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Geometry of W-algebras from the affine Lie algebra point of view

机译:从仿射李代数的角度看W代数的几何

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摘要

To classify the classical field theories with W-symmetry one has to classify the symplectic leaves of the corresponding W-algebra, which are the intersection of the defining constraint and the coadjoint orbit of the affine Lie algebra if the W-algebra in question is obtained by reducing a Wess-Zumino-Novikov-Witten (WZNW) model. The fields that survive the reduction will obey nonlinear Poisson bracket (or commutator) relations in general. For example, the Toda models are well known theories which possess such a nonlinear W-symmetry and many features of these models can only be understood if one investigates the reduction procedure. In this paper we analyse the SL(n, R) case from which the so-called W-n-algebras can be obtained. One advantage of the reduction viewpoint is that it gives a constructive way to classify the symplectic leaves of the W-algebra-for the n = 2 case corresponding to the coadjoint orbits of the Virasoro algebra and for the n = 3 case which gives rise to the Zamolodchikov algebra. Our method, in principle, is capable of constructing explicit representatives on each leaf. Another attractive feature of this approach is the fact that the global nature of the W-transformations can be explicitly described. The reduction method also enables one to determine the classical highest-weight (HW) states which are the stable minima of the energy on a W-leaf. These are important as only to those leaves can a HW representation space of the W-algebra be associated which contains a classical HW state. [References: 31]
机译:为了用W对称性对经典场理论进行分类,必须对相应W代数的辛叶进行分类,如果获得了W代数,则它们是定义约束与仿射李代数的共共轨道的交点。通过减少Wess-Zumino-Novikov-Witten(WZNW)模型。在还原中幸存的场通常将服从非线性泊松括号(或换向器)关系。例如,Toda模型是众所周知的理论,它具有这种非线性W对称性,并且只有在研究还原过程的情况下才能理解这些模型的许多特征。在本文中,我们分析了SL(n,R)的情况,从中可以得到所谓的W-n代数。归约观点的一个优点是,它为构造W代数的辛叶提供了一种构造性的方法-对于n = 2的情况对应于Virasoro代数的共伴随轨道,而对于n = 3的情况则产生W Zamolodchikov代数。原则上,我们的方法能够在每个叶子上构造明确的代表。这种方法的另一个吸引人的特点是可以明确描述W变换的全局性质。减少方法还使人们能够确定经典的最大重量(HW)状态,这是W叶上能量的稳定最小值。这些很重要,因为仅对于那些叶子,W代数的HW表示空间才能被关联,其中包含经典的HW状态。 [参考:31]

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