A Mathematical Theory of Communication
Shannon, 1948, A Mathematical Theory of Communication (Bell System Technical Journal)
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8 Representation of the encoding and decoding operations
- How does Shannon model transmitters and receivers in the discrete case?As finite-state transducers: output \(y_n = f(x_n, \alpha_n)\) and next state \(\alpha_{n+1} = g(x_n, \alpha_n)\). A transducer is non-singular if an inverse transducer can recover its input.
- Shannon, 1948, A Mathematical Theory of Communication (Bell System Technical Journal), §8
- What happens to entropy when a source passes through a finite-state transducer (Theorem 7)?The output is again a finite-state source with entropy per unit time no greater than the input’s; equal if the transducer is non-singular. Encoding cannot create information.
- Shannon, 1948, A Mathematical Theory of Communication (Bell System Technical Journal), §8
Source
- Claude E. Shannon. 1948. A Mathematical Theory of Communication. In Bell System Technical Journal, pp. 379–423, 623–656. doi:10.1002/j.1538-7305.1948.tb01338.x