Finite Isospin Chiral Perturbation Theory in a Magnetic Field
arXiv:1501.02737 · doi:10.1103/PhysRevC.91.045202
Abstract
The phase diagram of finite isospin, zero temperature QCD with the pions coupled to photons in a uniform external magnetic field is explored in the low field, small isospin density regime for which chiral perturbation theory is a valid description. For realistic pion masses, the system behaves as a type-II superconductor: a uniform superconducting state is formed at low-enough magnetic fields, a vortex state for intermediate magnetic fields and finally a normal state for large magnetic fields. In each these phases (including the vortex phase), the remains uncondensed just as in the zero-external field problem. The critical magnetic field where the phase transition from the uniform superconducting state to a vortex state occurs was found numerically.
9 pages, 4 figures
References in corpus (7)
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- Chiral transition in a strong magnetic background
- Quark-hadron phase transition in a magnetic field
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Cited by in corpus (10)
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- Quark, pion and axial condensates in three-flavor finite isospin chiral perturbation theory
- Heavy-quark spin polarization induced by the Kondo effect in a magnetic field
- Vortex solutions in the Abelian Higgs Model with a neutral scalar
- Phonon modes of magnetic vortex lattices in finite isospin chiral perturbation theory
- Multicomponent superfluidity in two-color QCD at finite density at next-to-leading order
- Chiral Symmetry Breaking and Pion Decay in a Magnetic Field