paper

Absorbing Boundary Condition as Limiting Case of Imaginary Potentials

arXiv:1911.12730 · doi:10.1088/1572-9494/ac9bea

Abstract

Imaginary potentials such as (with a constant, a subset of 3-space, and its characteristic function) have been used in quantum mechanics as models of a detector. They represent the effect of a "soft" detector that takes a while to notice a particle in the detector volume . In order to model a "hard" detector (i.e., one that registers a particle as soon as it enters ), one may think of taking the limit of increasing detector strength . However, as pointed out by Allcock, in this limit the particle never enters ; its wave function gets reflected at the boundary of in the same way as by a Dirichlet boundary condition on . This phenomenon, a cousin of the "quantum Zeno effect," might suggest that a hard detector is mathematically impossible. Nevertheless, a mathematical description of a hard detector has recently been put forward in the form of the "absorbing boundary rule" involving an absorbing boundary condition on the detecting surface . We show here that in a suitable (non-obvious) limit, the imaginary potential yields a non-trivial distribution of detection time and place in agreement with the absorbing boundary rule. That is, a hard detector can be obtained as a limit, but it is a different limit than Allcock considered.

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