Effective interactions, Fermi-Bose duality, and ground states of ultracold atomic vapors in tight de Broglie waveguides

TL;DR

This paper reviews the derivation of effective 1D atomic interactions in tight waveguides, explores Fermi-Bose duality, and applies these concepts to determine ground states of ultracold atomic vapors with spin considerations.

Contribution

It introduces a unified framework for 1D interactions, including odd-wave scattering, and extends Fermi-Bose duality to spinor gases with both even and odd-wave interactions.

Findings

Fermi-Bose duality holds for spinor gases with mixed interactions.

Derived phase diagram for ground-state total spin of spinor Fermi gases.

Applied Fermi-Bose mapping to various ultracold atomic systems.

Abstract

Derivation of effective zero-range one-dimensional (1D) interactions between atoms in tight waveguides is reviewed, as is the Fermi-Bose mapping method for determination of exact and strongly-correlated states of ultracold bosonic and fermionic atomic vapors in such waveguides, including spin degrees of freedom. Odd-wave 1D interactions derived from 3D p-wave scattering are included as well as the usual even-wave interactions derived from 3D s-wave scattering, with emphasis on the role of 3D Feshbach resonances for selectively enhancing s-wave or p-wave interactions. A duality between 1D fermions and bosons with zero-range interactions suggested by Cheon and Shigehara is shown to hold for the effective 1D dynamics of a spinor Fermi gas with both even and odd-wave interactions and that of a spinor Bose gas with even and odd-wave interactions, with even(odd)-wave Bose coupling constants inversely related to odd(even)-wave Fermi coupling constants. Some recent applications of Fermi-Bose mapping to determination of many-body ground states of Bose gases and of both magnetically trapped, spin-aligned and optically trapped, spin-free Fermi gases are described, and a new generalized Fermi-Bose mapping is used to determine the phase diagram of ground-state total spin of the spinor Fermi gas as a function of the even and odd-wave coupling constants.