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Discrete symmetries and the propagator approach to coupled fermions in Quantum Field Theory. Generalities: The case of a single fermion-antifermion pair

机译:量子场论中耦合费米子的离散对称性和传播子方法。普遍性:单对费米子-抗蚁体的情况

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Starting from Wigner's symmetry representation theorem, we give a general account of discrete symmetries (parity P, charge conjugation C, time-reversal T), focusing on fermions in Quantum Field Theory. We provide the rules of transformation of Weyl spinors, both at the classical level (grassmanian wave functions) and quantum level (operators). Making use of Wightman's definition of invariance, we outline ambiguities linked to the notion of classical fermionic Lagrangian. We then present the general constraints cast by these transformations and their products on the propagator of the simplest among coupled fermionic system, the one made with one fermion and its antifermion. Last, we put in correspondence the propagation of C eigenstates (Majorana fermions) and the criteria cast on their propagator by C and CP invariance.
机译:从维格纳的对称表示定理开始,我们给出了离散对称性(奇偶性P,电荷共轭C,时间反转T)的一般解释,重点是量子场论中的费米子。我们提供了经典水平(格拉斯曼波函数)和量子水平(算子)的Weyl旋转子的变换规则。利用Wightman不变性的定义,我们概述了与经典费米拉格朗日方程有关的歧义。然后,我们介绍了这些转换及其产物对耦合费米子系统中最简单的繁殖器(由一个费米子及其反费米子制造)所产生的一般约束。最后,我们将C本征态(马约拉那费米子)的传播与通过C和CP不变性在其传播子上施加的条件对应起来。

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