Limitations of the paraxial beam model in the study of quantum vacuum signals
arXiv:2503.04368 · doi:10.1103/bmxl-776l
Abstract
Studies of nonlinear quantum vacuum signals often model the driving laser fields as paraxial beams. This in particular holds for analytic approaches. While this allows for reliable predictions in most situations, there are also notable exceptions. A prominent example is the overestimation of the polarization-flipped signal photon yield in the collision of two equally focused, parallel polarized laser beams by a factor of about six. In the present work, we identify the origin of this deficiency and devise a strategy to obtain accurate closed-form expressions also in cases challenging the conventional (leading order) paraxial beam model. We demonstrate the potential of our approach on the example of two linearly polarized laser pulses colliding at a generic collision angle.
arXiv comment9 pages, 3 figures; v3: units added in tab. 1
References in corpus (16)
- Extremely high-intensity laser interactions with fundamental quantum systems
- Advances in QED with intense background fields
- Light diffraction by a strong standing electromagnetic wave
- Measuring Vacuum Polarisation with High Power Lasers
- Photon-photon scattering in collisions of laser pulses
- Stimulated photon emission from the vacuum
- Light by light diffraction in vacuum
- Probing vacuum polarization effects with high-intensity lasers
- All-optical signatures of Strong-Field QED in the vacuum emission picture
- Three-pulse photon-photon scattering
- All-optical signatures of quantum vacuum nonlinearities in generic laser fields
- Vacuum birefringence in the head-on collision of XFEL and optical high-intensity laser pulses
- The photon polarization tensor in pulsed Hermite- and Laguerre-Gaussian beams
- Vacuum birefringence at x-ray free-electron lasers
- Vacuum birefringence and diffraction at XFEL: from analytical estimates to optimal parameters
- Numerical Simulations of the Nonlinear Quantum Vacuum in the Heisenberg-Euler Weak-Field Expansion