Lifshitz transitions and crystallization of fully polarized dipolar fermions in an anisotropic two-dimensional lattice

被引:20
作者
Carr, Sam T. [1 ,2 ]
Quintanilla, Jorge [3 ,4 ]
Betouras, Joseph J. [5 ]
机构
[1] Karlsruher Inst Technol, Inst Theorie Kondensierten Mat, D-76128 Karlsruhe, Germany
[2] Karlsruher Inst Technol, DFG Ctr Funct Nanostruct, D-76128 Karlsruhe, Germany
[3] Univ Kent, Sch Phys Sci, Canterbury CT2 7NH, Kent, England
[4] STFC Rutherford Appleton Lab, ISIS Spallat Facil, Didcot OX11 0QX, Oxon, England
[5] Loughborough Univ Technol, Dept Phys, Loughborough LE11 3TU, Leics, England
来源
PHYSICAL REVIEW B | 2010年 / 82卷 / 04期
基金
英国工程与自然科学研究理事会;
关键词
PHASE-TRANSITION; POMERANCHUK INSTABILITY; QUANTUM CRITICALITY; RUTHENATE SR3RU2O7; LUTTINGER LIQUIDS; METALLIC SYSTEMS; OPTICAL LATTICES; HUBBARD-MODEL; GAS; CROSSOVER;
D O I
10.1103/PhysRevB.82.045110
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We consider a two-dimensional model of noninteracting chains of spinless fermions weakly coupled via a small interchain hopping and a repulsive interchain interaction. The phase diagram of this model has a surprising feature: an abrupt change in the Fermi surface as the interaction is increased. We study in detail this metanematic transition and show that the well-known 21/2-order Lifshitz transition is the critical end point of this first-order quantum phase transition. Furthermore, in the vicinity of the end point, the order parameter has a nonperturbative BCS-type form. We also study a competing crystallization transition in this model and derive the full phase diagram. This physics can be demonstrated experimentally in dipolar ultracold atomic or molecular gases. In the presence of a harmonic trap, it manifests itself as a sharp jump in the density profile.
引用
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页数:13
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