Typicality and Quantum Source Compression

Stub. Typical sequences and Shannon's source coding theorem as the classical baseline (compressing a classical i.i.d. source down to its entropy rate), then quantum source compression — Schumacher's theorem — doing the same for a source emitting quantum states, via a quantum analogue of the typical subspace.

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Corresponds to Lectures 15–16. Reviews the classical asymptotic equipartition property and Shannon’s source coding theorem (asymptotic-equipartition-property covers this in full) as the model to generalize: almost all the probability mass of a long i.i.d. sequence concentrates on a typical set of about 2nH2^{nH} sequences, so compressing to nHnH bits loses negligible fidelity. Quantum source compression (Schumacher compression) asks the same question when the source emits quantum states rather than classical symbols: there’s a typical subspace of the full nn-fold tensor product Hilbert space, of dimension about 2nS(ρ)2^{nS(\rho)} (the von Neumann entropy from the previous note), that carries almost all of the source’s quantum information, so projecting onto it and re-encoding gives a compression scheme with fidelity approaching 1 as n→∞n\to\infty — the direct quantum counterpart of Shannon’s theorem, with von Neumann entropy playing the role Shannon entropy played classically.

Outline (TODO — flesh out each)

  • Typicality and Shannon source compression (classical review)
  • Quantum source compression — the typical subspace
  • Schumacher’s theorem

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