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.
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 sequences, so compressing to 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 -fold tensor product Hilbert space, of dimension about (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 — 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