Rho meson: Difference between revisions
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Latest revision as of 22:16, 12 December 2024
Template:Short description Template:Infobox particle In particle physics, a rho meson is a short-lived hadronic particle that is an isospin triplet whose three states are denoted as Template:SubatomicParticle, Template:SubatomicParticle and Template:SubatomicParticle. Along with pions and omega mesons, the rho meson carries the nuclear force within the atomic nucleus. After the pions and kaons, the rho mesons are the lightest strongly interacting particle, with a mass of Template:Val for all three states.[lower-alpha 1]
The rho mesons have a very short lifetime and their decay width is about Template:Val with the peculiar feature that the decay widths are not described by a Breit–Wigner form. The principal decay route of the rho mesons is to a pair of pions with a branching rate of 99.9%.[lower-alpha 2]
History
After several false starts, the ρ meson and the ω meson were discovered at Lawrence Berkeley Laboratory in 1961.[1]
Composition
The rho mesons can be interpreted[2] as a bound state of a quark and an anti-quark and is an excited version of the pion. Unlike the pion, the rho meson has spin j = 1 (a vector meson) and a much higher value of the mass. This mass difference between the pions and rho mesons is attributed to a large hyperfine interaction between the quark and anti-quark. The main objection with the De Rujula–Georgi–Glashow description is that it attributes the lightness of the pions as an accident rather than a result of chiral symmetry breaking.
The rho mesons can be thought of as the gauge bosons of a spontaneously broken gauge symmetry whose local character is emergent (arising from QCD); Note that this broken gauge symmetry (sometimes called hidden local symmetry) is distinct from the global chiral symmetry acting on the flavors. This was described by Howard Georgi in a paper titled "The Vector Limit of Chiral Symmetry" where he ascribed much of the literature of hidden local symmetry to a non-linear sigma model.[3]
| Particle name | Particle symbol |
Antiparticle symbol |
Quark content[4] |
Mass (MeV/c2)[lower-alpha 3] | IG | JPC | S | C | B' | Mean lifetime (s)[lower-alpha 3] | Commonly decays to (>5% of decays) |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Charged rho meson[5] | Template:SubatomicParticle(770) | Template:SubatomicParticle(770) | Template:SubatomicParticleTemplate:SubatomicParticle | Template:Val | 1+ | 1− | 0 | 0 | 0 | Template:Val[lower-alpha 4] | Template:Nowrap |
| Neutral rho meson[5] | Template:SubatomicParticle(770) | Self | Template:Val | 1+ | 1−− | 0 | 0 | 0 | Template:Val[lower-alpha 4] | Template:Nowrap |
Notes
References
Template:Particles Template:Authority control
Cite error: <ref> tags exist for a group named "lower-alpha", but no corresponding <references group="lower-alpha"/> tag was found
- ↑ Template:Cite journal
- ↑ Template:Cite journal
- ↑ Template:Cite journal
- ↑ C. Amsler et al. (2008): Quark Model
- ↑ 5.0 5.1 C. Amsler et al. (2008): Particle listings – Template:SubatomicParticle