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arXiv:cond-mat/9703215 · Nuclear Physics B

Supersymmetric model of a 2D long-range Bose liquid

M. V. Feigel’man, M. A. Skvortsov

Published Dec 1, 1997• 15 citations
arXivHTMLPDF
DOI
10.1016/s0550-3213(97)00616-0

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The ννν-component two-dimensional (2D) Bose liquid is considered. It is shown that the finite temperature phase transition exists in this 2D continuously degenerate multicomponent system. The new type of quasi-long-range order occurs as a result of this transition. The correlation function in ordered state is a product of the power-law XY-universality class type function and the exponential function corresponding to the SU(ν)SU(ν)SU(ν) invariant model. The transition temperature is calculated for the diluted system. It is found that the physical mechanism of the phase transition is changed when ννν exceeds the critical value νc=4ν_c = 4νc​=4. The experimental realization of the considered model is discussed briefly.
The Gutzwiller wave function is shown to be the exact solution of a supersymmetric t-J-type model. The model realizes a Fermi-liquid state in one dimension with a discontinuity in the momentum distribution. Analytic results are obtained for spin and charge susceptibilities, and the specific-heat coefficient with the help of the Luttinger-liquid theory. In the high-density limit the model exhibits a Mott-Hubbard gap and reduces to an antiferromagnetic spin chain with long-range exchange solved by Haldane and Shastry.
The Gutzwiller wave function is shown to be the exact solution of a supersymmetric t-J-type model. The model realizes a Fermi-liquid state in one dimension with a discontinuity in the momentum distribution. Analytic results are obtained for spin and charge susceptibilities, and the specific-heat coefficient with the help of the Luttinger-liquid theory. In the high-density limit the model exhibits a Mott-Hubbard gap and reduces to an antiferromagnetic spin chain with long-range exchange solved by Haldane and Shastry.