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.
Projective measurement outcome weights are probabilities
Statement
Let be a density operator on a nonzero finite-dimensional complex inner-product space , and let be a finite projective measurement on . Then lies in for every , and .
Facts & Assumptions
Given: The density operator and the finite projective measurement stated above.
Finite projective measurements: , for , and ; zero projections are allowed.
Density operator: on a nonzero finite-dimensional complex inner-product space, a density operator is nonnegative and has trace one.
Non-negative and positive operators: a nonnegative operator is self-adjoint and has nonnegative quadratic form on every vector.
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.
For and , : for compatible rectangular matrices.
Trace is a linear functional on : trace preserves finite sums and scalar multiples.
The basis-independent trace of an endomorphism of a finite-dimensional vector space: endomorphism trace is the matrix trace in any basis and is basis-independent.
Proof
Fix . Set . Self-adjointness of and gives for all , so is self-adjoint. It is nonnegative, since for every by [F6]–[F7]. By [F2], has nonnegative diagonal entries in an orthonormal basis, so [F5] gives . By [F3] and , .
By [F4], the resolution of the identity in [F1], and [F6], .
For each , by step 1.1, with the empty sum interpreted as when . Therefore every weight is at most one and, by step 1.1, belongs to .
Depends on
- Finite projective measurements
- Density operator
- Non-negative and positive operators
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- Trace is a linear functional on $M_n(F)$
- For $A\in M_{m\times n}(F)$ and $B\in M_{n\times m}(F)$, $\operatorname{tr}(AB)=\operatorname{tr}(BA)$
- 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
Used by
- Amplitude amplification with a fixed integer iteration count Algorithm
- Amplitude amplification with independently chosen phase rotations Algorithm
- Exact success amplification by attenuating the good branch Algorithm
- Known-amplitude amplification with integer rounding Algorithm
- Power-of-two dihedral hidden-subgroup sieve Algorithm
- Quantum phase estimation Algorithm
- Szegedy-walk marked-set detection Algorithm
- Unknown-amplitude randomized search Algorithm
- Coherent variable-time algorithm model Definition
- Finite adiabatic path model Definition
- Prepared unitary and success subspace for amplitude amplification Definition
- QAOA circuit and expected combinatorial objective Definition
- Symmetric and antisymmetric swap-test measurement Definition
- A projective measurement branch with probability zero Example
- One-bit feed-forward and deferred measurement Example
- VQE and MaxCut-QAOA objective calculation Example
- Amplitude-amplification invariant plane Lemma
- Dihedral hidden-state pair combination Lemma
- Finite amplification preserves the good state with a deterministic call cap Lemma
- Fourier sample from a generalized-dihedral reflection coset state Lemma
- Phase-estimation finite outcome law Lemma
- Conditional state for a projective measurement Theorem
- CSS syndrome correction Theorem
- Dense-coding correctness and resources Theorem
- Element-distinctness gate cost in the QRAM model Theorem
- Exact success for known positive amplitude with explicit dilution Theorem
- Exact success probability after amplitude amplification Theorem
- Fingerprint swap-test error and communication cost Theorem
- Finite Naimark isometric compression Theorem
- Finite reversible-walk finding cost Theorem
- Fusion measurement branches are normalized exactly when nonzero Theorem
- Phase estimation on a superposition of eigenspaces Theorem
- QAOA objective is an expected feasible score only Theorem
- QPE output law and conditional state for a spectral input Theorem
- Success bound under an explicit amplitude-amplification phase mismatch Theorem
- Swap-test measurement and pure-state outcome law Theorem
- Teleportation outcomes are equiprobable Theorem
- Teleportation preserves a finite reference Theorem
- The measurement law for a finite continuous-time walk Theorem
- Unknown-amplitude search has no false positives and halts almost surely Theorem
…and 1 more result.
Cited to discharge well-definedness by Finite projective measurements.
Dependency tree · two levels
30 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), §§2.3.1–2.3.2 (standard reference, not scraped)
- John Preskill, Quantum Computation, Chapter 3: Foundations II: Measurement and Evolution, §3.1.1 (standard reference, not scraped)