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.
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- 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.
A zero-probability instrument branch has no conditioned state
Statement
Let be a finite instrument and let be an input density operator. If , then and the conditional value for outcome is , not a density operator.
Facts & Assumptions
Given: A finite instrument, an input density operator , and an outcome whose branch weight is zero.
Finite instruments and conditional states: , and the conditional value is when .
Completely positive maps: each finite-ancilla extension of a completely positive branch map preserves nonnegative operators.
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 it 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 sum of the diagonal entries in any chosen basis.
Non-negative and positive operators: a nonnegative operator is self-adjoint and has nonnegative quadratic form on every vector.
Proof
Since is completely positive, its extension sends the nonnegative from [F5] to the nonnegative operator by [F2], with nonnegativity as defined in [F6]. By [F3], is diagonal with entries in an orthonormal basis. Its trace is by the hypothesis and [F1], [F4]; a finite sum of nonnegative numbers is zero only when every . Hence .
The instrument definition [F1] assigns when . The algebraic quotient would have zero denominator, so it is not a normalized conditional density state.
Depends on
- Finite instruments and conditional states
- Completely positive maps
- 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
- Density operator
- Non-negative and positive operators
Used by
Dependency tree · two levels
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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)