Canonical forms of two-qubit states under local operations
arXiv:2007.00697 · doi:10.1103/PhysRevA.102.052419
Abstract
Canonical forms of two-qubits under the action of stochastic local operations and classical communications (SLOCC) offer great insight for understanding non-locality and entanglement shared by them. They also enable geometric picture of two-qubit states within the Bloch ball. It has been shown (Verstraete et.al. {Phys. Rev. A, 64, 010101(R) (2001)) that an arbitrary two-qubit state gets transformed under SLOCC into one of the {\em two} different canonical forms. One of these happens to be the Bell diagonal form of two-qubit states and the other non-diagonal canonical form is obtained for a family of rank deficient two-qubit states. The method employed by Verstraete et.al. required highly non-trivial results on matrix decompositions in dimensional spaces with indefinite metric. Here we employ an entirely different approach -- inspired by the methods developed by Rao et. al., (J. Mod. Opt. 45, 955 (1998)) in classical polarization optics -- which leads naturally towards the identification of two inequivalent SLOCC invariant canonical forms for two-qubit states. In addition, our approach results in a simple geometric visualization of two-qubit states in terms of their SLOCC canonical forms.
arXiv comment14 pages, two figures; proof of the theorem in page 4 is outlined in the Appendix A of this revised version; accepted for publication in Phys. Rev. A
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- Multiphoton, multimode state classification for nonlinear optical circuits
- Canonical structures of and forms
- Swapping of quantum correlations and the role of local filtering operations
- Lorentz invariants of pure three-qubit states
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- Entanglement and volume monogamy features of permutation symmetric N-qubit pure states with N-distinct spinors: GHZ and WWbar states