Universal properties of hard-core bosons confined on one-dimensional lattices.pdf

Universal properties of hard-core bosons confined on one-dimensional lattices.pdf

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Universal properties of hard-core bosons confined on one-dimensional lattices

a r X i v : c o n d - m a t / 0 4 0 3 0 7 8 v 2 [ c o n d - m a t .s t a t - m e c h ] 2 9 S e p 2 0 0 4 Universal properties of hard-core bosons confined on one-dimensional lattices Marcos Rigol and Alejandro Muramatsu Institut fu?r Theoretische Physik III, Universita?t Stuttgart, Pfaffenwaldring 57, D-70550 Stuttgart, Germany. Based on an exact treatment of hard-core bosons confined on one-dimensional lattices, we obtain the large distance behavior of the one-particle density matrix, and show how it determines the occupation of the lowest natural orbital in the thermodynamic limit. We also study the occupation λη of the natural orbitals for large-η at low densities. Both quantities show universal behavior independently of the confining potential. Finite-size corrections and the momentum distribution function for finite systems are also analyzed. PACS numbers: 03.75.Hh, 05.30.Jp Trapped atomic gases at very low temperatures be- came in the past years a center of attention in atomic and condensed matter physics. Particularly interesting is the case where the dynamics of the system is restricted to one-dimension (1D) due to a strong transversal confine- ment. It has been shown recently [1] that in regimes of large positive scattering length, low densities, and low temperatures, a quasi-1D gas of bosons behaves as a gas of impenetrable particles, i.e., as hard-core bosons (HCB). Ultracold Bose gases in 1D have been realized experimentally [2], so that it is expected that soon it will be possible to make the 1D HCB gas a physical reality. The 1D gas of HCB was first introduced theoretically by Girardeau [3], who also established its exact mapping to a gas of noninteracting spinless fermions. Since then, it remained a subject of recurring attention, and a number of exact results were obtained for the momentum distri- bution function (MDF) n(k) and the one-particle density matrix (OPDM) ρ(x) in the homogeneous [4, 5] and the periodic [6] case. It was shown that n

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