Abstract
A constant magnetic field in 3+1 and 2+1 dimensions is a strong catalyst of dynamical chiral symmetry breaking, leading to the generation of a fermion dynamical mass even at the weakest attractive interaction between fermions. The essence of this effect is the dimensional reduction D → D - 2 in the dynamics of fermion pairing in a magnetic field. The effect is illustrated in the Nambu-Jona-Lasinio (NJL) model and QED. Possible applications of this effect and its extension to inhomogeneous field configurations are discussed.
Cite
CITATION STYLE
Miransky, V. A. (1996). Catalysis of Dynamical Symmetry Breaking by a Magnetic Field. Progress of Theoretical Physics Supplement, (123), 49–59. https://doi.org/10.1143/PTPS.123.49
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