic particle that is anisospintriplet whose three states are denoted asρ+
,ρ0
andρ
. Along withpions andomega mesons, the rho meson carries thenuclear force within theatomic nucleus. After the octet consisting of the pions,kaons, andeta meson, the rhomesons are the lightest strongly interacting particle, with a mass of about775 MeV for all three states.[c]

The rho mesons have a very short lifetime and theirdecay width is about145 MeV; because that is large compared with the mass, the resonance width measurably deviates from aBreit–Wigner form. The principal decay route of the rho mesons is to a pair of pions with abranching rate of 99.9% (however, all neutral pions is forbidden).[d]

History

[edit]

After several false starts, the ρ meson and the ω meson were discovered atLawrence Berkeley Laboratory in 1961.[2]

Composition

[edit]

The rho mesons can be interpreted[3] as a bound state of aquark and an anti-quark and is an excited version of the pion. Unlike the pion, the rho meson has spinj = 1 (avector meson) and a much higher value of the mass. They[who?] attribute this mass difference between the pions and rho mesons to a largehyperfine interaction between the quark and anti-quark, although an objection with the De Rujula–Georgi–Glashow description is that it attributes the lightness of the pions as an accident rather than a result ofchiral symmetry breaking.

The rho mesons can be thought of as thegauge bosons of aspontaneously brokengauge symmetry whose local character isemergent (arising fromQCD); Note that this broken gauge symmetry (sometimes called hidden local symmetry) is distinct from theglobalchiral symmetry acting on theflavors. This was described byHoward Georgi in a paper titled "The Vector Limit of Chiral Symmetry" where he ascribed much of the literature of hidden local symmetry to anon-linear sigma model.[4]

Rho mesons
Particle nameParticle
symbol
Antiparticle
symbol
Quark
content[5]
Mass (MeV/c2)[a]IGJPCSCB'Mean lifetime (s)[a]Commonly decays to
(>5% of decays)
Charged rho meson[6]ρ+
(770)
ρ
(770)
ud775.11±0.341+1000(4.415±0.024)×10−24[b]π±
+π0
Neutral rho meson[6]ρ0
(770)
Selfuu¯dd¯2{\displaystyle \mathrm {\tfrac {u{\bar {u}}-d{\bar {d}}}{\sqrt {2}}} \,}775.26±0.251+1−−000(4.453±0.027)×10−24[b]π+
+π

Notes

[edit]
  1. ^abcdThe exact value depends on the method used. See the given reference for detail. In the table, data used is fromtau decays andelectron–positron annihilation.
  2. ^abcPDG reports the resonance width (Γ). Here the conversion τ = ħΓ is given instead.
  3. ^There must be a small mass difference between the chargedρ+
    and the neutralρ0
    that can be attributed to electromagnetic self-energy of the particle as well as the quark masses; however, the current experimental data are unable to show a significant difference.
  4. ^Neutral rho mesons can decay to a pair ofelectrons ormuons which occurs with a branching ratio of5×10−5. This decay of the neutral rho to leptons can be interpreted as a mixing between thephoton and rho. In principle the charged rho mesons mix with theweak vector bosons and can lead to decay to an electron or muon plus aneutrino; however, this has never been observed.

References

[edit]
  1. ^Zyla, P. A.; et al. (Particle Data Group) (2020)."Review of Particle Physics".Progress of Theoretical and Experimental Physics.2020 (8): 083C01.doi:10.1093/ptep/ptaa104.hdl:11585/772320.
  2. ^Maglich, B. (1976). "Discovery of omega meson-first neutral vector meson: one researcher's personal account - Discovery story".Adv. Exp. Phys.5: 79.
  3. ^De Rújula, A.; Georgi, Howard; Glashow, S. L. (1975-07-01). "Hadron masses in a gauge theory".Physical Review D.12 (1). American Physical Society (APS):147–162.Bibcode:1975PhRvD..12..147D.doi:10.1103/physrevd.12.147.ISSN 0556-2821.
  4. ^Georgi, Howard (1990). "Vector realization of chiral symmetry".Nuclear Physics B.331 (2). Elsevier BV:311–330.Bibcode:1990NuPhB.331..311G.doi:10.1016/0550-3213(90)90210-5.ISSN 0550-3213.
  5. ^C. Amsleret al. (2008):Quark Model
  6. ^abPDG 2025 atParticle listings –ρ
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