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Consider the Plancherel decomposition of the tensor product of a highest weight and a lowest weight unitary representations of . We construct explicitly the action of the Lie algebra in the direct integral of Hilbert spaces. It turns out that a Lie algebra operator is a second order differential operator in one variable and second order difference operator with respect to another variable. The difference operators are defined in terms of the shift in the imaginary direction $f(s)\mapsto f(s+i)i^2=-1s$).

生成讲解博客的中文版本

生成AI智能校验的中文版本