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 selective Lueders update by an orthogonal projection
Statement
Assume the Axiom of Countable Choice (The Axiom of Countable Choice ()). Let be a nonzero complex Hilbert space (Hilbert space), let be an orthogonal projection on (The Hilbert orthogonal projection onto a closed subspace) and let be a density operator with (Density operators and scalar spectral probability clause (a)). Define the selective update Then:
(a) is a positive trace-class operator with , so is a density operator;
(b) and in particular commutes with and is fixed by compression with ;
(c) if is an orthogonal projection with , then and ;
(d) if for a unit vector with , where (Rank-one operator calculus), then , the pure state of the normalized vector ; the value depends only on the ray of , meaning its equivalence class of nonzero vectors under if for some .
No physical interpretation of the update is asserted.
Facts & Assumptions
Given: A nonzero complex Hilbert space ; an orthogonal projection on ; a density operator with ; an orthogonal projection with ; a unit vector with .
Orthogonal projections. An orthogonal projection on is a bounded linear operator with , and for all (The Hilbert orthogonal projection onto a closed subspace).
Density operators. A density operator is self-adjoint, positive and trace class with , and it admits an expansion with a finite or countable orthonormal family and weights , (Density operators and scalar spectral probability clause (a)).
Rank-one calculus. is trace class with and ; for bounded one has and (Rank-one operator calculus clauses (b)-(d)). For any , and , so is positive under the general Hilbert-space definition (Self-adjoint, positive, unitary and normal operators).
Trace-class ideal and cyclicity. If is trace class and bounded, then and are trace class with and linear and trace-norm continuous (Trace class is a two sided Banach operator ideal, Nuclear bounded cyclicity for trace-class operators clause (b)).
Positivity of quadratic forms. If is positive on the Hilbert space , then for every ; sums of positive operators are positive, and with is a density operator (Self-adjoint, positive, unitary and normal operators, [F2], [F3]).
Proof
[The unnormalized update] Since and by [F1] and [F2], , so is self-adjoint. For , by [F1] and [F5], so . With bounded and trace class, and then are trace class by [F4], and by cyclicity [F4] and [F1].
[Clause (a)] Since , the operator is self-adjoint and positive with trace , hence a density operator by [F2]; this is (a).
[Clause (b)] By and cyclicity [F4], . Moreover and ; thus commutes with and is fixed by compression with . This is (b).
[Clause (c)] If then as an operator identity, and by cyclicity [F4]. This is (c).
[Clause (d)] Let with . By [F3], , whose trace is , and by [F3] and cyclicity [F4]; hence . For the identity from the conjugate-linearity of [F3] shows that the state depends only on the ray of . This is (d).
Depends on
The Axiom of Countable Choice ()
The Hilbert orthogonal projection onto a closed subspace
Hilbert space
Self-adjoint, positive, unitary and normal operators
Trace class operator
Trace of a trace class operator
Density operators and scalar spectral probability
Nuclear bounded cyclicity for trace-class operators
Rank-one operator calculus
Trace class is a two sided Banach operator ideal
Dependency tree · 2 levels
Sources
- J. Preskill, Lecture Notes for Ph219/CS219: Quantum Information, Chapter 3 'Foundations II: Measurement and Evolution' (updated July 2015), Section 3.1.2, printed pages 8-11 (measurement operators, outcome probabilities (3.26)-(3.29) and post-measurement states (3.27))
- D. Tong, Quantum Mechanics (author-hosted lecture set), Section 3.3, printed pages 76-77 (Born rule, collapse and the degenerate-spectrum update)