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arxiv: 2512.04150 · v2 · submitted 2025-12-03 · ❄️ cond-mat.str-el · cond-mat.mes-hall· hep-lat· hep-th

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Symmetry-Enforced Fermi Surfaces

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classification ❄️ cond-mat.str-el cond-mat.mes-hallhep-lathep-th
keywords symmetryfermisymmetry-enforcedgroupsurfacesfermionlatticemathbf
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We identify a symmetry that enforces every symmetric model to have a Fermi surface. These symmetry-enforced Fermi surfaces are realizations of a powerful form of symmetry-enforced gaplessness. The symmetry we construct exists in quantum lattice fermion models on a $d$-dimensional Bravais lattice, and is generated by the on-site U(1) fermion number symmetry and non-on-site Majorana translation symmetry. The resulting symmetry group is a noncompact Lie group closely related to the Onsager algebra. For a symmetry-enforced Fermi surface $\cal{F}$, we show that this UV symmetry group always includes the subgroup of the ersatz Fermi liquid L$_{\cal{F}}$U(1) symmetry group formed by even functions ${f(\mathbf{k})\in\mathrm{U}(1)}$ with ${\mathbf{k}\in \cal{F}}$. Furthermore, we comment on the topology of these symmetry-enforced Fermi surfaces, proving they generically exhibit at least two noncontractible components (i.e., open orbits).

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Cited by 2 Pith papers

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  1. Symmetry Spans and Enforced Gaplessness

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    Symmetry spans enforce gaplessness when a symmetry E embedded into two larger symmetries C and D has no compatible gapped phase that restricts from both.

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