Quantum One-Time Pad in the Presence of an Eavesdropper
Abstract
A classical one-time pad allows two parties to send private messages over a public classical channel—an eavesdropper who intercepts the communication learns nothing about the message. A quantum one-time pad is a shared quantum state which allows two parties to send private messages or private quantum states over a public quantum channel. If the eavesdropper intercepts the quantum communication she learns nothing about the message. In the classical case, a one-time pad can be created using shared and partially private correlations. Here we consider the quantum case in the presence of an eavesdropper, and find the single-letter formula for the rate at which the two parties can send messages using a general quantum state as a quantum one-time pad. Surprisingly, the formula coincides with the distillable entanglement assisted by a symmetric channel, an important quantity in quantum information theory, but which lacked a clear operational meaning.
Additional Information
© 2012 American Physical Society. (Received 10 May 2010; revised manuscript received 28 July 2011; published 27 January 2012) F. B. is supported by a fellowship "Conhecimento Novo" from Fundação de Amparo a Pesquisa do Estado de Minas Gerais (FAPEMIG). J. O. is supported by the Royal Society, and National Science Foundation under Grant No. PHY05-51164 during his stay at KITP.Attached Files
Published - PhysRevLett.108.040504.pdf
Files
Name | Size | Download all |
---|---|---|
md5:b94782374bbe136ee0c2f0ddf51106b4
|
119.4 kB | Preview Download |
Additional details
- Eprint ID
- 67717
- Resolver ID
- CaltechAUTHORS:20160607-101711780
- Fundação de Amparo a Pesquisa do Estado de Minas Gerais (FAPEMIG)
- Royal Society
- NSF
- PHY05-51164
- Created
-
2016-06-07Created from EPrint's datestamp field
- Updated
-
2021-11-11Created from EPrint's last_modified field