Abstract
The violation of the Bell inequality for Dirac fermions is investigated in the cosmological de Sitter spacetime, in the presence of background electromagnetic fields of constant strengths. The orthonormal Dirac mode functions are obtained and the relevant in-out squeezed state expansion in terms of the Bogoliubov coefficients are found. We focus on two scenarios here: strong electric field and heavy mass limits (with respect to the Hubble constant). Using the squeezed state expansion, we then demonstrate the Bell violations for the vacuum and some maximally entangled initial states. Even though a background magnetic field alone cannot create particles, in the presence of background electric field and or spacetime curvature, it can affect the particle creation rate. Thus, our chief aim here is to investigate the role of the background magnetic field strength in the Bell violation. Qualitative differences in this regard for different maximally entangled initial states are shown. Further extension of these results to the so-called $\ensuremath{\alpha}$ vacua are also discussed.
Highlights
One of the most outstanding features of quantum mechanics is certainly the entanglement, associated with the nonlocal properties of the quantum mechanical measurement procedure [1,2,3,4,5,6,7,8,9]
A very important and useful measure of quantum entanglement is the violation of the Bell inequality [2,3], which has been confirmed experimentally [10,11]
The Bell inequality was originally designed for bipartite pure states, which was later extended to multipartite systems, altogether known as the
Summary
One of the most outstanding features of quantum mechanics is certainly the entanglement, associated with the nonlocal properties of the quantum mechanical measurement procedure [1,2,3,4,5,6,7,8,9]. We wish to compute the Bell violation for fermions in the cosmological de Sitter spacetime, in the presence of constant background electromagnetic fields. Pair creation only due to a background electric field is expected to cease upon the application of a magnetic field of sufficiently high strength, due to the aforementioned oppositely directed Lorentz force created by them. This can possibly be used to constrain the corresponding field strengths and test the proposition of [50] With this motivation, and as a problem to begin with, we shall compute below the fermionic Bell violation in the cosmological de Sitter spacetime in the presence of background electromagnetic fields, as a viable measure of quantum entanglement.
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