Phase separation in strongly coupled binary ionic mixtures at zero temperature

1983 ◽  
Vol 119 (3) ◽  
pp. 527-552
Author(s):  
R. Mazighi
2011 ◽  
Vol 26 (26) ◽  
pp. 4617-4631 ◽  
Author(s):  
SANG-JIN SIN ◽  
SHAN-SHAN XU ◽  
YANG ZHOU

We consider the gravity dual of strongly coupled system at a Lifshitz-fixed point and finite temperature, which was constructed in a recent work arXiv:0909.0263. We construct an Abelian–Higgs model in that background and calculate condensation and conductivity using holographic techniques. We find that condensation happens and DC conductivity blows up when temperature turns below a critical value. We also study the zero temperature limit of strongly coupled system at the Lifshitz-fixed point.


2002 ◽  
Vol 12 (9) ◽  
pp. 337-341
Author(s):  
B. Spivak

We show that the existence of an intermediate phase between the Fermi liquid and the Wigner crystal phases is a generic property of the two-dimensional pure electron liquid in MOSFET's at zero temperature. The physical reason for the existence of the phases is a partial separation of the uniform phases. We discuss properties of these phases and a possible explanation of experimental results on transport properties of low density electron gas in MOSFET's. We also argue that in certain range of parameters the partial phase separation corresponds to a supersolid phase discussed in [25].


1990 ◽  
Vol 8 (4) ◽  
pp. 781-791
Author(s):  
D. Léger ◽  
C. Deutsch

This paper is devoted to a systematic investigation of linear transport properties in strongly coupled binary ionic mixtures of pointlike ions interacting solely through Coulomb interactions. The basic formalism rests upon suitable extensions of the Boltzmann–Ziman equation explained in this work. Validity conditions for the Lorentzian approximation are thoroughly discussed as well as entropy arguments. High temperature inelastic contributions are emphasized out.


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