Entanglement entropy of multipartite pure states
暂无分享,去创建一个
Consider a system consisting of n d-dimensional quantum particles and an arbitrary pure state vertical bar {psi}> of the whole system. Suppose we simultaneously perform complete von Neumann measurements on each particle. The Shannon entropy of the outcomes' joint probability distribution is a functional of the state vertical bar {psi}> and of n measurements chosen for each particle. Denote S[{psi}] the minimum of this entropy over all choices of the measurements. We show that S[{psi}] coincides with the entropy of entanglement for bipartite states. We compute S[{psi}] for some special multipartite states: the hexacode state vertical bar H> (n=6, d=2) and the determinant states vertical bar Det{sub n}> (d=n). The computation yields S[H]=4 log 2 and S[Det{sub n}]=log(n{exclamation_point}). Counterparts of the determinant state defined for d
[1] Charles H. Bennett,et al. Concentrating partial entanglement by local operations. , 1995, Physical review. A, Atomic, molecular, and optical physics.
[2] G. Vidal. On the characterization of entanglement , 1998 .
[3] I. Chuang,et al. Quantum Computation and Quantum Information: Introduction to the Tenth Anniversary Edition , 2010 .
[4] S. Popescu,et al. Thermodynamics and the measure of entanglement , 1996, quant-ph/9610044.