nLab electroweak field

Redirected from "electroweak force".
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

The standard model of particle physics is a Yang-Mills gauge theory with gauge group (a discrete quotient of) SU(3)×SU(2)×U(1)SU(3) \times SU(2) \times U(1). Here the first factor is the gauge group of QCD while the (SU(2)×U(1))(SU(2) \times U(1))-gauge field is that transmitting what is called the electroweak force.

The name is due to the fact that this gauge field unifies the electromagnetic field and that transmitting the weak nuclear force: the Higgs mechanism induces a spontaneous symmetry breaking of the electroweak field to these two fields. See at electroweak symmetry breaking.

References

The electroweak interaction was introduced in:

The history of Weinberg 67 is recounted in:

Textbook account:

See also

Discussion in causal perturbation theory is in

See also:

  • José M. Gracia-Bondía, Karl-Henning Rehren, Joseph C. Várilly: The full electroweak interaction: an autonomous account [arXiv:2409.10668]

Last revised on November 25, 2024 at 16:48:11. See the history of this page for a list of all contributions to it.