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.
Instrument outcome weights normalize
Statement
For a finite instrument and a density operator on its input space, the branch weights form a probability distribution on .
Facts & Assumptions
Given: A finite instrument and an input density operator .
Finite instruments and conditional states: each outcome map is completely positive and for every input operator ; .
Completely positive maps: complete positivity includes the extension, which is the original map and therefore preserves nonnegativity.
Density operator: on a nonzero finite-dimensional complex inner-product space, a density operator is nonnegative and has trace one.
A non-negative operator is equivalently self-adjoint with nonnegative eigenvalues, a positive semidefinite matrix in an orthonormal basis, or an operator of the form S^*S: a nonnegative operator has an orthonormal basis in which its matrix is diagonal with nonnegative real diagonal entries.
The basis-independent trace of an endomorphism of a finite-dimensional vector space: trace is the basis-independent matrix trace of a finite-dimensional endomorphism.
Non-negative and positive operators: a nonnegative operator is self-adjoint and has nonnegative quadratic form on every vector.
Proof
For each , complete positivity [F1]–[F2] at sends the nonnegative input from [F5] to a nonnegative in the sense of [F6]. By [F3], has nonnegative diagonal entries in an orthonormal basis, and [F4] therefore gives .
Apply the trace-preservation identity in [F1] to . It gives by [F5]. Thus the nonnegative branch weights sum to one.
For any , by step 1.1, including the empty sum when . Hence for every outcome, and the weights form a finite probability distribution.
Depends on
- Finite instruments and conditional states
- Density operator
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- A non-negative operator is equivalently self-adjoint with nonnegative eigenvalues, a positive semidefinite matrix in an orthonormal basis, or an operator of the form S^*S
- Completely positive maps
- Non-negative and positive operators
Used by
- One Simon Fourier-sampling sample Algorithm
- Finite authenticated key-distribution protocol Definition
- Finite measurement branches and classical control Definition
- Heralded success and conditional verification contract Definition
- Normalized output law for finite quantum query branches Definition
- Oracle-only bit-query algorithm Definition
- The outcome law and outputs of a measured circuit Definition
- Positive-probability instrument branches are density operators Theorem
- Simon query and output measurement produce a coset pair Theorem
- The nonselective output of an instrument is a density operator Theorem
Cited to discharge well-definedness by Finite instruments and conditional states.
Dependency tree · two levels
24 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 Watrous, The Theory of Quantum Information (2018), §2.3.2 (standard reference, not scraped)
- John Preskill, Quantum Computation, Chapter 3: Foundations II: Measurement and Evolution, §3.2.4 (standard reference, not scraped)