The photon polarization tensor in pulsed Hermite- and Laguerre-Gaussian beams
arXiv:1711.06151 · doi:10.1103/PhysRevD.96.116004
Abstract
In this article, we provide analytical expressions for the photon polarization tensor in pulsed Hermite- and Laguerre-Gaussian laser beams. Our results are based on a locally constant field approximation of the one-loop Heisenberg-Euler effective Lagrangian for quantum electrodynamics. Hence, by construction they are limited to slowly varying electromagnetic fields, varying on spatial and temporal scales significantly larger than the Compton wavelength/time of the electron. The latter criterion is fulfilled by all laser beams currently available in the laboratory. Our findings will, e.g., be relevant for the study of vacuum birefringence experienced by probe photons brought into collision with a high-intensity laser pulse which can be represented as a superposition of either Hermite- or Laguerre-Gaussian modes.
18 pages, 1 figure
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Cited by in corpus (14)
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- Vacuum birefringence and diffraction at XFEL: from analytical estimates to optimal parameters
- Reducible contributions to quantum electrodynamics in external fields
- Vacuum birefringence at the Gamma Factory
- Quantum vacuum signatures in multi-color laser pulse collisions
- QED vacuum nonlinearity in Laguerre-Gauss beams
- All-optical Quantum Vacuum Signals in Two-Beam Collision
- Fundamental constants from photon-photon scattering in three-beam collisions
- Two-beam laser photon merging
- The Vacuum Emission Picture Beyond Paraxial Approximation
- Limitations of the paraxial beam model in the study of quantum vacuum signals