How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
The outcome law and outputs of a measured circuit
Definition
For a finite instrument and input density operator , define the unnormalized branch output and probability . The family is a probability distribution by Instrument outcome weights normalize. Its uniquely induced POVM satisfies by Every finite instrument induces a unique POVM and the outcome-law definition in Finite POVMs and their outcome law.
The conditional branch output is when and is when , exactly as specified by Finite instruments and conditional states. No normalized state is assigned to a zero-probability branch. A Kraus representation is only a representation of the observed branch map: is the outcome and is not an additional observed outcome.
Facts & Assumptions
Given: A finite instrument, a density operator on its input space, and its finite outcome set .
Finite instruments and conditional states: , , and a conditional output is assigned only for .
Instrument outcome weights normalize: the weights are nonnegative and sum to one.
Every finite instrument induces a unique POVM: each branch weight equals the induced POVM weight .
Finite POVMs and their outcome law: a POVM assigns weights and does not specify a conditional output state.
Proof
The branch output is the unnormalized operator , and its trace is the branch weight , by [F1].
The weights form a finite probability law by [F2], and the same law is by [F3] and [F4]. This establishes consistency of the instrument and POVM descriptions.
If , the conditional output is defined by division by that positive scalar; if , [F1] assigns and no division is made. The finite Kraus index remains internal to and is not part of .
Depends on
Used by
Dependency tree · two levels
22 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- John Preskill, Quantum Computation, Chapter 3: Foundations II: Measurement and Evolution (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, arXiv:1907.09415v6 (standard reference, not scraped)