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Instabilities in a binary mixture of one-dimensional quantum fluids

Miguel A. Cazalilla, Andrew Fu Wah Ho

Published Mar 26, 2003• 0 citations
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A first-principles theory for the description of critical phenomena in mixtures is presented. This is a natural extension of the hierarchical reference theory of fluids, which has proven useful and accurate in the treatment of the critical region of one-component fluids. The case of a binary mixture is studied in detail. Near the critical point, the theory develops a renormalization-group structure that allows the identification of several possible critical behaviors corresponding to different fixed points. For a generic binary mixture, the most stable fixed point gives rise to the same critical exponents as are predicted by the well-known phenomenological approach, providing a microscopic mechanism for such behavior. The competition between two fixed points is identified as the mechanism leading to the strong corrections to scaling seen experimentally. Explicit expressions for the most interesting universal quantities are evaluated to O(4-d). This theory is then applied to a few simple models of mixtures in three dimensions. As a first step, the mean-field phase diagram is reproduced and the stability of this solution is determined. The physical nature of the relevant order parameter and the one-loop correction to mean-field results are also calculated within our approach.

Physical Review A•Nov 1, 1991•40 citations
We show that one-dimensional binary mixtures of bosons or of a boson and a spin-polarized fermion are Luttinger liquids with the following instabilities: (i) For different particle densities, strong attraction between the mixture components leads to collapse, while strong repulsion leads to demixing, and (ii) For a low-density mixture of two gases of impenetrable bosons (or a spin-polarized fermion and an impenetrable boson) of equal densities, the system develops a gap and exhibits enhanced pairing fluctuations when there is attraction between the components. In the boson-fermion mixture, the pairing fluctuations occur at finite momentum. Our conclusions apply to mixtures both on the continuum and on optical lattices away from integer or fractional commensurability.
We present a systematic investigation of attractive binary mixtures in the presence of both spin- and mass-imbalance in one-dimensional setups described by the Hubbard model. After discussing typical cold atomic experimental realizations and the relation between microscopic and effective parameters, we study several many-body features of trapped Fermi-Fermi and Bose-Bose mixtures such as density profiles, momentum distributions, and correlation functions by means of density-matrix-renormalization-group and quantum Monte Carlo simulations. In particular, we focus on the stability of Fulde-Ferrell-Larkin-Ovchinnikov, dimer, and trimer fluids in inhomogeneous situations, as typically realized in cold gas experiments due to the harmonic confinement. We finally consider possible experimental signatures of these phases both in the presence of a finite polarization and of a finite temperature.
A first-principles theory for the description of critical phenomena in mixtures is presented. This is a natural extension of the hierarchical reference theory of fluids, which has proven useful and accurate in the treatment of the critical region of one-component fluids. The case of a binary mixture is studied in detail. Near the critical point, the theory develops a renormalization-group structure that allows the identification of several possible critical behaviors corresponding to different fixed points. For a generic binary mixture, the most stable fixed point gives rise to the same critical exponents as are predicted by the well-known phenomenological approach, providing a microscopic mechanism for such behavior. The competition between two fixed points is identified as the mechanism leading to the strong corrections to scaling seen experimentally. Explicit expressions for the most interesting universal quantities are evaluated to O(4-d). This theory is then applied to a few simple models of mixtures in three dimensions. As a first step, the mean-field phase diagram is reproduced and the stability of this solution is determined. The physical nature of the relevant order parameter and the one-loop correction to mean-field results are also calculated within our approach.