Classical channel vs quantum channel

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I have a hard time understanding what a channel that transmits classical information is in the framework of quantum information theory. My textbook says the following:

Let P(ylx) be a classical channel defined by a conditional probability distribution. We define the corresponding quantum channel by:

x,y (Tr lx><xlX)P(ylx)ly><yl

How should I interpret this formula and what is the role of the trace appearing? And in general what is a classical channel as opposed to a quantum channel? I guess the answer is that a classical channel can send definite states given by some probability distribution, while quantum channels are maps between states in general.

Another place in the book it states that a classical channel of two bits is of the form:
C(X) = ∑i,j lij><ijl Tr lij><ijlX
Is this equivalent with the first formula?
 
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Could you explain what is X in your question?
Have you links to this subject?
 
The first thing which comes to my mind is that the trace of ##\rho X## is the mean value of X in the state ##\rho##
Now if X is an operator it sends X to another operator. How can we describe it? What is the image of a projector |z><z|?
 
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If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
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