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Memoryless quantum information source (ρ=∑x​px​∣ψx​⟩⟨ψx​∣,ρ(n)=ρ⊗n)

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2026-10-14  NaN By others on same topic  0 Discussions Create my own version
A pure-state source emits independent states from a fixed quantum state ensemble. Its average block density operator is the tensor power of the one-use average. Unassisted reliable quantum source compression preserves the emitted quantum states, rather than only their classical labels. Schumacher compression gives the optimum asymptotic qubit rate S(ρ) for such a source, with every larger rate achievable. Nonorthogonal equally likely pure states need not have entropy one: their classical labels have entropy one but their average density operator can have lower Von Neumann entropy.

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  • Past exam of the mathematics course of the University of Cambridge / 2004 / iii / Paper 32 / 5 / Solution
  • Past exam of the mathematics course of the University of Cambridge / 2007 / iii / Paper 34 / 2 / b / Solution
  • Past exam of the mathematics course of the University of Cambridge / 2008 / iii / Paper 60 / 1 / Solution

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