Abstract

We consider a realistic setting of quantum tasks that generate shared bipartite quantum states. Suppose \alice and \bob are located at different places and need to produce a target shared quantum state ρρ. In order to save quantum communication, they can choose to share a proper smaller quantum state σσ first, and then turn σσ to ρρ by performing only local quantum operations and classical communications (LOCC). We hope σσ is the optimal such that the quantum communication needed is as little as possible, which is called the generation cost of ρρ. In this paper, for an arbitrary bipartite ρρ, we characterize its generation cost completely by proving that it is exactly equivalent to the logarithm of the Schmidt number of ρρ. Similar quantum schemes where classical communication is not allowed have actually been considered. By comparing the two settings, we are able to look into the role that classical communication plays in these fundamental tasks, where we exhibit some instances in which classical communication is not helpful completely.

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