List of mesons
From Wikipedia, the free encyclopedia
This is a list of mesons; it is not comprehensive.
| Particle | Symbol | Anti- particle | Quark Makeup | Spin and parity | Rest mass MeV/c2 | S | C | B | Mean lifetime s | Principal decays | Notes |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Charged Pion | <math>\mathrm{\pi^+}</math> | <math>\mathrm{\pi^-}</math> | <math>\mathrm{u \bar{d}}</math> | Pseudoscalar | 139.6 | 0 | 0 | 0 | 2.60×10-8 | μ+ + νμ | |
| Neutral Pion | <math>\mathrm{\pi^0}</math> | Self | <math>\mathrm{\frac{u\bar{u} - d \bar{d}}{\sqrt{2}}}</math> | Pseudoscalar | 135.0 | 0 | 0 | 0 | 0.84×10-16 | 2γ | Makeup inexact due to non-zero quark masses |
| Charged Kaon | <math>\mathrm{K^+}</math> | <math>\mathrm{K^-}</math> | <math>\mathrm{u\bar{s}}</math> | Pseudoscalar | 493.7 | +1 | 0 | 0 | 1.24×10-8 | μ + νμ or π+ + π0 | |
| Neutral Kaon | <math>\mathrm{K^0}</math> | <math>\mathrm{\bar{K}^0}</math> | <math>\mathrm{d\bar{s}} </math> | Pseudoscalar | 497.7 | +1 | 0 | 0 | weak decay | Strong eigenstate - no definite lifetime (see kaon notes below) | |
| K-Short | <math>\mathrm{K_S^0}</math> | <math>\mathrm{K_S^0}</math> | <math>\mathrm{\frac{d\bar{s} - s\bar{d}}{\sqrt{2}}} </math> | Pseudoscalar | 497.7 | (*) | 0 | 0 | 0.89×10-10 | π+ + π- or 2π0 | Weak eigenstate - makeup is missing small CP-violating term (see kaon notes below) |
| K-Long | <math>\mathrm{K_L^0}</math> | <math>\mathrm{K_L^0}</math> | <math>\mathrm{\frac{d\bar{s} + s\bar{d}}{\sqrt{2}}}</math> | Pseudoscalar | 497.7 | (*) | 0 | 0 | 5.2×10-8 | π+ + e- + νe | Weak eigenstate - makeup is missing small CP-violating term (see kaon notes below) |
| Eta | <math>\mathrm{\eta}</math> | Self | <math>\mathrm{\frac{u\bar{u} + d\bar{d} - 2s\bar{s}}{\sqrt{6}}}</math> | Pseudoscalar | 547.8 | 0 | 0 | 0 | 5×10-19 | Makeup inexact due to non-zero quark masses | |
| Eta Prime | <math>\mathrm{\eta'}</math> | Self | <math>\mathrm{\frac{u\bar{u} + d\bar{d} + s\bar{s}}{\sqrt{3}}}</math> | Pseudoscalar | 957.6 | 0 | 0 | 0 | 3×10-21 | Makeup inexact due to non-zero quark masses | |
| Rho | <math>\mathrm{\rho^+}</math> | <math>\mathrm{\rho^-}</math> | <math>\mathrm{u\bar{d}}</math> | Vector | 776 | 0 | 0 | 0 | 0.4×10-23 | ||
| Phi | <math>\mathrm{\phi}</math> | Self | <math>\mathrm{s\bar{s}}</math> | Vector | 1019 | 0 | 0 | 0 | 16×10-23 | ||
| D | <math>\mathrm{D^+}</math> | <math>\mathrm{D^-}</math> | <math>\mathrm{c\bar{d}}</math> | Pseudoscalar | 1869 | 0 | +1 | 0 | 10.6×10-13 | ||
| D | <math>\mathrm{D^0}</math> | <math>\mathrm{\bar{D^0}}</math> | <math>\mathrm{c\bar{u}}</math> | Pseudoscalar | 1865 | 0 | +1 | 0 | 4.1×10-13 | ||
| Ds | <math>\mathrm{D_s^+}</math> | <math>\mathrm{D_s^-}</math> | <math>\mathrm{c\bar{s}}</math> | Pseudoscalar | 1968 | +1 | +1 | 0 | 4.9×10-13 | ||
| J/Psi | <math>\mathrm{J/\psi}</math> | Self | <math>\mathrm{c\bar{c}}</math> | Vector | 3096.9 | 0 | 0 | 0 | 7.2×10-21 | e+ + e- or μ+ + μ- ... | See charmonium |
| B | <math>\mathrm{B^+}</math> | <math>\mathrm{B^-}</math> | <math>\mathrm{u\bar{b}}</math> | Pseudoscalar | 5279 | 0 | 0 | +1 | 1.7×10-12 | ||
| B | <math>\mathrm{B^0}</math> | <math>\mathrm{\bar{B^0}}</math> | <math>\mathrm{d\bar{b}}</math> | Pseudoscalar | 5279 | 0 | 0 | +1 | 1.5×10-12 | ||
| Bs | <math>\mathrm{B_s^0}</math> | <math>\mathrm{\bar{B}_s^0}</math> | <math>\mathrm{s\bar{b}}</math> | Pseudoscalar | 5369 | -1 | 0 | +1 | 1.46×10-12 | ||
| Bc | <math>\mathrm{B_c^+}</math> | <math>\mathrm{B_c^-}</math> | <math>\mathrm{c\bar{b}}</math> | Pseudoscalar | 6400 | 0 | +1 | +1 | 5×10-13 | ||
| Upsilon | <math>\Upsilon\,</math> | Self | <math>\mathrm{b\bar{b}}</math> | Vector | 9460 | 0 | 0 | 0 | 1.3×10-20 | e+ + e- or μ+ + μ- ... | See bottomonium |
Image:Noneto mesônico de spin 0.png Image:Noneto mesônico de spin 1.png
[edit] Notes on neutral kaons
There are two complications with neutral kaons:
- Due to neutral kaon mixing, the <math>\mathrm{K_S^0}</math> and <math>\mathrm{K_L^0}</math> are not eigenstates of strangeness. However, they are eigenstates of the weak force, which determines how they decay, so these are the particles with definite lifetime.
- Furthermore, the linear combinations given in the table for the <math>\mathrm{K_S^0}</math> and <math>\mathrm{K_L^0}</math> are not exactly correct, since there is a small correction due to CP violation. See CP violation in kaons.
Note that these issues also exist in principle for other neutral flavored mesons; however, the weak eigenstates are considered separate particles only for kaons because of their dramatically different lifetimes.
[edit] See also
[edit] External link
[edit] Reference
- Griffiths, David J. (1998). Introduction to Electrodynamics (3rd ed.). Prentice Hall. ISBN 0-13-805326-X.
| Hadrons: Baryons (list) | Mesons (list)
Baryons: Nucleons | Hyperons | Exotic baryons | Pentaquarks
|

