Time- and space-resolved selective multi-pair creation
arXiv:1707.08450 · doi:10.1103/PhysRevD.96.056017
Abstract
The simultaneous creation of multiple electron-positron pairs by localized strong electric fields is studied by utilizing a time- and space-resolved quantum field theory approach. It is demonstrated that the number of simultaneously created pairs equals the number of the potential's supercritical quasibound states in the Dirac sea. This means it can be controlled by tuning the potential parameters. Furthermore, the energy of the created particles corresponds to the energy of the supercritical quasibound states. The simultaneously created electrons and positrons are statistically correlated, which is reflected in the spatial distribution and the momentum distribution of these particles and antiparticles.
References in corpus (9)
- Extremely high-intensity laser interactions with fundamental quantum systems
- Control of quantum phenomena: Past, present, and future
- Dynamically assisted Schwinger mechanism
- Multiple colliding electromagnetic pulses: a way to lower the threshold of pair production from vacuum
- Pair production in laser fields oscillating in space and time
- Resonantly enhanced pair production in a simple diatomic model
- Spin polarized electron-positron pair production via elliptical polarized laser fields
- Multi-pair states in electron-positron pair creation
- Bosonic pair creation and the Schiff-Snyder-Weinberg effect
Cited by in corpus (6)
- On the effect of time-dependent inhomogeneous magnetic fields on the particle momentum spectrum in electron-positron pair production
- Enhancement of pair creation due to locality in bound-continuum interactions
- Space-time resolved quantum field approach to Klein tunneling dynamics across a finite barrier
- Beam focus and longitudinal polarization influence on spin dynamics in the Kapitza-Dirac effect
- State of a particle pair produced by the Schwinger effect is not necessarily a maximally entangled Bell state
- Evolution of strictly localized states in non-interacting quantum field theories with background fields