Omega meson

In today's world, Omega meson has become a relevant and interesting topic for many people. Whether it's its impact on society, its relevance in history, or its influence on popular culture, Omega meson has captured the attention of many people around the world. In this article, we will explore the different facets of Omega meson, analyzing its importance, its evolution over time, and its role in different contexts. Through a comprehensive and multidisciplinary approach, we will attempt to shed light on this intriguing and significant topic, offering our readers a deeper and more comprehensive view of Omega meson.

Omega meson
Composition
StatisticsBosonic
FamilyMesons
InteractionsStrong, weak, electromagnetic, gravity
Symbol
ω
AntiparticleSelf
TheorizedYoichiro Nambu (1957)
DiscoveredLawrence Berkeley National Laboratory (1961)
Types1
Mass782.66±0.13 MeV/c2
Mean lifetime(7.58±0.11)×10−23 s
Decays into
π+
+
π0
+
π
or
π0
+
γ
Electric charge0 e
Spin1
Isospin0
Hypercharge0
Parity−1
C parity−1

The omega meson (
ω
) is a flavourless meson formed from a superposition of an up quarkantiquark and a down quark–antiquark pair. It is part of the vector meson nonet and mediates the nuclear force along with pions and rho mesons.

Properties

The most common decay mode for the ω meson is
π+

π0

π
at 89.2±0.7%, followed by
π0

γ
at 8.34±0.26%.

Particle name Particle
symbol
Antiparticle
symbol
Quark
content
Rest mass (MeV/c2) IG JPC S C B' Mean lifetime (s) Commonly decays to

(>5% of decays)

Omega meson
ω
(782)
Self 782.66 ± 0.13 0 1−− 0 0 0 (7.58±0.11)×10−23 s
π+
+
π0
+
π
 or

π0
+
γ

The quark composition of the
ω
meson can be thought of as a mix between
u

u
,
d

d
and
s

s
states, but it is very nearly a pure symmetric
u

u
-
d

d
state. This can be shown by deconstructing the wave function of the
ω
into its component parts. We see that the
ω
and
ϕ
mesons are mixtures of the SU(3) wave functions as follows.

,
,

where

is the nonet mixing angle,
and
.

The mixing angle at which the components decouple completely can be calculated to be , which almost corresponds to the actual value calculated from the masses of 35°. Therefore, the
ω
meson is nearly a pure symmetric
u

u
-
d

d
state.

See also

References

  1. ^ Nambu, Yoichiro (April 25, 1957). "Possible Existence of a Heavy Neutral Meson". Physical Review. 106 (6): 1366–1367. Bibcode:1957PhRv..106.1366N. doi:10.1103/PhysRev.106.1366.
  2. ^ Maglić, B. C.; Alvarez, L. W.; Rosenfeld, A. H.; Stevenson, M. L. (August 14, 1961). "Evidence for a T=0 three-pion resonance". Physical Review Letters. 7 (5): 178–182. Bibcode:1961PhRvL...7..178M. doi:10.1103/physrevlett.7.178. S2CID 121570977.
  3. ^ Maglich, B. (1976). "Discovery of omega meson-first neutral vector meson: one researcher's personal account - Discovery story". Advanced Experimental Physics. 5: 79–105.
  4. ^ Gell-Mann, M. (March 15, 1961). "The Eightfold Way: A Theory of Strong Interaction Symmetry" (TID-12608). Pasadena, CA: California Inst. of Tech., Synchrotron Laboratory: 24. doi:10.2172/4008239. {{cite journal}}: Cite journal requires |journal= (help)
  5. ^ Ne'eman, Y. (August 1961). "Derivation of Strong Interactions from a Gauge Invariance". Nuclear Physics. 26 (2). Amsterdam: North-Ho lland Publishing Co.: 222–229. Bibcode:1961NucPh..26..222N. doi:10.1016/0029-5582(61)90134-1.
  6. ^ a b Zyla, P. A. (2021) . "Particle listing - ω(782)" (PDF). Particle Data Group. Retrieved June 9, 2021.
  7. ^ Amsler, C.; DeGrand, T.; Krusche, B. (August 2019). "15. Quark Model" (PDF). Particle Data Group. Retrieved 9 June 2021.