Lean, informalized

Nielsen & Chuang · Chapter 2, Introduction to quantum mechanics · p. 71

Exercise 2.24 - Nonnegative expectation values make an operator equal to its adjoint

A positive operator is Hermitian.

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The Exercise

A positive operator TT on a complex inner product space VV is a linear operator on VV whose expectation value in every vector, normalized or not, is a real, nonnegative number: ⟨v|T|v⟩≥0for every |v⟩∈V.\langle v|T|v\rangle \ge 0 \qquad \text{for every } |v\rangle \in V.(1) Density operators and projectors are positive. The exercise asks to show that every positive operator TT is Hermitian, that is, equal to its adjoint.

Hermitian and Symmetric Operators

The adjoint T†T^\dagger of a linear operator TT on a finite-dimensional VV is the linear operator on VV with ⟨w|T†|v⟩=⟨v|T|w⟩*for all |v⟩,|w⟩∈V,\langle w|T^\dagger|v\rangle = \langle v|T|w\rangle^* \qquad \text{for all } |v\rangle, |w\rangle \in V,(2) and a Hermitian, or self-adjoint, operator TT on a finite-dimensional VV is a linear operator equal to its adjoint. A symmetric operator TT on VV, of any dimension, is a linear operator whose matrix element between two vectors is the complex conjugate of the one with the two vectors exchanged.

The Claim

Theorem 1. Let TT be a positive operator (1) on a complex inner product space VV. If VV is finite-dimensional, TT is Hermitian: T†=T.T^\dagger = T.(3)✦ For VV of any dimension, TT is symmetric: ⟨w|T|v⟩=⟨v|T|w⟩*for all |v⟩,|w⟩∈V.\langle w|T|v\rangle = \langle v|T|w\rangle^* \qquad \text{for all } |v\rangle, |w\rangle \in V.(4)✦

What Is Checked

Both conclusions are checked for every positive operator on a complex inner product space, the first when the space is finite-dimensional.