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A class of P, T-invariant topological phases of interacting electrons

机译:一类相互作用电子的P,T不变拓扑相

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We describe a class of parity- and time-reversal-invariant topological states of matter which can arise in correlated electron systems in 2+1-dimensions. These states are characterized by particle-like excitations exhibiting exotic braiding statistics. P and T invariance are maintained by a 'doubling' of the low-energy degrees of freedom which occurs naturally without doubling the underlying microscopic degrees of freedom. The simplest examples have been the subject of considerable interest as proposed mechanisms for high-T-c superconductivity. One is the 'doubled' version of the chiral spin liquid. The chiral spin liquid gives rise to anyon superconductivity at finite doping and the corresponding field theory is U(1) Chern-Simons theory at coupling constant m = 2. The 'doubled' theory is two copies of this theory, one with m = 2 the other with m = -2. The second example corresponds to Z(2) gauge theory, which describes a scenario for spin-charge separation. Our main concern, with an eye towards applications to quantum computation, are richer models which support non-Abelian statistics. All of these models, richer or poorer, lie in a tightly organized discrete family indexed by the Baraha numbers, 2 cos(pi/ (k + 2)), for positive integer k. The physical inference is that a material manifesting the Z(2) gauge theory or a doubled chiral spin liquid might be easily altered to one capable of universal quantum computation. These phases of matter have a field-theoretic description in terms of gauge theories which, in their infrared limits, are topological field theories. We motivate these gauge theories using a parton model or slave-fermion construction and show how they can be solved exactly. The structure of the resulting Hilbert spaces can be understood in purely combinatorial terms. The highly constrained nature of this combinatorial construction, phrased in the language of the topology of curves on surfaces, lays the groundwork for a strategy for constructing microscopic lattice models which give rise to these phases. (C) 2004 Elsevier Inc. All rights reserved. [References: 96]
机译:我们描述了一类奇偶性和时间反转不变的物质拓扑状态,该状态可能在2 + 1维的相关电子系统中出现。这些状态的特征在于表现出奇异编织统计的类粒子激发。 P和T不变性通过低能量自由度的“加倍”来维持,这自然发生而不会将基础微观自由度加倍。最简单的示例作为高T-c超导性的拟议机制引起了人们的极大兴趣。一种是手性纺丝液的“加倍”版本。手性自旋液体在有限掺杂时会引起任何超导,相应的场论为耦合常数m = 2时的U(1)Chern-Simons理论。“加倍”理论是该理论的两个副本,其中一个m = 2另一个m = -2。第二个示例对应于Z(2)规范理论,该理论描述了自旋电荷分离的方案。我们着眼于量子计算的应用,是支持非阿贝尔统计的更丰富的模型。所有这些模型,无论贫富,都位于一个紧密组织的离散族中,该族由正整数k的Baraha数2 cos(pi /(k + 2))索引。物理推断是,表现出Z(2)规理论的材料或加倍的手性自旋液体可能会容易地更改为能够进行通用量子计算的材料。物质的这些阶段根据规范理论对场论进行了描述,规范理论在其红外范围内是拓扑场论。我们使用parton模型或从属费米子构造激励这些规范理论,并展示如何精确解决它们。所得希尔伯特空间的结构可以用纯粹的组合术语来理解。这种组合构造的高度受约束的性质,用表面上的曲线拓扑的语言来表达,为构建引起这些阶段的微观晶格模型的策略奠定了基础。 (C)2004 Elsevier Inc.保留所有权利。 [参考:96]

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