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Nielsen & Chuang · Chapter 2, Introduction to quantum mechanics · p. 74

Exercise 2.31 - Positive operators on two systems give a positive operator on the composite system

Tensor products of positive operators are positive.

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The Exercise

Two quantum systems have state spaces VV and WW, complex inner product spaces, and the composite system has state space V⊗WV \otimes W. An operator AA on the first system and an operator BB on the second give the operator A⊗BA \otimes B on the composite system. The exercise asks to show that if AA and BB are positive, so is A⊗BA \otimes B.

Positive Operators and Tensor Products

An operator TT on a complex inner product space ℋ\mathcal{H} is positive if, for every vector |φ⟩|\varphi\rangle of ℋ\mathcal{H}, ⟨φ|T|φ⟩≥0.\langle \varphi | T | \varphi \rangle \ge 0 .(1)

The space V⊗WV \otimes W is spanned by the product vectors |v⟩⊗|w⟩|v\rangle \otimes |w\rangle, whose inner products are ⟨v⊗w|v′⊗w′⟩=⟨v|v′⟩⟨w|w′⟩\langle v \otimes w | v' \otimes w' \rangle = \langle v | v' \rangle \langle w | w' \rangle.

The tensor product A⊗BA \otimes B of an operator AA on VV and an operator BB on WW is the operator on V⊗WV \otimes W that acts on product vectors as (A⊗B)(|v⟩⊗|w⟩)=A|v⟩⊗B|w⟩(A \otimes B)\bigl(|v\rangle \otimes |w\rangle\bigr) = A|v\rangle \otimes B|w\rangle(2) and on the rest of V⊗WV \otimes W by linearity.

The Claim

Theorem 1. Let VV and WW be complex inner product spaces, AA a positive operator on VV and BB a positive operator on WW. Then for every vector |ψ⟩|\psi\rangle of V⊗WV \otimes W, ⟨ψ|(A⊗B)|ψ⟩≥0.\langle \psi | (A \otimes B) | \psi \rangle \ge 0 .(3)✦

What Is Checked

The claim is stated over two complex inner product spaces VV and WW, a positive operator on each in the sense of (1), and their tensor product (2), an operator on V⊗WV \otimes W. What the library proves about these constructions is the inequality (3).