摘要Many properties of partial transposition are unclear as yet. Here we carefully consider the number of the negative eigenvalues of ρT (ρ's partial transposition) when ρ is a two-partite state. There is strong evidence to show that the number of negative eigenvalues of ρT is N(N-1)/2 at most when ρ is a state in Hilbert space CN×CN. For the special case, the 2×2 system, we use this result to give a partial proof of the conjecture |ρT|T≥0. We find that this conjecture is strongly connected with the entanglement of the state corresponding to the negative eigenvalue of ρ^T or the negative entropy of ρ.
Abstract:Many properties of partial transposition are unclear as yet. Here we carefully consider the number of the negative eigenvalues of ρT (ρ's partial transposition) when ρ is a two-partite state. There is strong evidence to show that the number of negative eigenvalues of ρT is N(N-1)/2 at most when ρ is a state in Hilbert space CN×CN. For the special case, the 2×2 system, we use this result to give a partial proof of the conjecture |ρT|T≥0. We find that this conjecture is strongly connected with the entanglement of the state corresponding to the negative eigenvalue of ρ^T or the negative entropy of ρ.
[1] Nielsen M A and Chuang I L 2000 Quantum Computationand Quantum Information (Cambridge: Cambridge University Press) [2] Bennett C H et al 1996 Phys. Rev. A 54 3824 [3] Vedral V and Plenio M B 1998 Phys. Rev. A 571619 [4] Lewenstein M et al 2001 Phys. Rev. A 63 044304 [5] D\"{ur W and Cirac J I 2000 Phys. Rev. A 62022302 [6] Peres A 1996 Phys. Rev. Lett. 77 1413 [7] Horodecki M et al 1996 Phys. Lett. A 223 1 [8] Audenaert K et al 2002 Phys. Rev. A 66 032310 [9] Ishizaka S 2004 Phys. Rev. A 69 020301 [10] Horn R A and Johnson C R 1985 Matrix Analysis(Cambridge: Cambridge University) [11] Verstraete F et al 2001 J. Phys. A 34 10327 [12] Landau D P and Binder K 2005 A Guide to Monte CarloSimulations in Statistical Physics (Cambridge: Cambridge UniversityPress) [13] Vidal G and Werner R F 2002 Phys. Rev. A 65032314