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Rindler's acceleration-induced partitioning of spacetime leads to anature-given interferometer. It accomodates quantum mechanical and wavemechanical processes in spacetime which in (Euclidean) optics correspond towave processes in a ``Mach-Zehnder'' interferometer: amplitude splitting,reflection, and interference. These processes are described in terms ofamplitudes which behave smoothly across the event horizons of all four Rindlersectors. In this context there arises quite naturally a complete set oforthonormal wave packet histories, one of whose key properties is their"explosivity index". In the limit of low index values the wave packets traceout fuzzy world lines. By contrast, in the asymptotic limit of high indexvalues, there are no world lines, not even fuzzy ones. Instead, the wave packethistories are those of entities with non-trivial internal collapse andexplosion dynamics. Their details are described by the wave processes in theabove-mentioned Mach-Zehnder interferometer. Each one of them is a double slitinterference process. These wave processes are applied to elucidate theamplification of waves in an accelerated inhomogeneous dielectric. Alsodiscussed are the properties and relationships among the transition amplitudesof an accelerated finite-time detector.

Paired accelerated frames: The perfect interferometer with everywhere smooth wave amplitudes