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arXiv:1908.01005 · Physical review. D/Physical review. D.

State of a particle pair produced by the Schwinger effect is not necessarily a maximally entangled Bell state

De-Chang Dai

Published Aug 15, 2019• 7 citations
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Abstract

We analyze the spins of a Schwinger particle pair in a spatially uniform but time dependent electric field. The particle pair's spins are in the maximally entangled Bell state only if the particles' momenta are parallel to the electric field. However if transverse momentum is present, the spins are not in the maximally entangled Bell state. The reason is that the pair is created by the external field, which also carries angular momentum, and the particle pair can take away some of this external angular momentum.

DOI
10.1103/physrevd.100.045015

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We study the charge resolved structure of the pairwise mode entanglement produced by the Schwinger effect. Using the U(1)U(1)U(1) electric charge of quantum electrodynamics, we decompose the entanglement of the reduced density matrices of momentum modes into individual charge sectors, applying the symmetry resolved entanglement entropy to the pure bipartition reductions and the charge imbalance resolved negativity to the mixed particle-antiparticle pair. For a constant electric field we obtain closed form results for every mode pairing, with all field dependence controlled by the single pair production probability ∣β∣2=e−πμ|β|^2=e^{-πμ}∣β∣2=e−πμ. For the particle, particle and antiparticle antiparticle pairs the entanglement entropy within each charge sector is field independent, so that the field acts only by redistributing statistical weight among the sectors; for the mixed particle antiparticle pair the populated sector additionally carries a field dependent entropy. The vacuum created pair is the richest case: its resolved negativity is distributed over three imbalance sectors and is transported from one sector to the next as the field increases, the sectors contributing equally only at the critical field. The entanglement across a fixed momentum bipartition, by contrast, is frozen at its initial value because pair creation conserves the sector charge. Symmetry resolution thus refines the total entanglement measures into a sector resolved picture, exposing where in charge space the entanglement of the Schwinger mechanism resides and how the electric field moves it, information beyond that contained in the total measures or in particle number distributions.
We examine the behaviour of the maximally entangled Bell state of two spin 1 massive particles under relativistic transformations. On the basis of explicit calculations of the Wigner rotation and the use of transformation properties of Dirac spinors, we establish that the constituent particles of the Bell state undergo momentum dependent rotation of the spin orientations characterized by the Wigner angle φW = tan −1 sinhsinh τ cosh � +cosh τ . However, since local unitarity is retained in the process, the corresponding entanglement fidelity is not lost. c
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Abstract: We examine the behaviour of the maximally entangled Bell state of two spin 12 massive particles under relativistic transformations. On the basis of explicit calculations of the Wigner rotation and the use of transformation properties of Dirac spinors, we establish that the constituent particles of the Bell state undergo momentum dependent rotation of the spin orientations characterized by the Wigner angle φW = tan−1 sinh sinh τcosh+cosh τ. However, since local unitarity is retained in the process, the corresponding entanglement fidelity is not lost.