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Scalar 1-loop Feynman integrals as meromorphic functions in space-time dimension d

机译:标量一环Feynman积分为时空维度 d 的亚纯函数

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The long-standing problem of representing the general massive one-loop Feynman integral as a meromorphic function of the space-time dimensiondhas been solved for the basis of scalar one- to four-point functions with indices one. In 2003 the solution of difference equations in the space-time dimension allowed to determine the necessary classes of special functions: self-energies need ordinary logarithms and Gauss hypergeometric functionsF12, vertices need additionally Kampé de Fériet-Appell functionsF1, and box integrals also Lauricella-Saran functionsFS. In this study, alternative recursive Mellin-Barnes representations are used for the representation ofn-point functions in terms of(n?1)-point functions. The approach enabled the first derivation of explicit solutions for the Feynman integrals at arbitrary kinematics. In this article, we scetch our new representations for the general massive vertex and box Feynman integrals and derive a numerical approach for the necessary Appell functionsF1and Saran functionsFSat arbitrary kinematical arguments.
机译:在标量为一的标量一到四点函数的基础上,解决了将大质量单环费曼积分表示为时空维的亚纯函数的长期存在的问题。在2003年,时空维差分方程的解决方案可以确定必要的特殊函数类别:自能量需要普通对数和高斯超几何函数F12,顶点还需要KampédeFériet-Appell函数F1,而盒积分也需要Lauricella-萨兰函数FS。在这项研究中,将交替递归的Mellin-Barnes表示用于表示(n?1)点函数。该方法可以在任意运动学上首次推导Feynman积分的显式解。在本文中,我们提取了一般的整体顶点和Box Feynman积分的新表示形式,并为任意运动学参数上的必要Appell函数F1和Saran函数FS导出了一种数值方法。

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