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Operators, Domains, and Spectra

Infinite-dimensional quantum operators are formula–domain pairs. Formal Hermiticity or real expectation values on a convenient test domain do not establish the self-adjointness needed for a real spectral measure or unitary evolution.

On-ramp. State Vectors supplies the Hilbert-space vectors, inner products, and norm convergence used below. The operator treatment also assumes introductory functional analysis: dense subspaces, continuous linear functionals, and closed operators.

Self-Adjoint Operators is the foundation of the rigorous operator sequence. It develops:

  • dense domains, adjoints, closedness, and closures;
  • the difference between symmetric, self-adjoint, and essentially self-adjoint operators;
  • boundary forms, deficiency indices, and the extension criterion;
  • real-spectrum and resolvent consequences;
  • the links to spectral calculus and Stone’s theorem.

The central identity

A=A∗A=A^*

means equality of both action and domain. Every later occurrence of a self-adjoint observable or generator inherits that requirement.

From this chapter, two branches open:

These branches reconverge at Stone’s Theorem. Complete both before that theorem: its forward direction uses spectral calculus to construct e−itAe^{-itA}, while its converse recovers a generator from the strong derivative domain of the unitary group.

Core Formalism retains the physicist-facing warning about Hermitian versus self-adjoint operators; this chapter owns the operator-theoretic consequences used by the rigorous theorem sequence.

Additional domain, extension, form, and spectral-analysis entries are visible with Planned labels and do not yet contain articles. Use the substantive Self-Adjoint Operators treatment above for the definitions and arguments needed by the spectral and dynamical continuations.