Chiral soliton lattice in QCD-like theories
arXiv:1905.11409 · doi:10.1007/JHEP12(2019)029
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 potential carries a crystalline condensate of neutral pions: the chiral soliton lattice (CSL). While the result was obtained in a model-independent manner using effective field theory 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 inhomogeneous 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 quasiparticle 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.
arXiv comment1+26 pages; v2 matches published version
References in corpus (27)
- Chiral perturbation theory
- Quantum field theory in a magnetic field: From quantum chromodynamics to graphene and Dirac semimetals
- QCD at finite isospin density
- Absence of Quantum Time Crystals
- Chiral Perturbation Theory
- Impossibility of Spontaneously Rotating Time-Crystals: A No-Go Theorem
- QCD-like Theories at Finite Baryon Density
- Inhomogeneous chiral condensates
- Magnetic catalysis and anisotropic confinement in QCD
- QCD-like Theories at Finite Baryon and Isospin Density
- Axial anomaly and magnetism of nuclear and quark matter
- QCD phase diagram for nonzero isospin-asymmetry
- Exceptional Confinement in G(2) Gauge Theory
- Massive Nambu-Goldstone Bosons
- Chiral Soliton Lattice and Charged Pion Condensation in Strong Magnetic Fields
- General Effective Actions
- Phonons, pions and quasi-long-range order in spatially modulated chiral condensates
- Magnetic structure of isospin-asymmetric QCD matter in neutron stars
- Anomalous effects of dense matter under rotation
- Landau-Peierls instability in a Fulde-Ferrell type inhomogeneous chiral condensed phase
- Invariant Effective Actions, Cohomology of Homogeneous Spaces and Anomalies
- Two-flavor chiral perturbation theory at nonzero isospin: Pion condensation at zero temperature
- Anomalous electrodynamics of neutral pion matter in strong magnetic fields
- Anomaly-Induced Inhomogeneous Phase in Quark Matter without the Sign Problem
- Gauged Wess-Zumino terms for a general coset space
- Inhomogeneous phases in the 1+1 dimensional Gross-Neveu model at finite number of fermion flavors
- Lattice QCD with mismatched Fermi surfaces
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- Quantum nucleation of topological solitons
- Formation of Chiral Soliton Lattice
- Chiral soliton lattice at next-to-leading order
- Quasicrystals in QCD
- Competition of chiral soliton lattice and Abrikosov vortex lattice in QCD with isospin chemical potential
- Phonon and Shifton from a Real Modulated Scalar
- Solitonic ground state in supersymmetric theory in background
- Novel transition dynamics of topological solitons
- Holographic QCD Matter: Chiral Soliton Lattices in Strong Magnetic Field
- Floquet vacuum engineering: Laser-driven chiral soliton lattice in the QCD vacuum
- Vorticity-induced effects from Wess-Zumino-Witten terms
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