Dynamical Chiral Symmetry Breaking by a Magnetic Field in QED

dc.creatorGusynin, V. P.
dc.creatorMiransky, V. A.
dc.creatorShovkovy, I. A.
dc.date1995-01-16
dc.date1995-11-09
dc.date.accessioned2026-07-07T11:14:31Z
dc.date.available2026-07-07T11:14:31Z
dc.descriptionIt is shown that the chiral symmetry is spontaneously broken by a constant magnetic field in QED. The dynamical mass of fermions (energy gap in the fermion spectrum) is $m_{dyn}\simeq C\sqrt{eB}\exp\left[-\left(π/α\right) ^{1/2}\right]$, where $B$ is the magnetic field, the constant $C$ is of order one and $α=e^2/4π$ is the renormalized coupling constant. Possible applications of this effect are discussed.
dc.description12 pages, LaTeX. The final journal version (with minor corrections)
dc.identifierhttps://arxiv.org/abs/hep-ph/9501304
dc.identifierhttp://arxiv.org/abs/hep-ph/9501304
dc.identifierPhys.Rev.D52:4747-4751,1995
dc.identifierdoi:10.1103/PhysRevD.52.4747
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/192094
dc.subjectHigh Energy Physics - Phenomenology
dc.subjectHigh Energy Physics - Theory
dc.titleDynamical Chiral Symmetry Breaking by a Magnetic Field in QED
dc.typetext

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