Mean spin entanglement of two massive Dirac particles under Lorentz transformations
arXiv:1008.3447 · doi:10.1103/PhysRevA.84.012334
Abstract
We have studied the relativistic effects on the mean spin entanglement of two massive Dirac particles using the simultaneous eigen-spinors of the Foldy-Woutheysen mean spin operator and the Dirac Hamiltonian. We have obtained the transformation matrix from the spinor with specific momentum to the spinor with a transformed momentum under an arbitrary Lorentz transformation. Using the transformation matrix we have shown the consistent monotonic behavior between the concurrence and the maximum value of Bell parameter in Bell inequality of transformed spin states.
References in corpus (6)
- Spintronics: Fundamentals and applications
- Quantum Entanglement of Moving Bodies
- Lorentz-covariant reduced spin density matrix and EPR-Bohm correlations
- Comment on "Quantum entropy and special relativity" [by A. Peres, P. F. Scudo, and D. R. Terno, Phys. Rev. Lett. 88, 230402 (2002)]
- Einstein-Podolsky-Rosen correlations of Dirac particles - quantum field theory approach
- Lorentz-invariant Bell's inequality
Cited by in corpus (13)
- Physical interpretation of the Wigner rotations and its implications for relativistic quantum information
- Relativistic spin operators in various electromagnetic environments
- Spin quantum correlations of relativistic particles
- Global Dirac bispinor entanglement under Lorentz boosts
- Relativistic spin operator and Lorentz transformation of spin state of a massive Dirac particle
- Wigner rotations and an apparent paradox in relativistic quantum information
- Spin Operator and Entanglement in Quantum Field Theory
- Effects of Lorentz boosts on Dirac bispinor entanglement
- Quantum discord and entropic measures of two relativistic fermions
- Genuine multipartite entanglement and quantum coherence in an electron-positron system: Relativistic covariance
- Lorentz Invariant Quantum Concurrence for SU(2) x SU(2) spin-parity states
- Lorentz-covariance of Position Operator and its Eigenstates for a massive spin field
- Information under Lorentz transformation