<p>Lattice <i>ℤ</i><sub>3</sub> theories with complex actions share many key features with finite- density QCD including a sign problem and <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13130_2025_25733_Article_IEq1.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">CK</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{CK} \)</EquationSource> </InlineEquation> symmetry. Complex <i>ℤ</i><sub>3</sub> spin and gauge models exhibit a generalized Kramers-Wannier duality mapping them onto chiral <i>ℤ</i><sub>3</sub> spin and gauge models, which are simulatable with standard lattice methods in large regions of parameter space. The Migdal-Kadanoff real-space renormalization group (RG) preserves this duality, and we use it to compute the approximate phase diagram of both spin and gauge <i>ℤ</i><sub>3</sub> models in dimensions one through four. Chiral <i>ℤ</i><sub>3</sub> spin models are known to exhibit a Devil’s Flower phase structure, with inhomogeneous phases that can be thought of as <i>ℤ</i><sub>3</sub> analogues of chiral spirals. Out of the large class of models we study, we find that only chiral spin models and their duals have a Devil’s Flower structure with an infinite set of inhomogeneous phases, a result we attribute to Elitzur’s theorem. We also find that different forms of the Migdal-Kadanoff RG produce different numbers of phases, a violation of the expectation for universal behavior from a real-space RG. We discuss extensions of our work to <i>ℤ</i><sub><i>N</i></sub> models, SU(<i>N</i>) models and nonzero temperature.</p>

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Exotic phases in finite-density 3 theories

  • Michael C. Ogilvie,
  • Moses A. Schindler,
  • Stella T. Schindler

摘要

Lattice 3 theories with complex actions share many key features with finite- density QCD including a sign problem and CK \( \mathcal{CK} \) symmetry. Complex 3 spin and gauge models exhibit a generalized Kramers-Wannier duality mapping them onto chiral 3 spin and gauge models, which are simulatable with standard lattice methods in large regions of parameter space. The Migdal-Kadanoff real-space renormalization group (RG) preserves this duality, and we use it to compute the approximate phase diagram of both spin and gauge 3 models in dimensions one through four. Chiral 3 spin models are known to exhibit a Devil’s Flower phase structure, with inhomogeneous phases that can be thought of as 3 analogues of chiral spirals. Out of the large class of models we study, we find that only chiral spin models and their duals have a Devil’s Flower structure with an infinite set of inhomogeneous phases, a result we attribute to Elitzur’s theorem. We also find that different forms of the Migdal-Kadanoff RG produce different numbers of phases, a violation of the expectation for universal behavior from a real-space RG. We discuss extensions of our work to N models, SU(N) models and nonzero temperature.