We study the second quantized -or guiding center- description of the torusLaughlin state. Our main focus is the change of the guiding center degrees offreedom with the torus geometry, which we show to be generated by a two-bodyoperator. We demonstrate that this operator can be used to evolve the fulltorus Laughlin state at given modular parameter \tau\ from its simple(Slater-determinant) thin torus limit, thus giving rise to a new presentationof the torus Laughlin state in terms of its "root partition" and an exponentialof a two-body operator. This operator therefore generates in particular theadiabatic evolution between Laughlin states on regular tori and thequasi-one-dimensional thin torus limit. We make contact with the recentlyintroduced notion of a "Hall viscosity" for fractional quantum Hall states, towhich our two-body operator is naturally related, and which serves as ademonstration of our method to generate the Laughlin state on the torus.
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机译:我们研究了torusLaughlin状态的第二个量化或指导中心描述。我们的主要焦点是导向中心自由度随环面几何形状的变化,我们证明这是由两体操作者产生的。我们证明了该算子可用于在给定的模块化参数\ tau \下从其简单的(Slater-determinant)薄圆环极限演化出Fulltorus Laughlin状态,从而根据其“根”产生了新的圆环Laughlin状态表示。分区”和两体运算符的指数。因此,该算子尤其在规则花托和准一维薄花托极限上的劳克林状态之间产生绝热演化。我们接触了最近引入的分数量子霍尔态的“霍尔粘度”概念,该概念与我们的二体算子自然相关,并且证明了我们在圆环上生成Laughlin态的方法。
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