Catalysis of Dynamical Symmetry Breaking by a Magnetic Field
arXiv:hep-th/9511224 · doi:10.1143/PTPS.123.49
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 mass even at the weakest attractive interaction between fermions. The essence of this effect is the dimensional reduction in the dynamics of fermion pairing in a magnetic field. The effect is illustrated in the Nambu-Jona-Lasinio model and QED. Possible applications of this effect and its extension to inhomogeneous field configurations are discussed.
Based on a talk given at Yukawa International Seminar'95 "From the Standard Model to Grand Unified Theories",15 pages,Latex
Cited by in corpus (16)
- Magnetic field driven metal-insulator phase transition in planar systems
- Magnetic oscillations in planar systems with the Dirac-like spectrum of quasiparticle excitations
- Magnetic catalysis and anisotropic confinement in QCD
- Theory of the Magnetic Catalysis of Chiral Symmetry Breaking in QED
- Magnetic Catalysis: A Review
- Quark droplets stability induced by external magnetic field
- Strong-Field Physics in QED and QCD: From Fundamentals to Applications
- Chiral Transition Within Effective Quark Models Under Magnetic Fields
- The Influence of an External Chromomagnetic Field on Color Superconductivity
- Magnetic catalysis of parity breaking in a massive Gross-Neveu model and high-temperature superconductivity
- The influence of a repulsive vector coupling in magnetized quark matter
- Does there arise a significant enhancement of the dynamical quark mass in external magnetic field?
- Dynamical Symmetry Breaking on a Cylinder in Magnetic Field
- Quark and pion condensation in a chromomagnetic background field
- Large N dynamics in QED in a magnetic field
- Low-temperature renormalization group study of uniformly frustrated models for type-II superconductors