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TheoremStatement: AI-adaptedProof: AI-generatedPipeline-generatedprecheck passverified 2026-10-22 (gpt-6.1-sol)
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Conditional mutual information and finite channel monotonicity

Statement

Let HA,HB,HC be nonzero finite-dimensional complex inner-product spaces and let ρABC be a density operator on HA⊗HB⊗HC. With dimensionless entropy S and conditional mutual information I(A:C∣B) defined by the conventions below,

I(A:C∣B)ρ=S(ρAB)+S(ρBC)−S(ρB)−S(ρABC)≥0.

Also let d,e≥1 and let Φ:Md(C)→Me(C) be a finite completely positive trace-preserving map. For all positive semidefinite X,Y∈Md(C),

D(Φ(X)∥Φ(Y))≤D(X∥Y),

where D is the support-sensitive finite-dimensional quantum relative entropy: it equals Tr⁡(Xlog⁡X)−Tr⁡(Xlog⁡Y) when supp⁡X⊆supp⁡Y, and +∞ otherwise. These are finite-dimensional mathematical statements. The channel inequality is one-sided and asserts no equality condition, recovery map, or infinite-dimensional extension.

Stinespring factorization diagram

diagram failed to render:
\begin{tikzcd}
M_d(\mathbb C)_+ \arrow[r, "X\mapsto VXV^*"] \arrow[dr, "\Phi"'] & \operatorname{End}(\mathbb C^e\otimes\mathcal E)_+ \arrow[d, "\operatorname{Tr}_{\mathcal E}"] \\
& M_e(\mathbb C)_+
\end{tikzcd}

Here Md(C)+ denotes positive semidefinite matrices, E is the finite environment constructed in step 1.2, and V is its isometry. The triangle commutes because step 1.2 computes Tr⁡E(VXV∗)=Φ(X) entrywise. The proof uses that computation and the stated partial-trace inequality, not the diagram.

Facts & Assumptions

Given: The spaces and state in the first clause of the Statement; integers d,e≥1 and the finite channel Φ in the second clause. Use natural logarithms and the ordered finite tensor conventions of the cited definitions.

[A1]

Dimensionless entropy, mutual and conditional information: I(A:C∣B)ρ=S(ρAB)+S(ρBC)−S(ρB)−S(ρABC), with each marginal formed by partial trace.

[A2]

Finite completely positive trace-preserving maps: a finite channel is a complex-linear completely positive and trace-preserving map on matrix algebras.

[F1]

Strong subadditivity of finite-dimensional quantum entropy: for a density operator on any ordered finite triple HA⊗HB⊗HC, S(ρAB)+S(ρBC)≥S(ρB)+S(ρABC).

[F2]

Partial-trace data processing for finite quantum relative entropy: for positive semidefinite R,S on a finite tensor product, D(Tr⁡ER∥Tr⁡ES)≤D(R∥S), including the extended-real support-failure cases.

[F3]

Complete finite Choi-Kraus equivalence: a finite CPTP map has a finite Kraus representation Φ(X)=∑a=1qKaXKa∗, and trace preservation entails ∑aKa∗Ka=Id.

[F4]

Partial trace over a finite tensor factor: in product bases, the partial trace over the second factor sums diagonal blocks in that factor.

[F5]

Finite-dimensional quantum relative entropy: D(R∥S) is finite on support inclusion and +∞ otherwise; the finite branch uses support-restricted spectral logarithms.

[F6]

Finite matrix spectral and state calculus: positive finite matrices have finite spectral decompositions and spectral logarithms on their positive supports; the finite trace is basis-independent and satisfies Tr⁡(AB)=Tr⁡(BA).

Proof

1.1givenA1F1

By [A1], the left side of the first assertion is the displayed four-entropy difference. Apply [F1] to the given state with the same factor order; the resulting inequality is exactly I(A:C∣B)ρ≥0.

1.2givenA2F3F4constructalgebra

By [F3], choose a finite Kraus list K1,…,Kq with ∑aKa∗Ka=Id; because d≥1, this identity rules out q=0. Let E=Cq with orthonormal basis (fa) and define V:Cd→Ce⊗E by Vx=∑aKax⊗fa. Orthogonality of the fa gives ⟨Vx,Vy⟩=∑a⟨Kax,Kay⟩=⟨x,(∑aKa∗Ka)y⟩=⟨x,y⟩, so V∗V=Id. The coordinate formula [F4] then gives Tr⁡E(VXV∗)=∑aKaXKa∗=Φ(X) for every X∈Md(C).

2.1givenF5F6step 1.2algebra

The isometry V maps each positive-eigenvalue eigenspace of X≥0 onto the corresponding eigenspace of VXV∗, with the same eigenvalue; the orthogonal complement of ran⁡V is in the kernel. Hence supp⁡(VXV∗)=V(supp⁡X), and likewise for Y. Because V is injective, support inclusion holds for X,Y exactly when it holds for VXV∗,VYV∗. If it fails, both relative entropies are +∞ by [F5]. If it holds, the support-restricted spectral logarithms satisfy log⁡(VXV∗)=V(log⁡X)V∗ and log⁡(VYV∗)=V(log⁡Y)V∗ on the corresponding supports. The trace identity in [F6] therefore yields D(VXV∗∥VYV∗)=D(X∥Y).

3.1givenF2step 1.2step 2.1algebra∎

Apply [F2] to R=VXV∗ and S=VYV∗, which are positive semidefinite because V is linear and X,Y≥0. By step 1.2 their partial traces are Φ(X),Φ(Y), and by step 2.1 their relative entropy equals D(X∥Y). Thus D(Φ(X)∥Φ(Y))≤D(X∥Y), including when the right side is +∞.

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