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      Entanglement and the foundations of statistical mechanics

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      Nature Physics
      Springer Science and Business Media LLC

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          Partial quantum information.

          Information--be it classical or quantum--is measured by the amount of communication needed to convey it. In the classical case, if the receiver has some prior information about the messages being conveyed, less communication is needed. Here we explore the concept of prior quantum information: given an unknown quantum state distributed over two systems, we determine how much quantum communication is needed to transfer the full state to one system. This communication measures the partial information one system needs, conditioned on its prior information. We find that it is given by the conditional entropy--a quantity that was known previously, but lacked an operational meaning. In the classical case, partial information must always be positive, but we find that in the quantum world this physical quantity can be negative. If the partial information is positive, its sender needs to communicate this number of quantum bits to the receiver; if it is negative, then sender and receiver instead gain the corresponding potential for future quantum communication. We introduce a protocol that we term 'quantum state merging' which optimally transfers partial information. We show how it enables a systematic understanding of quantum network theory, and discuss several important applications including distributed compression, noiseless coding with side information, multiple access channels and assisted entanglement distillation.
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            Entropy of an n‐system from its correlation with a k‐reservoir

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              Quantum Thermodynamics

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                Author and article information

                Journal
                Nature Physics
                Nature Phys
                Springer Science and Business Media LLC
                1745-2473
                1745-2481
                November 2006
                October 29 2006
                November 2006
                : 2
                : 11
                : 754-758
                Article
                10.1038/nphys444
                e05ff10b-d773-4eeb-8a3f-4bf3b8eec74e
                © 2006

                http://www.springer.com/tdm

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