Abstract

Recently, it has been shown that the ground state of quantum chromodynamics (QCD) in sufficiently strong magnetic fields and at moderate baryon number chemical po- tential carries a crystalline condensate of neutral pions: the chiral soliton lattice (CSL) [1]. While the result was obtained in a model-independent manner using effective field the- ory techniques, its realization from first principles using lattice Monte Carlo simulation is hampered by the infamous sign problem. Here we show that CSL, or a similar inhomoge- neous phase, also appears in the phase diagram of a class of vector-like gauge theories that do not suffer from the sign problem even in the presence of a baryon chemical potential and external magnetic field. We also show that the onset of nonuniform order manifests itself already in the adjacent homogeneous Bose-Einstein-condensation phase through a characteristic roton-like minimum in the dispersion relation of the lowest-lying quasipar- ticle mode. Last but not least, our work gives a class of explicit counterexamples to the long-standing conjecture that positivity of the determinant of the Dirac operator (that is, absence of the sign problem) in a vector-like gauge theory precludes spontaneous breaking of translational invariance, and thus implies the absence of inhomogeneous phases in the phase diagram of the theory.

Highlights

  • Recently, it has been shown that the ground state of quantum chromodynamics (QCD) in sufficiently strong magnetic fields and at moderate baryon number chemical potential carries a crystalline condensate of neutral pions: the chiral soliton lattice (CSL) [1]

  • We show that CSL, or a similar inhomogeneous phase, appears in the phase diagram of a class of vector-like gauge theories that do not suffer from the sign problem even in the presence of a baryon chemical potential and external magnetic field

  • The goal of this paper is to show that the CSL phase, or a similar inhomogeneous phase, appears in the phase diagram of an infinite class of QCD-like theories free of the sign problem

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Summary

Effective field theory setup

We consider a class of QCD-like theories where quarks transform in a real or pseudoreal representation of the gauge group. It is well-known that for N flavors of massless quarks, (pseudo)real QCD-like theories possess an enlarged global symmetry, G = SU(2N ) This includes the usual chiral symmetry of QCD, SU(N )L × SU(N )R × U(1)B, as a subgroup. The low-energy EFT for the NG degrees of freedom is constructed as a nonlinear sigma model on the coset space G/H It would appear from our above discussion that we need two different EFTs, one for real and one for pseudoreal theories. The low-energy physics will be dominated by the electrically neutral NG modes To construct their EFT description, it is sufficient to consider the subgroups of G and H, left intact by the magnetic field. This has to be specified concretely before we can proceed with the analysis of the EFT

Wess-Zumino term
Effective Lagrangian and Hamiltonian
Ground state
Excitation spectrum
Away from the chiral limit
Spectrum in the BEC phase
Spectrum in the CSL phase
Summary and conclusions
A Variational minimization of the Hamiltonian
States with constant θ
States with periodic θ and linear φ
States with periodic θ and CSL-like φ
Full Text
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