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Exact evaluation of large-charge correlation functions in non-relativistic conformal field theory

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arxiv 2403.18898 v2 pith:CUEG4VAT submitted 2024-03-27 hep-th cond-mat.quant-gashep-phnucl-th

classification hep-thcond-mat.quant-gashep-phnucl-th
keywords fieldlarge-chargetheoryconformalcorrelationfunctionschargecompute
verification ladder T0 review T1 audit T2 compute T3 formal
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The large-charge master field which generates all n-point correlation functions with an insertion of large charge Q in non-relativistic conformal field theory is obtained. This field is used to compute Schr\"odinger-invariant n-point correlation functions of large-charge operators via a direct evaluation of the path integral. Conformal dimensions are found to agree with calculations based on the state-operator correspondence. The master field solution exhibits an emergent harmonic trap whose frequency is a function of the Euclidean time. The large-charge effective action with operator insertions describes a droplet of superfluid matter whose spatial size scales with the time separation of sources. The solution is used to compute Schr\"odinger symmetry breaking corrections in the large-charge effective field theory (EFT) due to a finite scattering length in the fundamental theory of fermions near unitarity. The scaling of these effects in the large-charge power counting scheme is established, and the size of the effects is quantified using input from quantum Monte Carlo simulations of the near-unitary gas, as well as from the large-N expansion at large charge.

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Cited by 2 Pith papers

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  1. Trapping-potential dependence of the unitary Fermi gas at the BCS-BEC crossover

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    Trap-induced corrections to the unitary Fermi gas phonon spectrum and dynamic structure factor are computed in three EFT/WKB regimes, with low-energy corrections depending on trap shape and high-energy corrections set...

  2. Unnuclear matter at large-charge

    nucl-th 2025-01 conditional novelty 6.0 of 10

    In the large-charge EFT of neutrons, effective-range corrections to the two-point function first appear at second order in the effective range, and the deformed theory has a narrow but usable perturbative window for Q...

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