nLab compact QED

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

Quantum Field Theory

algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)

Introduction

Concepts

field theory:

Lagrangian field theory

quantization

quantum mechanical system, quantum probability

free field quantization

gauge theories

interacting field quantization

renormalization

Theorems

States and observables

Operator algebra

Local QFT

Perturbative QFT

Contents

Idea

What is called compact QED (following Polyakov 1975, 1977, 1987 §4.3) is quantum electrodynamics (QED) with the compactness of the U ( 1 ) U(1) gauge group taken properly into account (which is not typically done in perturbation theory).

The pleonastic terminology results from the infamous tradition in parts of theoretical physics to conflate Lie groups — here the compact U ( 1 ) U(1) or the non-compact \mathbb{R} — , with their Lie algebras, which here in both cases is 𝔲(1)\mathfrak{u}(1) \simeq \mathbb{R}. After this conflation, people have to speak of a “compact U(1)U(1)” to indicate that they really mean the circle group, cf. Preskill 1984 p. 471.

In particular, in the context of “compact QED” one considers magnetic monopole backgrounds and condensates which in 3 dimensions are argued (Polyakov 1975, 1977, 1997) to exhibit confinement in an abelian version of the dual superconductor model of color confinement.

References

The original discussion:

See also:

Further discussion:

Last revised on May 14, 2026 at 13:22:15. See the history of this page for a list of all contributions to it.