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A particle in a one-dimensional {δ}-function potential possesses both discrete and continuum solutions. The configuration-space Green's function and propagator for this problem are derived by explicit summation over the spectrum of eigenstates. The momentum-space Green's function is also obtained. The propagator does not contain the classical action function in any simple way, in contrast to the usual structure in Feynman's path-integral formalism. Various analogies between the {δ}-function and Coulomb problems are discussed.
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S. M. Blinder (1988) studied this question.
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