Entanglement of Dirac bi-spinor states driven by Poincaré classes of $\mbox{SU}(2) \otimes \mbox{SU}(2)$ coupling potentials
arXiv:1511.07047 · doi:10.1016/j.aop.2015.11.004
Abstract
A generalized description of entanglement and quantum correlation properties constraining internal degrees of freedom of Dirac(-like) structures driven by arbitrary Poincaré classes of external field potentials is proposed. The role of (pseudo)scalar, (pseudo)vector and tensor interactions in producing/destroying intrinsic quantum correlations for $\mbox{SU}(2) \otimes \mbox{SU}(2)$ bi-spinor structures is discussed in terms of generic coupling constants. By using a suitable ansatz to obtain the Dirac Hamiltonian eigenspinor structure of time-independent solutions of the associated Liouville equation, the quantum entanglement, via concurrence, and quantum correlations, via geometric discord, are computed for several combinations of well-defined Poincaré classes of Dirac potentials. Besides its inherent formal structure, our results setup a framework which can be enlarged as to include localization effects and to map quantum correlation effects into Dirac-like systems which describe low-energy excitations of graphene and trapped ions.
29 pages, 8 figures
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- Graphene lattice-layer entanglement under non-Markovian phase noise
- Schrödinger cat and Werner state disentanglement simulated by trapped ion systems
- Effects of Lorentz boosts on Dirac bispinor entanglement
- Phase-space elementary information content of confined Dirac spinors
- Lorentz Invariant Quantum Concurrence for SU(2) x SU(2) spin-parity states
- CP symmetry and thermal effects on Dirac bi-spinor spin-parity local correlations
- Dirac bi-spinor entanglement under local noise and its simulation by Jaynes-Cummings interactions