nLab
h1-meson

Contents

Context

Fields and quanta

fields and particles in particle physics

and in the standard model of particle physics:

force field gauge bosons

scalar bosons

matter field fermions (spinors, Dirac fields)

flavors of fundamental fermions in the
standard model of particle physics:
generation of fermions1st generation2nd generation3d generation
quarks (qq)
up-typeup quark (uu)charm quark (cc)top quark (tt)
down-typedown quark (dd)strange quark (ss)bottom quark (bb)
leptons
chargedelectronmuontauon
neutralelectron neutrinomuon neutrinotau neutrino
bound states:
mesonslight mesons:
pion (udu d)
ρ-meson (udu d)
ω-meson (udu d)
f1-meson
a1-meson
strange-mesons:
ϕ-meson (ss¯s \bar s),
kaon, K*-meson (usu s, dsd s)
eta-meson (uu+dd+ssu u + d d + s s)

charmed heavy mesons:
D-meson (uc u c, dcd c, scs c)
J/ψ-meson (cc¯c \bar c)
bottom heavy mesons:
B-meson (qbq b)
ϒ-meson (bb¯b \bar b)
baryonsnucleons:
proton (uud)(u u d)
neutron (udd)(u d d)

(also: antiparticles)

effective particles

hadrons (bound states of the above quarks)

solitons

in grand unified theory

minimally extended supersymmetric standard model

superpartners

bosinos:

sfermions:

dark matter candidates

Exotica

auxiliary fields

Contents

Idea

One of the light vector mesons, with Wigner classification being a Lorentz group bivector (DHR 11, DHR 12) and isospin scalar.

References

  • J. C. R. Bloch, Yu. L. Kalinovsky, C. D. Roberts, S. M. Schmidt, Describing a 1a_1 and b 1b_1 decays, Phys. Rev. D60:111502, 1999 (arXiv:nucl-th/9906038)

Discussion within holographic QCD:

  • Sophia K. Domokos, Jeffrey Harvey, Andrew B. Royston, Completing the framework of AdS/QCD: h 1h_1/b 1b_1 mesons and excited ω\omega/ρ\rho‘s, JHEP 05(2011)107 (arXiv:1101.3315)

  • Sophia K. Domokos, Jeffrey Harvey, Andrew B. Royston, Successes and Failures of a More Comprehensive Hard Wall AdS/QCD, JHEP 04(2013)104 (arXiv:1210.6351)

Last revised on May 8, 2020 at 16:30:27. See the history of this page for a list of all contributions to it.