Abstract

We study operators in Schrödinger invariant field theories (non-relativistic conformal field theories or NRCFTs) with large charge (particle number) and spin. Via the state-operator correspondence for NRCFTs, such operators correspond to states of a superfluid in a harmonic trap with phonons or vortices. Using the effective field theory of the Goldstone mode, we compute the dimensions of operators to leading order in the angular momentum L and charge Q. We find a diverse set of scaling behaviors for NRCFTs in both d = 2 and d = 3 spatial dimensions. These results apply to theories with a superfluid phase, such as unitary fermions or critical anyon systems.

Highlights

  • 133Cs [21], 85Rb [22],39K [23], and various spin chain models [24]

  • We study operators in Schrodinger invariant field theories with large charge and spin

  • We find a diverse set of scaling behaviors for non-relativistic conformal field theories (NRCFTs) in both d = 2 and d = 3 spatial dimensions

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Summary

The set up: superfluid hydrodynamics and large charge NRCFT

We briefly review the superfluid hydrodynamics in the Hamiltonian formalism, specialized to the case of a Schrodinger invariant system in a harmonic potential. We’ll be interested in excited state configurations which carry some angular momentum These will correspond to spinful operators in the large charge sector of the NRCFTs which the superfluid EFT describes. The other configuration of a superfluid that can support angular momentum is a vortex, which gives rise to a singular velocity field of the condensate This is a distinct semi-classical saddle point which is not related to the ground state. These two excitations, phonons and vortices, are the configurations of the superfluid we know support angular momentum. By answering this and using the superfluid EFT defined above we compute the scaling behavior of operators carrying charge and angular momentum

Phonons
Single vortex in the trap
Multi-vortex profile
Conclusions and future directions
A Particle-vortex duality
B A contour integral
Full Text
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