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.

[1]  Andreas J. Winter,et al.  On the Distributed Compression of Quantum Information , 2006, IEEE Transactions on Information Theory.

[2]  Igor Devetak The private classical capacity and quantum capacity of a quantum channel , 2005, IEEE Transactions on Information Theory.

[3]  M. Horodecki,et al.  The entanglement of purification , 2002, quant-ph/0202044.

[4]  David P. DiVincenzo,et al.  Entanglement of Assistance , 1998, QCQC.

[5]  I Devetak,et al.  Relating quantum privacy and quantum coherence: an operational approach. , 2004, Physical review letters.

[6]  A. Winter,et al.  Quantum, classical, and total amount of correlations in a quantum state , 2004, quant-ph/0410091.

[7]  Charles H. Bennett,et al.  Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels. , 1993, Physical review letters.

[8]  E. Schrödinger Die gegenwärtige Situation in der Quantenmechanik , 1935, Naturwissenschaften.

[9]  Schumacher,et al.  Quantum data processing and error correction. , 1996, Physical review. A, Atomic, molecular, and optical physics.

[10]  E. Schrödinger Die gegenwärtige Situation in der Quantenmechanik , 2005, Naturwissenschaften.

[11]  Sang Joon Kim,et al.  A Mathematical Theory of Communication , 2006 .

[12]  R. A. McDonald,et al.  Noiseless Coding of Correlated Information Sources , 1973 .

[13]  M. Horodecki,et al.  Local versus nonlocal information in quantum-information theory: Formalism and phenomena , 2004, quant-ph/0410090.

[14]  P. Horodecki,et al.  Quantum redundancies and local realism , 1994 .

[15]  C. Adami,et al.  Negative entropy and information in quantum mechanics , 1995, quant-ph/9512022.

[16]  S. Lloyd Capacity of the noisy quantum channel , 1996, quant-ph/9604015.

[17]  J I Cirac,et al.  Entanglement versus correlations in spin systems. , 2004, Physical review letters.

[18]  E. Lieb,et al.  Proof of the strong subadditivity of quantum‐mechanical entropy , 1973 .

[19]  Albert Einstein,et al.  Can Quantum-Mechanical Description of Physical Reality Be Considered Complete? , 1935 .

[20]  John A. Smolin,et al.  Entanglement of assistance and multipartite state distillation , 2005 .

[21]  A. Wehrl General properties of entropy , 1978 .

[22]  Aaron D. Wyner,et al.  On source coding with side information at the decoder , 1975, IEEE Trans. Inf. Theory.

[23]  Nicolas Spyratos,et al.  An operational approach to data bases , 1982, PODS.