Alphabeta Math
DefinitionDefinition: AI-adaptedProof: Not applicablePipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-22
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.

Self-adjoint, positive, unitary and normal operators

Definition

Assume the Axiom of Countable Choice, and let H be a real or complex Hilbert space with T∈B(H) a bounded linear operator and T∗ its Hilbert adjoint (The Hilbert-space adjoint of a bounded operator, The spaces (\mathcal B(X,Y)) and (\mathcal B(X)) of bounded linear operators).

  • T is self-adjoint when T∗=T;
  • T is positive when ⟨Tx,x⟩ is a real number in [0,+∞) for every x∈H;
  • T is unitary when T∗T=TT∗=I, the identity operator;
  • T is normal when T∗T=TT∗.

The definitions are read over either scalar field with the same inner product. Two immediate consequences. Every self-adjoint operator is normal, because T∗T=T2=TT∗ when T∗=T. Every unitary operator is normal, because its defining identity says exactly that T∗T and TT∗ are both the identity. Positivity is a condition on the values of the quadratic form and therefore forces those values to be real, which for a complex Hilbert space does not follow from boundedness alone; a positive operator on a complex Hilbert space is in fact self-adjoint, but that is proved later and is not assumed here.

Consistency of the vocabulary. The identity operator is self-adjoint, positive and unitary, and the zero operator is self-adjoint and positive; on the one-dimensional Hilbert space C the operator λI is self-adjoint exactly when λ is real, unitary exactly when ∣λ∣=1, and normal for every scalar λ.

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