Exact equivalence between one-dimensional Bose gases interacting via hard-sphere and zero-range potentials
arXiv:1108.3723 · doi:10.1209/0295-5075/98/10010
Abstract
We prove the equivalence between the hard-sphere Bose gas and a system with momentum-dependent zero-range interactions in one spatial dimension, which we call extended hard-sphere Bose gas. The two-body interaction in the latter model has the advantage of being a regular pseudopotential. The most immediate consequence is the existence of its Fourier transform, permitting the formulation of the problem in momentum space, not possible with the original hard-core interaction. In addition, in the extended system, interactions are defined in terms of the scattering length, positive or negative, identified with the hard-sphere diameter only when it is positive. We are then able to obtain, directly in the thermodynamic limit, the ground state energy of the strongly repulsive Lieb-Liniger gas and, more importantly, the energy of the lowest-lying super Tonks-Girardeau gas state with finite, strongly attractive interactions, in perturbation theory from the novel extended hard-sphere Bose gas. Tan relations involving the large-momentum behavior of the Lieb-Liniger gas are also derived, and then applied to the super Tonks-Girardeau gas within our perturbative approach.
5 pages, 2 figures. Final published version
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- Field-theoretical aspects of one-dimensional Bose and Fermi gases with contact interactions
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- Comparative study of one-dimensional Bose and Fermi gases with contact interactions from the viewpoint of universal relations for correlation functions
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- From few to many body degrees of freedom