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超几何中的等变上同调与局部化公式

Equivariant Cohomology and Localization Formula in Supergeometry

Pascal Lavaud

摘要:

设G是紧李群.设M是光滑G-流形,V --> M是定向G-等变向量丛.定义了V和M上具有广义系数的等变形式空间。V上的等变Thom形式$θ$是紧支撑的闭等变形式,使得它沿纤维的积分是M上的常数函数1。这种Thom形式是由Mathai和Quillen构建的。它的限制M给出了一个代表的等变欧拉类的V.在超几何的情况下,我们给适当的定义所涉及的所有对象。但是,在这种情况下,Thom形式并不总是存在的。在本文中,当G在V上的作用充分非平凡时,我们构造了这样一个具有广义系数的Thom形式。我们用它来构造V的一个等变Euler形式,并将Berline-Vergne的局部化公式推广到超几何情形。

英文摘要:

Let G be a compact Lie group. Let M be a smooth G-manifold and V --> M be an oriented G-equivariant vector bundle. One defines the spaces of equivariant forms with generalized coefficients on V and M. An equivariant Thom form $θ$ on V is a compactly supported closed equivariant form such that its integral along the fibres is the constant function 1 on M. Such a Thom form was constructed by Mathai and Quillen. Its restriction to M gives a representative of the equivariant Euler class of V. In the supergeometric situation we give proper definitions of all the objects involved. But, in this case a Thom form doesn't always exist. In this article, when the action of G on V is sufficiently non-trivial, we construct such a Thom form with generalized coefficients. We use it to construct an equivariant Euler form of V and to generalize Berline-Vergne's localization formula to the supergeometric situation.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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