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Gapped Goldstones at the cut-off scale: a non-relativistic EFT

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arxiv 2005.12924 v2 pith:XJJVGWCO submitted 2020-05-26 hep-th cond-mat.othercond-mat.str-el

classification hep-thcond-mat.othercond-mat.str-el
keywords gappedgoldstonesgaplessfieldmodesnon-abeliannonrelativisticnumber
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At finite density, the spontaneous breakdown of an internal non-Abelian symmetry dictates, along with gapless modes, modes whose gap is fixed by the algebra and proportional to the chemical potential: the gapped Goldstones. Generically the gap of these states is comparable to that of other non-universal excitations or to the energy scale where the dynamics is strongly coupled. This makes it non-straightforward to derive a universal ef effective field theory (EFT) description realizing all the symmetries. Focusing on the illustrative example of a fully broken SU (2) group, we demonstrate that such an EFT can be constructed by carving out around the Goldstones, gapless and gapped, at small 3-momentum. The rules governing the EFT, where the gapless Goldstones are soft while the gapped ones are slow, are those of standard nonrelativistic EFTs, like for instance nonrelativistic QED. In particular, the EFT Lagrangian formally preserves gapped Goldstone number, and processes where such number is not conserved are described inclusively by allowing for imaginary parts in the Wilson coefficients. Thus, while the symmetry is manifestly realized in the EFT, unitarity is not. We comment on the application of our construction to the study of the large charge sector of conformal field theories with non-Abelian symmetries.

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  1. An EFT for anisotropic anti-ferromagnets: gapped Goldstones, pseudo-Goldstones, and phase transitions

    cond-mat.str-el 2024-11 conditional novelty 6.0 of 10

    A new effective field theory for easy-plane anisotropic antiferromagnets in a magnetic field captures pseudo-Goldstone gaps, a first-order spin-flop transition, and a nontrivial quantization in the anisotropy-dominated phase.

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