Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

On a conjecture of the quantum correlations

Zhang Lin, Junde Wu

Published May 16, 2011• 0 citations
OpenAlex

Abstract

In this paper, two conjectures which were proposed in [Phys. Rev. A \textbf{82}, 052122(2010)] on the correlations in a bipartite state $\rho^{AB}$ are studied. If the mutual information $I\Pa{\rho^{AB}}$ between two quantum systems $A$ and $B$ before any measurement is considered as the total amount of correlations in the state $\rho^{AB}$, then it can be separated into two parts: classical correlations and quantum correlations. The so-called classical correlations $C\Pa{\rho^{AB}}$ in the state $\rho^{AB}$, defined by the maximizing mutual information between two quantum systems $A$ and $B$ after von Neumann measurements on system $B$, we show that it is upper bounded by the von Neumann entropies of both subsystems $A$ and $B$, this answered the conjecture on the classical correlation. If the quantum correlations $Q\Pa{\rho^{AB}}$ in the state $\rho^{AB}$ is defined by $Q\Pa{\rho^{AB}}= I\Pa{\rho^{AB}} - C\Pa{\rho^{AB}}$, we show also that it is upper bounded by the von Neumann entropy of subsystem $B$. It is also obtained that $Q\Pa{\rho^{AB}}$ is upper bounded by the von Neumann entropy of subsystem $A$ for a class of states.

Related papers

On conjectures of classical and quantum correlations in bipartite states

Lin Zhang, Junde Wu

In this paper, two conjectures which were proposed in Luo et al (2010 Phys. Rev. A 82 052122 ) on the correlations in a bipartite state ρ AB are studied. If the mutual information I (ρ AB ) between two quantum systems A and B before any measurement is considered as the total amount of correlations in the state ρ AB , then it can be separated into two parts: classical correlations and quantum correlations. The so-called classical correlations C (ρ AB ) in the state ρ AB are defined by the maximizing mutual information between two quantum systems A and B after von Neumann measurements on system B . We show that it is upper bounded by the von Neumann entropies of both subsystems A and B , which answered the conjecture on the classical correlation. If the quantum correlations Q (ρ AB ) in the state ρ AB are defined by Q (ρ AB ) = I (ρ AB ) − C (ρ AB ), we also show that it is upper bounded by the von Neumann entropy of subsystem B . It is also found that Q (ρ AB ) is upper bounded by the von Neumann entropy of subsystem A for a class of states.

arXiv:1105.2993•Journal of Physics A Mathematical and Theoretical•Dec 8, 2011•24 citations

On the upper bound of classical correlations in a bipartite quantum system

Theresa Christ, Haye Hinrichsen

Abstract For a bipartite quantum system consisting of subsystems A and B it was shown by Zhang et al (2012 Phys. Lett . A 376 3588–92) that the amount of classical correlations, which is used to define the quantum discord, is known to be bounded from above by the minimum of the von Neumann entropies of the subsystems A and B . We provide an alternative proof that is shorter and more transparent as it works without defining correlation matrices.

arXiv:1702.07264•Journal of Physics A Mathematical and Theoretical•Aug 22, 2017•0 citations

Total versus quantum correlations in a two-mode Gaussian state

Jamal El Qars

Abstract In Li and Luo (2007 Phys. Rev. A 76 032327), the inequality ( 1 / 2 )  ≥  was identified as a fundamental postulate for a consistent theory of quantum versus classical correlations for arbitrary measures of total  and quantum  correlations in bipartite quantum states. Besides, Hayden et al (2006 Commun. Math. Phys. 265 95) have conjectured that, in some conditions within systems endowed with infinite-dimensional Hilbert spaces, quantum correlations may dominate not only half of total correlations but total correlations itself. Here, in a two-mode Gaussian state, quantifying  and  respectively by the quantum mutual information  G and the entanglement of formation (EoF)  F G , we verify that  F , R G is always less than ( 1 / 2 )  R G when  G and  F G are defined via the Rényi-2 entropy. While via the von Neumann entropy,  F , V G may even dominate 

Communications in Theoretical Physics•Mar 2, 2021•7 citations

Classical and quantum correlative capacities of quantum systems

Nan Li, Shunlong Luo

How strongly can one system be correlated with another? In the classical world, this basic question concerning correlative capacity has a very satisfying answer: The ``effective size'' of the marginal system, as quantified by the Shannon entropy, sets a tight upper bound to the correlations, as quantified by the mutual information. Although in the quantum world bipartite correlations, like their classical counterparts, are also well quantified by mutual information, the similarity ends here: The correlations in a bipartite quantum system can be twice as large as the marginal entropy. In the paradigm of quantum discord, the correlations are split into classical and quantum components, and it was conjectured that both the classical and quantum correlations are (like the classical mutual information) bounded above by each subsystem's entropy. In this work, by exploiting the interplay between entanglement of formation, mutual information, and quantum discord, we disprove that conjecture. We further indicate a scheme to restore harmony between quantum and classical correlative capacities. The results illustrate dramatically the asymmetric nature of quantum discord and highlight some subtle and unusual features of quantum correlations.

Physical Review A•Oct 31, 2011•31 citations

Extracting classical correlations from a bipartite quantum system

S. Hamieh, J. Qi, David J. Siminovitch +1 more

In this paper, we discuss the problem of splitting of the total correlations for a bipartite quantum state described by the Von Neumann mutual information into classical and quantum parts. We propose a measure of the classical correlations as the difference between the Von Neumann mutual information and the relative entropy of entanglement. We compare this measure with different measures proposed in the literature.

arXiv:quant-ph/0211006•Physical Review A•Jan 9, 2003•16 citations

Von Neumann entropy, mutual information and total correlations of Gaussian states

Alessio Serafini, Fabrizio Illuminati, Silvio De Siena

We determine the Von Neumann entropy and the mutual information of an arbitrary bipartite Gaussian state. A comparison between mutual information and entanglement of formation for symmetric states is considered, remarking the crucial role of the symplectic eigenvalues in qualifying and quantifying correlations.

•Jul 9, 2003•1 citation
In this paper, two conjectures which were proposed in [Phys. Rev. A \textbf{82}, 052122(2010)] on the correlations in a bipartite state ρAB\rho^{AB}ρAB are studied. If the mutual information I\PaρABI\Pa{\rho^{AB}}I\PaρAB between two quantum systems AAA and BBB before any measurement is considered as the total amount of correlations in the state ρAB\rho^{AB}ρAB, then it can be separated into two parts: classical correlations and quantum correlations. The so-called classical correlations C\PaρABC\Pa{\rho^{AB}}C\PaρAB in the state ρAB\rho^{AB}ρAB, defined by the maximizing mutual information between two quantum systems AAA and BBB after von Neumann measurements on system BBB, we show that it is upper bounded by the von Neumann entropies of both subsystems AAA and BBB, this answered the conjecture on the classical correlation. If the quantum correlations Q\PaρABQ\Pa{\rho^{AB}}Q\PaρAB in the state ρAB\rho^{AB}ρAB is defined by Q\PaρAB=I\PaρAB−C\PaρABQ\Pa{\rho^{AB}}= I\Pa{\rho^{AB}} - C\Pa{\rho^{AB}}Q\PaρAB=I\PaρAB−C\PaρAB, we show also that it is upper bounded by the von Neumann entropy of subsystem BBB. It is also obtained that Q\PaρABQ\Pa{\rho^{AB}}Q\PaρAB is upper bounded by the von Neumann entropy of subsystem AAA for a class of states.
In this paper, two conjectures which were proposed in Luo et al (2010 Phys. Rev. A 82 052122 ) on the correlations in a bipartite state ρ AB are studied. If the mutual information I (ρ AB ) between two quantum systems A and B before any measurement is considered as the total amount of correlations in the state ρ AB , then it can be separated into two parts: classical correlations and quantum correlations. The so-called classical correlations C (ρ AB ) in the state ρ AB are defined by the maximizing mutual information between two quantum systems A and B after von Neumann measurements on system B . We show that it is upper bounded by the von Neumann entropies of both subsystems A and B , which answered the conjecture on the classical correlation. If the quantum correlations Q (ρ AB ) in the state ρ AB are defined by Q (ρ AB ) = I (ρ AB ) − C (ρ AB ), we also show that it is upper bounded by the von Neumann entropy of subsystem B . It is also found that Q (ρ AB ) is upper bounded by the von Neumann entropy of subsystem A for a class of states.
Abstract In Li and Luo (2007 Phys. Rev. A 76 032327), the inequality ( 1 / 2 )  ≥  was identified as a fundamental postulate for a consistent theory of quantum versus classical correlations for arbitrary measures of total  and quantum  correlations in bipartite quantum states. Besides, Hayden et al (2006 Commun. Math. Phys. 265 95) have conjectured that, in some conditions within systems endowed with infinite-dimensional Hilbert spaces, quantum correlations may dominate not only half of total correlations but total correlations itself. Here, in a two-mode Gaussian state, quantifying  and  respectively by the quantum mutual information  G and the entanglement of formation (EoF)  F G , we verify that  F , R G is always less than ( 1 / 2 )  R G when  G and  F G are defined via the Rényi-2 entropy. While via the von Neumann entropy,  F , V G may even dominate 
How strongly can one system be correlated with another? In the classical world, this basic question concerning correlative capacity has a very satisfying answer: The ``effective size'' of the marginal system, as quantified by the Shannon entropy, sets a tight upper bound to the correlations, as quantified by the mutual information. Although in the quantum world bipartite correlations, like their classical counterparts, are also well quantified by mutual information, the similarity ends here: The correlations in a bipartite quantum system can be twice as large as the marginal entropy. In the paradigm of quantum discord, the correlations are split into classical and quantum components, and it was conjectured that both the classical and quantum correlations are (like the classical mutual information) bounded above by each subsystem's entropy. In this work, by exploiting the interplay between entanglement of formation, mutual information, and quantum discord, we disprove that conjecture. We further indicate a scheme to restore harmony between quantum and classical correlative capacities. The results illustrate dramatically the asymmetric nature of quantum discord and highlight some subtle and unusual features of quantum correlations.