
doi: 10.1007/bf02726388
The phase factors which can appear in the definition of the inversions,C, P, T and their products are discussed. It is shown that because of the existence of « physically equivalent » Hamiltonians, the phases inC, CP, T andTP for complex fields are unmeasurable. For the remaining inversions, it is possible to construct interactions which require more general phases for complex fields than the usual ±1, ±i, when and only when the theory contains certain discrete multiplicative symmetries. Examples of such interactions are given.
quantum theory
quantum theory
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