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Separable states are more disordered globally than locally
Quantum Physics · Submitted 30 Nov 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this paper we prove the stronger result that for separable states the vector of eigenvalues of the density matrix of system AB is majorized by the vector of eigenvalues of the density matrix of system A alone.
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The abstract, sentence by sentence
A remarkable feature of quantum entanglement is that an entangled state of two parties, Alice (A) and Bob (B), may be more disordered locally than globally. That is, S(A) > S(A,B), where S(.) is the von Neumann entropy. It is known that satisfaction of this inequality implies that a state is non-separable. In this paper we prove the stronger result that for separable states the vector of eigenvalues of the density matrix of system AB is majorized by the vector of eigenvalues of the density matrix of system A alone. This gives a strong sense in which a separable state is more disordered globally than locally and a new necessary condition for separability of bipartite states in arbitrary dimensions. We also investigate the extent to which these conditions are sufficient to characterize separability, exhibiting examples that show separability cannot be characterized solely in terms of the local and global spectra of a state. We apply our conditions to give a simple proof that non-separable states exist sufficiently close to the completely mixed state of $n$ qudits.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A remarkable feature of quantum entanglement is that an entangled state of two parties, Alice (A) and Bob (B), may be more disordered locally than globally. | background 1.00 | 0.08 | 0.06 | hedged possibility 0.94 |
| s1 | That is, S(A) > S(A,B), where S(.) is the von Neumann entropy. | background 0.92 | 0.10 | 0.03 | asserted 0.99 |
| s2 | It is known that satisfaction of this inequality implies that a state is non-separable. | background 1.00 | 0.05 | 0.03 | asserted 1.00 |
| s3 | In this paper we prove the stronger result that for separable states the vector of eigenvalues of the density matrix of system AB is majorized by the vector of eigenvalues of the density matrix of system A alone. | result 0.91 | 0.95 | 0.90 | asserted 1.00 |
| s4 | This gives a strong sense in which a separable state is more disordered globally than locally and a new necessary condition for separability of bipartite states in arbitrary dimensions. | interpretation 0.67 | 0.92 | 0.74 | asserted 0.96 |
| s5 | We also investigate the extent to which these conditions are sufficient to characterize separability, exhibiting examples that show separability cannot be characterized solely in terms of the local and global spectra of a state. | result 0.45 | 0.96 | 0.07 | asserted 1.00 |
| s6 | We apply our conditions to give a simple proof that non-separable states exist sufficiently close to the completely mixed state of $n$ qudits. | contribution 0.51 | 0.94 | 0.04 | asserted 1.00 |
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Original abstract
A remarkable feature of quantum entanglement is that an entangled state of two parties, Alice (A) and Bob (B), may be more disordered locally than globally. That is, S(A) > S(A,B), where S(.) is the von Neumann entropy. It is known that satisfaction of this inequality implies that a state is non-separable. In this paper we prove the stronger result that for separable states the vector of eigenvalues of the density matrix of system AB is majorized by the vector of eigenvalues of the density matrix of system A alone. This gives a strong sense in which a separable state is more disordered globally than locally and a new necessary condition for separability of bipartite states in arbitrary dimensions. We also investigate the extent to which these conditions are sufficient to characterize separability, exhibiting examples that show separability cannot be characterized solely in terms of the local and global spectra of a state. We apply our conditions to give a simple proof that non-separable states exist sufficiently close to the completely mixed state of $n$ qudits.
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