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When examining a field theory in a general state, the propagator must be made consistent with that state and new counterterms are allowed if the state breaks some of the space-time’s symmetries. This talk describes the specific example of how the propagator for the alpha-vacua of de Sitter space must become the Green’s function for two antipodal sources to obtain a renormalizable theory.

生成讲解博客的中文版本

生成AI智能校验的中文版本