Classical channel vs quantum channel

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SUMMARY

This discussion clarifies the distinction between classical channels and quantum channels within quantum information theory. A classical channel is defined by a conditional probability distribution P(ylx), while a quantum channel is represented by the formula ∑x,y (Tr lx> PREREQUISITES

  • Understanding of quantum information theory
  • Familiarity with conditional probability distributions
  • Knowledge of linear algebra, particularly trace operations
  • Basic concepts of quantum states and operators
NEXT STEPS
  • Study the mathematical foundations of quantum channels and their properties
  • Explore the implications of the trace operation in quantum mechanics
  • Investigate the differences between classical and quantum information transmission
  • Learn about specific examples of quantum channels, such as depolarizing and amplitude damping channels
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Researchers, students, and professionals in quantum computing, quantum information theory, and anyone interested in the mathematical underpinnings of classical versus quantum communication channels.

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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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