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arXiv 1502.00557hep-thmath-phmath.MPmath.NT
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亏格为2的镜像曲线的直接积分与几乎亚纯Siegel模形

Direct Integration for Mirror Curves of Genus Two and an Almost Meromorphic Siegel Modular Form

Albrecht Klemm, Maximilian Poretschkin, Thorsten Schimannek, Martin Westerholt-Raum

摘要:

这项工作认为方面的几乎全纯和亚纯西格尔模形式从物理和数学的角度。第一部分是关于(精化的)拓扑弦论和全纯反常方程的直接积分。在这里,一个中心的对象来计算更高的属振幅,作为各种枚举不变量的生成函数,是由所谓的传播。我们推导出一个普遍的表达式的几何形状,具有镜像曲线的亏格2,这是由衍生物的对数Igusa的尖点形式的重量10的传播。此外,我们通过求解三阶、五阶和六阶复曲面轨道的分辨率上的精细拓扑弦来说明我们的发现。在第二部分中,我们给出了Siegel模形式上的降算子和升算子的显式表达式,并在此基础上定义了几乎全纯Siegel模形式。将傅里叶-雅可比展开理论推广到几乎全纯的西格尔模形式,并建立在Pitale、Saha和Schmidt最近的工作基础上,我们可以证明几乎全纯的椭圆第二爱森斯坦级数没有类似物。在亏格2的情况下,我们给出了一个几乎亚纯的替代,特别是,这使我们得到了第二Eisenstein级数的Ramanujan微分方程的推广。这两个部分是交织在一起的观察,亚纯模拟的几乎全纯的第二爱森斯坦系列符合物理传播。此外,广义拉马努金身份匹配的物理一致性条件,需要施加在传播。

英文摘要:

This work considers aspects of almost holomorphic and meromorphic Siegel modular forms from the perspective of physics and mathematics. The first part is concerned with (refined) topological string theory and the direct integration of the holomorphic anomaly equations. Here, a central object to compute higher genus amplitudes, which serve as the generating functions of various enumerative invariants, is provided by the so-called propagator. We derive a universal expression for the propagator for geometries that have mirror curves of genus two which is given by the derivative of the logarithm of Igusa's cusp form of weight 10. In addition, we illustrate our findings by solving the refined topological string on the resolutions of the three toric orbifolds of order three, five and six. In the second part, we give explicit expressions for lowering and raising operators on Siegel modular forms, and define almost holomorphic Siegel modular forms based on them. Extending the theory of Fourier-Jacobi expansions to almost holomorphic Siegel modular forms and building up on recent work by Pitale, Saha, and Schmidt, we can show that there is no analogue of the almost holomorphic elliptic second Eisenstein series. In the case of genus 2, we provide an almost meromorphic substitute for it. This, in particular, leads us to a generalization of Ramanujan's differential equation for the second Eisenstein series. The two parts are intertwined by the observation that the meromorphic analogue of the almost holomorphic second Eisenstein series coincides with the physical propagator. In addition, the generalized Ramanujan identities match precisely the physical consistency conditions that need to be imposed on the propagator.

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