Scattering Cross Section Formula Derived From Macroscopic Model of Detectors
arXiv:2601.01625 · doi:10.1088/1751-8121/ae880a
Abstract
We are concerned with the justification of the statement, commonly (explicitly or implicitly) used in quantum scattering theory, that for a free non-relativistic quantum particle with initial wave function , surrounded by detectors along a sphere of large radius , the probability distribution of the detection time and place has asymptotic density (i.e., scattering cross section) with the Fourier transform of . We give two derivations of this formula, based on different macroscopic models of the detection process. The first one consists of a negative imaginary potential of strength in the detector volume (i.e., outside the sphere of radius ) in the limit . The second one consists of repeated nearly-projective measurements of (approximately) the observable at times in the limit ; this setup is similar to that of the quantum Zeno effect, except that there one considers instead of . We also provide a comparison to Bohmian mechanics: while in the absence of detectors, the arrival times and places of the Bohmian trajectories on the sphere of radius have asymptotic distribution density given by the same formula as , their deviation from the detection times and places is not necessarily small, although it is small compared to , so the effect of the presence of detectors on the particle can be neglected in the far-field regime. We also cover the generalization to surfaces with non-spherical shape, to the case of non-interacting particles, to time-dependent surfaces, and to the Dirac equation.
40 pages LaTeX, 4 figures; v3 minor additions and improvements