In particle physics, a rho meson is a short-lived hadronic particle that is an isospin triplet whose three states are denoted as ρ+, ρ0 and ρ−. After the pions and kaons, the rho mesons are the lightest strongly interacting particle with a mass of roughly MeV for all three states. There should be a small mass difference between the 770 ρ+ and the ρ0 that can be attributed to the electromagnetic self-energy of the particle as well as a small effect due to isospin breaking arising from the light quark masses; however, the current experimental limit is that this mass difference is less than . 0.7 MeV
The rho mesons have a very short lifetime and their decay width is about with the peculiar feature that the decay widths are not described by a 145 MeVBreit–Wigner form. The principal decay route of the rho mesons is to a pair of pions with a branching rate of 99.9%. Neutral rho mesons can decay to a pair of electrons or muons which occurs with a branching ratio of ×10−5. This decay of the neutral rho to leptons can be interpreted as a mixing between the 5photon and rho. In principle the charged rho mesons mix with the weak vector bosons and can lead to decay to an electron or muon plus a neutrino; however, this has never been observed.
In the De Rujula–Georgi–Glashow description of hadrons, the rho mesons can be interpreted 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.
|Rest mass (MeV/c2)||IG||JPC||S||C||B'||Mean lifetime (s)||Commonly decays to
(>5% of decays)
|Charged rho meson||ρ+(770)||ρ−(770)||ud||±0.4775.4||1+||1−||0||0||0||×10−24~4.5[a][b]||π± + π0|
|Neutral rho meson||ρ0(770)||Self||±0.34775.49||1+||1−−||0||0||0||×10−24~4.5[a][b]||π+ + π−|