Information Theory

3 min read#information

The mathematics of measuring information — quantifying surprise, and the hard limits it sets on compression and communication.

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Information Theory

Information theory is the science of how much — how much a message tells you, how far it can be squeezed, and how fast it can be pushed through a noisy wire without error. Born in a single 1948 paper by Claude Shannon, it replaced the vague notion of "information" with a number measured in bits, and then proved exactly what those bits can and cannot do.

The whole edifice rests on one idea: information is surprise. A message that you could have predicted tells you nothing; a message you did not expect tells you a lot. Make that intuition quantitative and everything else follows — the Entropy of a source, the floor on Data Compression, the capacity of a noisy channel, the redundancy needed for error correction.

The two limits Shannon proved

Information theory is anchored by two theorems that bracket every communication system ever built.

  • Source coding (compression). No lossless code can represent a source in fewer bits per symbol than its entropy. Entropy is the floor; Huffman Coding and its relatives chase it. This ties the abstract Entropy of a Probability Distribution directly to file sizes on a disk.
  • Channel coding (communication). Every noisy channel has a capacity C. Below C you can communicate with arbitrarily small error using enough redundancy; above C you cannot. The bridge between input and output is Mutual Information.

Information meets randomness and chaos

Information theory does not live alone. Its measures are expectations over a Probability Distribution, so it shares a border with Probability & Random Processes. And its deepest question — what is the shortest possible description of an object? — is Kolmogorov Complexity, which says a string is random exactly when it is incompressible. That same idea reaches into Chaos: a chaotic trajectory generates fresh, incompressible information at a rate set by its Lyapunov Exponent, so determinism and unpredictability shake hands here.

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See also