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Magnetars as Laboratories for Strong Field QED

Published 5 Dec 2021 in astro-ph.HE and hep-ph | (2112.02460v1)

Abstract: A strong electromagnetic field polarizes the vacuum and in the presence of an electric field creates pairs of a charged particle and its anti-particle. Magnetars, highly magnetized neutron stars with magnetic field comparable to or greater than the Schwinger field, give a significant amount of the vacuum polarization and vacuum birefringence and the induced electric field can create the electron-positron pairs, which are strong field quantum electrodynamics (QED) processes. In this paper, we use a closed formula for the one-loop effective action in the presence of a supercritical magnetic field and a subcritical electric field, find the vacuum birefringence analytically and numerically, and then discuss possible measurements in magnetars.

Summary

  • The paper introduces magnetars as effective natural laboratories that test strong field QED predictions beyond terrestrial capabilities.
  • It employs combined analytical and numerical methods using the Heisenberg-Euler effective action to simulate observable vacuum birefringence and pair production.
  • The findings offer measurable predictions for light polarization effects in extreme astrophysical conditions, guiding future x-ray polarimetry missions.

Magnetars as Laboratories for Strong Field QED

Introduction

This paper presents a comprehensive analysis of magnetars, highly magnetized neutron stars, as natural laboratories for studying strong field quantum electrodynamics (QED). Traditionally, laboratory experiments fail to replicate the extreme electromagnetic field strengths found in astrophysical objects, which exceed the critical fields where nonlinear QED effects become significant. These include vacuum polarization, vacuum birefringence, and electron-positron pair production, processes that can be analytically described by the Heisenberg-Euler and Schwinger effective actions under such conditions. The authors focus on using magnetars to probe these effects, whose magnetic fields surpass the Schwinger limit, providing a unique opportunity to experimentally test strong field QED predictions.

Strong Field QED Phenomena

The core of QED at strong fields lies in the nonlinear response of the vacuum, leading to phenomena such as vacuum birefringence and pair production. The Schwinger effect, significant at electric fields E∼Ec=1.3×1016 V/cmE \sim E_c = 1.3 \times 10^{16}\, {\rm V/cm}, results in prolific electron-positron pair production. Similarly, a critical magnetic field, Bc=4.4×1013 GB_c = 4.4 \times 10^{13}\, {\rm G}, leads to vacuum effects like birefringence. These processes are analytically captured by the Heisenberg-Euler effective action, from which observables in a magnetically charged vacuum can be derived.

Magnetars provide magnetic field strengths greater than BcB_c, yielding observable vacuum birefringence. This occurs due to refractive index changes in the vacuum, leading to polarization-dependent light propagation. This paper employs novel analytical formulations of the QED effective action to address these observations, serving as potent probes of theoretical predictions.

Experimental Implications and Numerical Results

The study provides a detailed exploration of refractive indices for electromagnetic waves propagating through magnetized vacua. With magnetars offering macroscopic scales vastly larger than the Compton wavelength, the Heisenberg-Euler action remains applicable for theoretical predictions. Numerical modeling incorporates both analytic and numerical calculations, allowing simulations of vacuum birefringence observable in high-field environments.

Significant deviation from unity refractive index occurs for both parallel and perpendicular wave polarizations. Particularly, for fields approaching or exceeding BcB_c, the variations become substantial enough to offer observational signatures. The implications extend towards direct measurements of light polarization near neutron stars and magnetars, offering pathways to validate the theoretical models against astrophysical data.

Conclusion

This paper elucidates the role of magnetars in advancing our understanding of strong field QED. By extending laboratory-scale predictions to astrophysical phenomena, it offers a bridge between theoretical predictions and empirically observable effects such as vacuum birefringence and pair production. Theoretical advancements presented here set the stage for future observational campaigns targeting magnetars, capitalizing on their extreme conditions to examine the predictions of quantum electrodynamics in regimes inaccessible in terrestrial laboratories. Future developments in space-based x-ray polarimetry and enhanced sensitivity observatories promise to refine these observational tests, possibly revolutionizing our understanding of electromagnetism under extreme conditions.

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