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.
Bloch-ball representation of a qubit density matrix
Statement
Every Hermitian trace-one matrix has a unique vector such that
Conversely, for every this formula defines a Hermitian trace-one matrix, and that matrix is positive semidefinite exactly when , where is the Euclidean norm defined in Pauli matrices and the two-qubit exchange operator. Thus the one-qubit density matrices of Finite two-qubit density matrices and separability are exactly the displayed matrices with . Their coordinates are .
Facts & Assumptions
Given: The Pauli matrices and trace convention of Pauli matrices and the two-qubit exchange operator, and the definition of a one-qubit density matrix in Finite two-qubit density matrices and separability.
Pauli matrices and the two-qubit exchange operator: the Pauli matrices are the displayed Hermitian matrices; , , and matrix trace is the sum of diagonal entries.
Finite two-qubit density matrices and separability: a one-qubit density matrix is Hermitian, positive semidefinite, and has trace one.
Proof
Write , where because is Hermitian and the lower diagonal entry is fixed by . Set , , and . Direct substitution of the displayed Pauli matrices gives . Direct multiplication gives for each , so the entries of force uniqueness and each coefficient is real.
The constructed matrix is with , , and . Its quadratic form at is . If , completing the square gives , so positivity is equivalent to . If , positivity forces (otherwise choosing and for sufficiently large makes the quadratic form negative), and then is equivalent to . In both cases the criterion is and . Here . Thus implies the criterion, and the criterion implies . Hence is positive semidefinite exactly on the closed unit ball.