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The Landau-Lifshitz equation describes the Ising spin correlation function in the free-fermion model

机译:Landau-Lifshitz方程描述了自由费米子模型中的Ising自旋相关函数

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We consider time and space dependence of the Ising spin correlation function in a continuous one-dimensional free-fermion model. By the Ising spin we imply the 'sign' variable, which rakes alternating fl values in adjacent domains bounded by domain walls (fermionic world paths). The two-point correlation function is expressed in terms of the solution of the Cauchy problem for a nonlinear partial differential equation, which is proved to be equivalent to the exactly solvable Landau-Lifshitz equation. A new zero-curvature representation for this equation is presented. In turn, the initial condition for the Cauchy problem is given by the solution of a nonlinear ordinary differential equation, which has also been derived. In the Ising limit the above-mentioned partial and ordinary differential equations reduce to the sine-Gordon and Painleve III equations, respectively. [References: 21]
机译:我们考虑连续一维自由费米子模型中Ising自旋相关函数的时间和空间依赖性。通过Ising自旋,我们隐含了'sign'变量,该变量在以畴壁为边界的相邻畴(铁离子世界路径)中产生交替的fl值。两点相关函数用非线性偏微分方程的柯西问题的解表示,事实证明它等效于可精确求解的Landau-Lifshitz方程。给出了该方程的新的零曲率表示。反过来,柯西问题的初始条件由非线性常微分方程的解给出,该方程也已经导出。在Ising极限中,上述偏微分方程和常微分方程分别简化为正弦Gordon和Painleve III方程。 [参考:21]

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