fields and particles in particle physics
and in the standard model of particle physics:
matter field fermions (spinors, Dirac fields)
| flavors of fundamental fermions in the standard model of particle physics: | |||
|---|---|---|---|
| generation of fermions | 1st generation | 2nd generation | 3d generation |
| quarks () | |||
| up-type | up quark () | charm quark () | top quark () |
| down-type | down quark () | strange quark () | bottom quark () |
| leptons | |||
| charged | electron | muon | tauon |
| neutral | electron neutrino | muon neutrino | tau neutrino |
| bound states: | |||
| mesons | light mesons: pion () ρ-meson () ω-meson () f1-meson a1-meson | strange-mesons: ϕ-meson (), kaon, K*-meson (, ) eta-meson () charmed heavy mesons: D-meson (, , ) J/ψ-meson () | bottom heavy mesons: B-meson () ϒ-meson () |
| baryons | nucleons: proton neutron |
(also: antiparticles)
hadrons (bound states of the above quarks)
minimally extended supersymmetric standard model
bosinos:
dark matter candidates
Exotica
algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
quantum mechanical system, quantum probability
interacting field quantization
What is called compact QED (following Polyakov 1975, 1977, 1987 §4.3) is quantum electrodynamics (QED) with the compactness of the 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 or the non-compact — , with their Lie algebras, which here in both cases is . After this conflation, people have to speak of a “compact ” 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.
The original discussion:
Alexander M. Polyakov: Compact Gauge Fields and the Infrared Catastrophe, Physics Letters B 59 1 (1975) [doi:10.1016/0370-2693(75)90162-8]
Alexander M. Polyakov: Quark confinement and topology of gauge theories, Nuclear Physics B 120 3 (1977) 429–458 [doi:10.1016/0550-3213(77)90086-4]
Alexander Polyakov, §4.3 in: Gauge Fields and Strings, Routledge, Taylor and Francis (1987, 2021) [doi:10.1201/9780203755082, oapen:20.500.12657/50871]
Alexander Polyakov: Confining strings, Nuclear Physics B 486 1–2 (1997) 23–33 [doi:10.1016/S0550-3213(96)00601-3]
See also:
Further discussion:
J. Jersak et al.: Charge Renormalization in Compact Lattice QED, Nucl. Phys. B 251 (1985) 299–310 [doi:10.1016/0550-3213(85)90263-9]
Ian I. Kogan, Alex Kovner: Compact — a simple example of a variational calculation in a gauge theory, Phys. Rev. D 51 (1995) 1948–1955 [doi:10.1103/PhysRevD.51.1948, arXiv:hep-th/9410067]
D. V. Antonov: Various properties of compact QED and confining strings, Phys. Lett. B 428 (1998) 3–4 [doi:10.1016/S0370-2693(98)00419-5, arXiv:hep-th/9802056]
Orlando Oliveira, Lee C. Loveridge, Paulo J. Silva: Compact QED: the photon propagator, confinement and positivity violation for the pure gauge theory, EPJ Web Conf. 274 02004 (2022) [doi:10.1051/epjconf/202227402004, arXiv:2211.12593]
M. Cristina Diamantini, Fernando Quevedo, Carlo A. Trugenberger, Luis Zapata: Universal Confining Strings: From Compact QED to the Hadron Spectrum [arXiv:2605.13791]
Last revised on May 14, 2026 at 13:22:15. See the history of this page for a list of all contributions to it.