The chiral soliton lattice is a universal feature of gauged Skyrme theory at finite baryon density in magnetic fields, remains unchanged under sub-leading large-Nc corrections, and produces a gapped, shifted Dirac spectrum when coupled to quarks.
Topological crystals and soliton lattices in a Gross-Neveu model with Hilbert-space fragmentation
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abstract
We explore the finite-density phase diagram of the single-flavour Gross-Neveu-Wilson (GNW) model using matrix product state (MPS) simulations. At zero temperature and along the symmetry line of the phase diagram, we find a sequence of inhomogeneous ground states that arise through a real-space version of the mechanism of Hilbert-space fragmentation. For weak interactions, doping the symmetry-protected topological (SPT) phase of the GNW model leads to localized charges or holes at periodic arrangements of immobile topological defects separating the fragmented subchains: a topological crystal. Increasing the interactions, we observe a transition into a parity-broken phase with a pseudoscalar condensate displaying a modulated periodic pattern. This soliton lattice is a sequence of topological charges corresponding to anti-kinks, which also bind the doped fermions at their respective centers. Out of this symmetry line, we show that quasi-spiral profiles appear with a characteristic wavevector set by the density $k = 2{\pi}{\rho}$, providing non-perturbative evidence for chiral spirals beyond the large-N limit. These results demonstrate that various exotic inhomogeneous phases can arise in lattice field theories, and motivate the use of quantum simulators to confirm such QCD-inspired phenomena in future experiments.
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Universality of the chiral soliton lattice and its interaction with quark matter
The chiral soliton lattice is a universal feature of gauged Skyrme theory at finite baryon density in magnetic fields, remains unchanged under sub-leading large-Nc corrections, and produces a gapped, shifted Dirac spectrum when coupled to quarks.