Eur. Phys. J. D 55, 379-389 (2009)
https://doi.org/10.1140/epjd/e2009-00149-x

Signatures of the Unruh effect via high-power, short-pulse lasers

¹ Faculty of Physics, Ludwig-Maximilians-University München, 85748 Garching, Germany
² Max-Planck Institute of Quantum Optics, 85748 Garching, Germany
³ Imperial College, SW7 2, AZ London, UK
⁴ Fachbereich Physik, University of Duisburg-Essen, 47048 Duisburg, Germany
⁵ Institut für Theoretische Physik, TU Berlin, 10623 Berlin, Germany

Corresponding author: ^a Peter.Thirolf@physik.uni-muenchen.de

Received: 14 November 2008
Revised: 28 February 2009
Published online: 16 May 2009

Abstract

The ultra-high fields of high-power short-pulse lasers are expected to contribute to understanding fundamental properties of the quantum vacuum and quantum theory in very strong fields. For example, the neutral QED vacuum breaks down at the Schwinger field strength of 1.3×10¹⁸ V/m, where a virtual e⁺e^- pair gains its rest mass energy over a Compton wavelength and materializes as a real pair. At such an ultra-high field strength, an electron experiences an acceleration of a_S=2×10²⁸g and hence fundamental phenomena such as the long predicted Unruh effect start to play a role. The Unruh effect implies that the accelerated electron experiences the vacuum as a thermal bath with the Unruh temperature. In its accelerated frame the electron scatters photons off the thermal bath, corresponding to the emission of an entangled pair of photons in the laboratory frame. While it remains an experimental challenge to reach the critical Schwinger field strength within the immediate future even in view of the enormous thrust in high-power laser developments in recent years, the near-future laser technology may allow to probe the signatures of the Unruh effect mentioned above. Using a laser-accelerated electron beam (γ∼300) and a counter-propagating laser beam acting as optical undulator should allow to create entangled Unruh photon pairs (i.e., signatures of the Unruh effect) with energies of the order of several hundred keV. An even substantially improved experimental scenario can be realized by using a brilliant 20 keV photon beam as X-ray undulator together with a low-energy (γ≈2) electron beam. In this case the separation of the Unruh photon pairs from background originating from linearly accelerated electrons (classical Larmor radiation) is significantly improved. Detection of the Unruh photons may be envisaged by Compton polarimetry in a 2D-segmented position-sensitive germanium detector.