Stability of a spin-triplet nematic state near to a quantum critical point

被引:1
|
作者
Hannappel, G. [1 ]
Pedder, C. J. [1 ,2 ]
Krueger, F. [1 ,3 ]
Green, A. G. [1 ]
机构
[1] UCL, London Ctr Nanotechnol, Gordon St, London WC1H 0AH, England
[2] Univ Luxembourg, Phys & Mat Sci Res Unit, L-1511 Luxembourg, Luxembourg
[3] Rutherford Appleton Lab, ISIS Facil, Didcot OX11 0QX, Oxon, England
基金
英国工程与自然科学研究理事会;
关键词
ELECTRONIC-STRUCTURE; PHASE-TRANSITIONS; FERMI-LIQUID; SUPERCONDUCTIVITY; DISORDER; ORDER; FERROMAGNETISM; WAVE;
D O I
10.1103/PhysRevB.93.235105
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We analyze a model of itinerant electrons interacting through a quadrupole density-density repulsion in three dimensions. At the mean-field level, the interaction drives a continuous Pomeranchuk instability towards d-wave, spin-triplet nematic order, which simultaneously breaks the SU(2) spin-rotation and spatial-rotation symmetries. This order is characterized by spin-antisymmetric, elliptical deformations of the Fermi surfaces of up and down spins. We show that the effects of quantum fluctuations are similar to those in metallic ferromagnets, rendering the nematic transition first order at low temperatures. Using the fermionic quantum order-by-disorder approach to self-consistently calculate fluctuations around possible modulated states, we show that the first-order transition is preempted by the formation of a helical spin-triplet d-density wave. Such a state is closely related to d-wave bond density wave order in square-lattice systems. Moreover, we show that it may coexist with a modulated, p-wave superconducting state.
引用
收藏
页数:15
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