Abstract

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 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.

Highlights

  • With systems that spontaneously break spacetime symmetries as well, in which case Goldstone theorem allows for a much richer set of possibilities

  • Integrating out the gapped modes in favor of an ordinary effective field theory (EFT) for the gapless ones, while certainly doable, does not seem satisfactory, as it would preclude describing those aspects of the dynamics that are dictated by symmetry

  • In order to account for the gapped Goldstone’s decay or annihilation, we argue that the nonrelativistic EFT (NREFT) must contain imaginary coefficients, which makes it non-unitary

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Summary

A benchmark model: the linear triplet

We present a simple model with internal SU(2) symmetry, admitting a finite density state for one of the charges where SU(2) and time translations are broken down to a diagonal subgroup, H × SU(2) → H. We study perturbations around such state, identify the gapped Goldstone modes and examine the amplitudes for their scattering and annihilation in the regime where their 3-momentum is small. The model is weakly coupled and renormalizable, and all observables can be computed perturbatively. We will use it as the main example to match the effective theory developed in the rest of the paper

The model
Interactions of slow gapped Goldstones
Building the EFT with the left parametrization
The NREFT to quadratic order
Gapped Goldstone number conservation and non-unitarity
Interactions and power counting
Integrating out the gapped Goldstones: a less effective field theory
Conclusions and future directions
Gapped Goldstone decay
B The spacetime coset construction
The inverse Higgs constraint in the NREFT
C NREFT details
Loops in dimensional regularization
Full Text
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