Spin-incoherent Luttinger liquid of one-dimensional SU() fermions
arXiv:1805.02383 · doi:10.1103/PhysRevA.98.013623
Abstract
We theoretically investigate one-dimensional (1D) SU() fermions in the regime of spin-incoherent Luttinger liquid. We specifically focus on the Tonks-Girardeau gas limit where its density is sufficiently low that effective repulsions between atoms become infinite. In such case, spin exchange energy of 1D SU() fermions vanishes and all spin configurations are degenerate, which automatically puts them into spin-incoherent regime. In this limit, we are able to express the single-particle density matrices in terms of those of anyons. This allows us to numerically simulate the number of particles up to . We numerically calculate single-particle density matrices in two cases: (1) equal populations for each spin components (balanced) and (2) all manifolds included. In contrast to noninteracting multi-component fermions, the momentum distributions are broadened due to strong interactions. As increases, the momentum distributions are less broadened for fixed , while they are more broadened for fixed number of particle per spin component. We then compare numerically calculated high momentum tails with analytical predictions which are proportional to , in good agreement. Thus, our theoretical study provides a comparison with the experiments of repulsive multicomponent alkaline-earth fermions with a tunable SU() spin-symmetry in the spin-incoherent regime.
arXiv comment8 pages and 5 figures
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