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首页> 外文期刊>Communications in Mathematical Physics >Gauge theoretical equivariant Gromov-Witten invariants and the full Seiberg-Witten invariants of ruled surfaces
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Gauge theoretical equivariant Gromov-Witten invariants and the full Seiberg-Witten invariants of ruled surfaces

机译:规的理论等规Gromov-Witten不变量和直纹曲面的完整Seiberg-Witten不变量

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Let F be a differentiable manifold endowed with an almost Kahler structure (J, omega), alpha a J-holomorphic action of a compact Lie group (K) over cap on F, and K a closed normal subgroup of (K) over cap which leaves omega invariant. The purpose of this article is to introduce gauge theoretical invariants for such triples (F, alpha, K). The invariants are associated with moduli spaces of solutions of a certain vortex type equation on a Riemann surface Sigma. Our main results concern the special case of the triple (Hom ((C-r, C-r0), alpha(can), U(r)), where alpha(can) denotes the canonical action of (K) over cap = U(r) x U(r(0)) on Hom(C-r, C-r0). We give a complex geometric interpretation of the corresponding moduli spaces of solutions in terms of gauge theoretical quot spaces, and compute the invariants explicitly in the case r = 1. Proving a comparison theorem for virtual fundamental classes, we show that the full Seiberg-Witten invariants of ruled surfaces, as defined in [OT2], can be identified with certain gauge theoretical Gromov-Witten invariants of the triple (Hom(C, C-r0), alpha(can), U(])). We find the following formula for the full Seiberg-Witten invariant of a ruled surface over a Riemann surface of genus g: SWX,(O1,H0)-sign[c,[f]](c) = 0, SWX,(O1,H0)sign[c, [F]](c) = sign[c, [F]] [Sigma(igreater than or equal tomax(0, g-wc/2))(g) Theta(c)(i)/i! boolean AND l, l(O1)], where [F] denotes the class of a fibre. The computation of the invariants in the general C, case r > 1 should lead to a generalized Vafa-Intriligator formula for "twisted" Gromov-Witten invariants associated with sections in Grassmann bundles. [References: 37]
机译:设F为具有几乎Kahler结构(J,omega)的可微流形,α为F上的紧Lie组(K)的J-全同构作用,K为F上的(K)的闭合正态子组保持欧米茄不变。本文的目的是介绍此类三元组(F,α,K)的规范理论不变量。不变量与Riemann表面Sigma上某个涡旋型方程解的模空间相关。我们的主要结果涉及三元组的特殊情况(Hom((Cr,C-r0),alpha(can),U(r)),其中alpha(can)表示(K)在上限= U(在Hom(Cr,C-r0)上的r)x U(r(0))。我们根据规范的理论空间对溶液的相应模空间进行复杂的几何解释,并在r情况下显式计算不变量= 1.证明了虚拟基本类的比较定理,我们表明,[OT2]中定义的直纹表面的完整Seiberg-Witten不变量可以用三元组的某些规范理论Gromov-Witten不变量(Hom(C ,C-r0),alpha(can),U(]))我们发现以下关于g属Riemann曲面上直纹曲面的Seiberg-Witten不变量的完整公式:SWX,(O1,H0)-sign [c,[f]](c)= 0,SWX,(O1,H0)sign [c,[F]](c)= sign [c,[F]] [Sigma(大于或等于max(0 ,g-wc / 2))(g)Theta(c)(i)/ i!布尔值AND l,l(O1)],其中[F]表示纤维的类别。对于一般C的不变量,如果r> 1,将导致与“格拉斯曼束”中的截面相关的“扭曲” Gromov-Witten不变量的广义Vafa-Intriligator公式。 [参考:37]

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