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Non-Invertible Defects in Nonlinear Sigma Models and Coupling to Topological Orders

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arxiv 2212.08608 v2 pith:TBPKV6JA submitted 2022-12-16 cond-mat.str-el hep-thquant-ph

classification cond-mat.str-elhep-thquant-ph
keywords defectssigmamodelsnonlinearmagneticnon-invertiblequantumtheories
verification ladder T0 review T1 audit T2 compute T3 formal
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Nonlinear sigma models appear in a wide variety of physics contexts, such as the long-range order with spontaneously broken continuous global symmetries. There are also large classes of quantum criticality admit sigma model descriptions in their phase diagrams without known ultraviolet complete quantum field theory descriptions. We investigate defects in general nonlinear sigma models in any spacetime dimensions, which include the "electric" defects that are characterized by topological interactions on the defects, and the "magnetic" defects that are characterized by the isometries and homotopy groups. We use an analogue of the charge-flux attachment to show that the magnetic defects are in general non-invertible, and the electric and magnetic defects form junctions that combine defects of different dimensions into analogues of higher-group symmetry. We explore generalizations that couple nonlinear sigma models to topological quantum field theories by defect attachment, which modifies the non-invertible fusion and braiding of the defects. We discuss several applications, including constraints on energy scales and scenarios of low energy dynamics with spontaneous symmetry breaking in gauge theories, and axion gauge theories.

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Cited by 3 Pith papers

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  1. SymTFT for Continuous Symmetries: Non-linear Realizations and Spontaneous Breaking

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    The paper shows that local gauge theories in 3+1d and 2+1d can realize SPT, SET, and symmetry-breaking phase transitions for one-form symmetries, including phases distinguished by symmetry fractionalization.

  3. Twisted Partition Functions as Order Parameters

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    Twisted partition functions work as an order parameter that separates broken-symmetry, symmetry-protected, and symmetry-enriched phases, reproduce the Wilson-'t Hooft classification in 4d gauge theories, and tie U(1) ...

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