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arXiv 1005.0153math-phgr-qcmath.MPnlin.SI
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对称轨道的递推与不约化约化

Recursions of Symmetry Orbits and Reduction without Reduction

Andrei A. Malykh, Mikhail B. Sheftel

摘要:

本文主要以复Monge-Ampère方程(CMA)为例,研究了具有伙伴对称性的四维偏微分方程.我们同时使用两对相关的递归关系的对称性,这是相互复杂的共轭CMA。对于这两对合作伙伴的对称性,使用李方程,我们明确地引入组参数作为额外的变量,取代对称性特征和它们的复杂共轭的衍生物的未知的组参数。我们研究了八维空间中的六个方程组,其中包括CMA,四个伙伴对称之间的递归方程和这个系统的一个可积条件。我们使用这个扩展系统的点对称性进行其对称性减少相对于组参数,有利于解决扩展系统。这个过程并不意味着减少物理变量的数量,因此,我们最终与CMA的非不变解的轨道,产生的一个合作伙伴的对称性,不使用的减少。这些解决方案是由六个常系数的线性方程组在五维空间,这是通过三维勒让德变换的减少扩展系统。我们提出了代数和指数的例子,这样的解决方案,治理勒让德变换的Ricci平坦的Kähler度量没有Killing向量。对Husain方程也作了类似的处理。

英文摘要:

We consider a four-dimensional PDE possessing partner symmetries mainly on the example of complex Monge-Ampère equation (CMA). We use simultaneously two pairs of symmetries related by a recursion relation, which are mutually complex conjugate for CMA. For both pairs of partner symmetries, using Lie equations, we introduce explicitly group parameters as additional variables, replacing symmetry characteristics and their complex conjugates by derivatives of the unknown with respect to group parameters. We study the resulting system of six equations in the eight-dimensional space, that includes CMA, four equations of the recursion between partner symmetries and one integrability condition of this system. We use point symmetries of this extended system for performing its symmetry reduction with respect to group parameters that facilitates solving the extended system. This procedure does not imply a reduction in the number of physical variables and hence we end up with orbits of non-invariant solutions of CMA, generated by one partner symmetry, not used in the reduction. These solutions are determined by six linear equations with constant coefficients in the five-dimensional space which are obtained by a three-dimensional Legendre transformation of the reduced extended system. We present algebraic and exponential examples of such solutions that govern Legendre-transformed Ricci-flat Kähler metrics with no Killing vectors. A similar procedure is briefly outlined for Husain equation.

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