Access
To read this story in full you will need to login or make a payment (see right).
Letter
Nature 436, 673-676 (4 August 2005) | doi:10.1038/nature03909; Received 20 February 2005; Accepted 9 June 2005
Open Innovation Challenges
-
Single-cell Analysis Platform
This Challenge is looking for novel approaches to analyzing changes at a single-cell level. This is...
-
Direct Molecular Detection of Proteins and Nucleic Acids
This Challenge is looking for novel approaches to protein and nucleic acid detection. This is an Id...
nature jobs
Research Assistant Professor, Post-Doctoral Fellow, Statistical Genetic Analyst, and Scientific Programmer Positions in Statistical Human Genetics
- University of Michigan
- Ann Arbor, Michigan, USA
Faculty Positions in Cancer, Cardiovascular and Metabolic Diseases, Immunology
- Institut de recherches cliniques de Montreal
- Montreal, Quebec, Canada
Partial quantum information
Micha
Horodecki1,
Jonathan Oppenheim2
&
Andreas Winter3
- Institute of Theoretical Physics and Astrophysics, University of Gda
sk, 80-952 Gda
sk, Poland - Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, UK
- Department of Mathematics, University of Bristol, Bristol BS8 1TW, UK
Correspondence to: Jonathan Oppenheim2 Correspondence and requests for materials should be addressed to J.O. (Email: j.oppenheim@damtp.cam.ac.uk).
Abstract
Information—be it classical1 or quantum2—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 needed3. 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.
- Institute of Theoretical Physics and Astrophysics, University of Gda
sk, 80-952 Gda
sk, Poland - Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, UK
- Department of Mathematics, University of Bristol, Bristol BS8 1TW, UK
Correspondence to: Jonathan Oppenheim2 Correspondence and requests for materials should be addressed to J.O. (Email: j.oppenheim@damtp.cam.ac.uk).
To read this story in full you will need to login or make a payment (see right).
MORE ARTICLES LIKE THIS
These links to content published by NPG are automatically generated.
NEWS AND VIEWS
Entanglement Entangled and boundNature Physics News and Views (01 Oct 2009)
Instant teleportationNature News and Views (15 Apr 1993)
Quantum information theory The bits don't add upNature Physics News and Views (01 Apr 2009)
See all 18 matches for News And ViewsRESEARCH
Supplementary InformationNature Physics Article (01 Sep 2008)
See all 43 matches for Research
