Strong coupling of virtual negative states in the Kapitza-Dirac effect
arXiv:2601.07157 · doi:10.1103/nlzn-11yf
Abstract
Negative states are an intrinsic property of relativistic quantum theory and related to anti-particles in the context of the Dirac sea concept. We show that negative states can dominantly contribute to the diffraction amplitude in the quantum dynamics of the two-photon Kapitza-Dirac effect. We draw our conclusion by investigating solutions from time-dependent perturbation theory, where the perturbative solutions are in match with numeric solutions of the relativistic quantum system and also with the numeric and analytic solutions from the relativistic equations of motion of a classical point-like electron in an external standing wave light field. While our numeric solutions assume a strong laser field, the analytic solutions indicate that negative state coupling remains dominant for arbitrary low field amplitudes, where in the single-photon case (Compton scattering) negative state coupling can be mathematically associated with the interaction of a virtual electron-positron pair in the context of a quantized theory in old-fashioned perturbation theory.
14 pages, 5 figures
References in corpus (12)
- Relativistic ponderomotive force, uphill acceleration, and transition to chaos
- Spin dynamics in the Kapitza-Dirac effect
- The Kapitza - Dirac effect
- Spin-polarizing interferometric beam splitter for free electrons
- Kapitza-Dirac effect in the relativistic regime
- Polarization-dependent ponderomotive gradient force in a standing wave
- Spin effects in Kapitza-Dirac scattering at light with elliptical polarization
- Spin-dependent two-color Kapitza-Dirac effects
- Electron spin filter and polarizer in a standing light wave
- Spin dynamics in Kapitza-Dirac scattering of electrons from bichromatic laser fields
- Spin-dependent two-photon Bragg scattering in the Kapitza-Dirac effect
- Beam focus and longitudinal polarization influence on spin dynamics in the Kapitza-Dirac effect