“…This problem may be roughly described in this manner [1,2,3,4,5,6]: Suppose that a transmitter, Alice, wants to convey classical information to a receiver, Bob, using a quantum channel, and Alice represents the message conveyed as a mixed quantum state that, with given prior probabilities, belongs to a finite set of mixed quantum states, say {ρ 1 , ρ 2 , . .…”