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A Systematization for One-Loop 4D Feynman Integrals-Different Species of Massive Fields

机译:一环4D Feynman积分不同质场的系统化

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A systematization for the manipulations and calculations involving divergent (or not) Feynman integrals, typical of the one loop perturbative solutions of Quantum Field Theory, is proposed. A previous work on the same issue is generalized to treat theories and models having different species of massive fields. An improvement on the strategy is adopted so that no regularization needs to be used. The final results produced, however, can be converted into the ones of reasonable regularizations, especially those belonging to the dimensional regularization (in situations where the method applies). Through an adequate interpretation of the Feynman rules and a convenient representation for involved propagators, the finite and divergent parts are separated before the introduction of the integration in the loop momentum. Only the finite integrals obtained are in fact integrated. The divergent content of the amplitudes are written as a combination of standard mathematical object which are never really integrated. Only very general scale properties of such objects are used. The finite parts, on the other hand, are written in terms of basic functions conveniently introduced. The scale properties of such functions relate them to a well defined way to the basic divergent objects providing simple and transparent connection between both parts in the assintotic regime. All the arbitrariness involved in this type of calculations are preserved in the intermediary steps allowing the identification of universal properties for the divergent integrals, which are required for the maintenance of fundamental symmetries like translational invariance and scale independence in the perturbative amplitudes. Once these consistency relations are imposed no other symmetry is violated in perturbative calculations neither ambiguous terms survive at any theory or model formulated at any space-time dimension including nonrenormalizable cases. Representative examples of perturbative amplitudes involving different species of massive fermions are considered as examples. The referred amplitudes are calculated in detail within the context of the presented strategy (and systematization) and their relations among other Green functions are explicitly verified. At the end a generalization for the finite functions is presented.
机译:提出了涉及发散(或没有)费曼积分的操纵和计算的系统化,这是量子场论的单环摄动解的典型特征。对于相同问题的先前工作被概括为处理具有不同种类的大范围场的理论和模型。对策略进行了改进,因此不需要使用正则化。但是,可以将产生的最终结果转换为合理的正则化结果,尤其是属于维度正则化的结果(在使用该方法的情况下)。通过对费曼规则的充分解释和对相关传播者的方便表示,在引入回路动量积分之前,将有限部分和发散部分分离。实际上只有获得的有限积分是积分的。振幅的差异内容被写成标准数学对象的组合,但从未真正集成过。仅使用此类对象的非常普通的比例尺属性。另一方面,有限部分是根据方便介绍的基本功能编写的。此类函数的比例属性将它们与基本散布对象的定义明确的方法相关联,从而在缔合状态下的两个部分之间提供简单透明的连接。此类计算中涉及的所有任意性都保留在中间步骤中,从而可以确定发散积分的通用属性,这对于维持基本对称性(例如平移不变性和扰动幅度的尺度独立性)是必需的。一旦强加了这些一致性关系,在扰动计算中就不会破坏任何其他对称性,在任何时空维度上制定的任何理论或模型(包括不可重整的情况)下,模棱两可的术语都不会幸免。涉及不同种类的块状费米子的摄动振幅的代表性示例被认为是示例。在所提出的策略(和系统化)的上下文中详细计算了参考振幅,并明确验证了它们在其他Green函数之间的关系。最后给出了有限函数的一般化。

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