No-broadcast theorem

In physics, the no-broadcast theorem is a result in quantum information theory. In the case of pure quantum states, it is a corollary of the no-cloning theorem: since quantum states cannot be copied in general, they cannot be broadcast. Here, the word "broadcast" is used in the sense of conveying the state to two or more recipients. For multiple recipients to each receive the state, there must be, in some sense, a way of duplicating the state. The no-broadcast theorem generalizes the no-cloning theorem for mixed states.

The no-cloning theorem says that it is impossible to create two copies of a state given a single copy of the state.

The no-broadcast theorem says that, given a single copy of a state, it is impossible to create a state such that one part of it is the same as the original state and the other part is also the same as the original state. I.e., given an initial state \rho_1, it is impossible to create a state \rho_{AB} in a Hilbert space H_A\otimes H_B such that the partial trace Tr_A\rho_{AB}=\rho_1 and Tr_B\rho_{AB}=\rho_1. Although here we work with mixed states, a broadcasting machine would have to work on any pure state ensemble of \rho_1.

See also

References

This article is issued from Wikipedia - version of the Saturday, February 06, 2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.