Global Dirac bispinor entanglement under Lorentz boosts

TL;DR

This paper investigates how Lorentz boosts affect quantum entanglement in Dirac bispinor systems, revealing that boosts degrade certain entanglements but preserve others, with a comprehensive covariant framework for analysis.

Contribution

It develops a Lorentz covariant framework to analyze entanglement changes in Dirac bispinor systems under boosts, including specific results for anti-symmetric and chiral states.

Findings

Spin-spin entanglement cannot be created by boosts in separable states.

High-speed boosts degrade maximal spin-spin entanglement.

Chiral states exhibit invariance properties under Lorentz boosts.

Abstract

The effects of Lorentz boosts on the quantum entanglement encoded by a pair of massive spin one-half particles are described according to the Lorentz covariant structure described by Dirac bispinors. The quantum system considered incorporates four degrees of freedom -- two of them related to the bispinor intrinsic parity and other two related to the bispinor spin projection, i.e. the Dirac particle helicity. Because of the natural multipartite structure involved, the Meyer-Wallach global measure of entanglement is preliminarily used for computing global quantum correlations, while the entanglement separately encoded by spin degrees of freedom is measured through the negativity of the reduced two-particle spin-spin state. A general framework to compute the changes on quantum entanglement induced by a boost is developed, and then specialized to describe three particular anti-symmetric two-particle states. According to the obtained results, two-particle spin-spin entanglement cannot be created by the action of a Lorentz boost in a spin-spin separable anti-symmetric state. On the other hand, the maximal spin-spin entanglement encoded by anti-symmetric superpositions is degraded by Lorentz boosts driven by high-speed frame transformations. Finally, the effects of boosts on chiral states are shown to exhibit interesting invariance properties, which can only be obtained through such a Lorentz covariant formulation of the problem.