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Berry Phase in Quantum Field Theory: Diabolical Points and Boundary Phenomena

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arxiv 2004.10758 v2 pith:K56IOM2K submitted 2020-04-22 cond-mat.str-el hep-th

classification cond-mat.str-elhep-th
keywords boundarydiabolicalphasepointstermsberryquantumconsideration
verification ladder T0 review T1 audit T2 compute T3 formal
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We study aspects of Berry phase in gapped many-body quantum systems by means of effective field theory. Once the parameters are promoted to spacetime-dependent background fields, such adiabatic phases are described by Wess-Zumino-Witten (WZW) and similar terms. In the presence of symmetries, there are also quantized invariants capturing generalized Thouless pumps. Consideration of these terms provides constraints on the phase diagram of many-body systems, implying the existence of gapless points in the phase diagram which are stable for topological reasons. We describe such diabolical points, realized by free fermions and gauge theories in various dimensions, which act as sources of "higher Berry curvature" and are protected by the quantization of the corresponding WZW terms or Thouless pump terms. These are analogous to Weyl nodes in a semimetal band structure. We argue that in the presence of a boundary, there are boundary diabolical points---parameter values where the boundary gap closes---which occupy arcs ending at the bulk diabolical points. Thus the boundary has an "anomaly in the space of couplings" in the sense of C\'ordova et al. Consideration of the topological effective action for the parameters also provides some new checks on conjectured infrared dualities and deconfined quantum criticality in 2+1d.

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Cited by 3 Pith papers

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    Generalized family anomalies for broken higher-group and non-invertible symmetries constrain RG flows and IR phases of QFT families, with explicit application to deformed 4d QCD.

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    In a Dirac fermion BCFT with SU(2) conformal boundary conditions parametrized by a three-sphere, the filled Fermi sea carries a higher Berry curvature whose integral is quantized, realizing Berry curvature flow and Ch...

  3. Generalized Symmetries Phase Transitions with Local Quantum Fields

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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.

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