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.
Zero-probability Pauli measurement branch
Statement
Let be a nonzero finite-dimensional complex inner-product space, let be a density operator on , and let be a Hermitian Pauli observable on with . For put and . If , then . The outcome has probability zero and, under the conditional-state convention, has no normalized conditional state.
Facts & Assumptions
Given: The data of the Statement, with .
The setup defines and .
Density operator: is a nonnegative endomorphism on a nonzero finite-dimensional complex inner-product space.
For and , : trace is cyclic for compatible finite-dimensional endomorphisms.
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 endomorphism has an orthonormal eigenbasis with nonnegative real eigenvalues.
The basis-independent trace of an endomorphism of a finite-dimensional vector space: trace is basis-independent and equals the matrix trace in any ordered basis.
Proof
Given: The data in the Statement.
Set . For every , self-adjointness of in [F2] gives by [A1]. Thus is nonnegative.
By [F1], [F2], and cyclicity [F3], . By [F4], choose an orthonormal eigenbasis of whose eigenvalues are nonnegative; [F5] expresses its trace as their finite sum. A finite sum of nonnegative reals is zero only when each term is zero, so .
The branch output is therefore zero. Normalization would require dividing it by , which is undefined; the conditional-state convention assigns no state to this zero-probability outcome.
Sources
De Wolf §20.3, PDF pp. 187–188, separates deterministic outcomes from random outcomes; Watrous Lesson 14 §14.1, printed pp. 405–407 (PDF pp. 411–413), specifies the two projective branches. The zero-trace implication is proved locally using the finite spectral theorem.
Depends on
- Pauli measurement branch semantics
- Density operator
- The trace $\operatorname{tr}(A)$ as the sum of the diagonal entries
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- Pauli measurement projectors and total probability
- 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
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
- Ronald de Wolf, Quantum Computing: Lecture Notes, §20.3 (standard reference, not scraped)
- John Watrous, Understanding Quantum Information and Computation, Lesson 14 (standard reference, not scraped)