Reflecting an interval repeatedly across its endpoints maps a reflected path to a free path in an image interval. A return trajectory from ends at after an even number of wall reflections, or after an odd number. An infinite square well has reflection amplitude , so the corresponding Dirichlet heat kernel on an interval is the difference of direct and mirrored free kernels. Individual straight paths illustrate the geometry; the path integral sums all time-sliced paths with the same endpoints.
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