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Norm-continuous finite channel semigroups are GKSL

Statement

Let d≥1 and let Tt:Md(C)→Md(C), t≥0 measured in seconds, be a semigroup of finite channels, so T0=id⁡ and Tt+s=Tt∘Ts. Assume t↦Tt is continuous in the induced operator norm on the finite-dimensional space of linear maps Md(C)→Md(C). For a bounded operator A on a complex Banach space, write etA:=∑n=0∞tnAn/n! for the operator-norm convergent exponential series of The exponential series of a bounded operator. Then there is a unique linear generator L, in s−1, with Tt=etL, and L has the finite GKSL form in Finite GKSL generators and units with at most d2−1 jump matrices. Conversely, every such finite GKSL generator produces a norm-continuous channel semigroup, as in Finite GKSL generates CPTP semigroups.

Facts & Assumptions

Given: d≥1, the finite channel definition, a norm-continuous semigroup Tt with T0=id⁡, and ℏ>0 in the units of the GKSL definition.

[F1]

Finite completely positive trace-preserving maps: each Tt is completely positive and trace-preserving.

[F2]

Finite GKSL generators and units: the finite GKSL form is −iℏ[H,X]+∑a(LaXLa∗−12{La∗La,X}) with H=H∗.

[F3]

Finite matrix spectral and state calculus: finite Hermitian matrices have real spectral decompositions and positive matrices have positive square roots.

[F4]

Complete finite Choi-Kraus equivalence: a finite map is completely positive exactly when its Choi matrix is positive, and every finite CP map has a Kraus form.

[F5]

Finite GKSL generates CPTP semigroups: every finite GKSL generator has a norm-continuous semigroup of channels for t≥0, with the operator exponential defined by its norm-convergent series.

[F6]

Every finite-dimensional normed space is Banach: every finite-dimensional real or complex normed space is complete.

[F7]

Riemann integration of continuous curves in a complete normed space, with the fundamental theorem of calculus and coefficient functionals: a continuous curve into a complete normed real vector space has a norm-Riemann integral, its indefinite integral differentiates to the curve, and bounded-interval integrals are additive.

[F8]

Finite matrix trace cyclicity and nondegeneracy: setting the rectangular dimensions equal gives square trace cyclicity.

[F9]

The exponential series of a bounded operator: the operator-norm exponential series satisfies E(0)=I, E′(t)=AE(t)=E(t)A, and E(t+s)=E(t)E(s), with the stated quadratic remainder bound.

Proof

1.1givenF6F7algebra

Let E=End⁡C(Md(C)) with its induced operator norm. It has finite complex dimension d4, so its underlying real normed space is complete by [F6]. For small h>0, set Ah=h−1∫0hTs ds, using [F7]. The integral norm bound in [F7] and norm continuity at zero give ∥Ah−I∥≤sup⁡0≤s≤h∥Ts−I∥→0; hence ∥I−Ah∥<1 for sufficiently small h. The series BN:=∑k=0N(I−Ah)k is Cauchy in the finite-dimensional complete map space: the induced operator norm is submultiplicative, so ∥(I−Ah)k∥≤∥I−Ah∥k, and the geometric series converges to a limit B. The telescoping identities AhBN=BNAh=I−(I−Ah)N+1 pass to the limit, so AhB=BAh=I and Ah is invertible. The semigroup law gives TtAh=h−1∫tt+hTu du. By additivity and the fundamental theorem [F7], this moving integral has derivative (Tt+h−Tt)/h for t>0, and the same right derivative at t=0. Right multiplication by Ah−1 yields Tt′=TtGh, where Gh=(Th−I)Ah−1/h, with right derivative Gh at zero. Since that right derivative is unique, Gh is independent of all sufficiently small h; set L=Gh.

2.1step 1.1F9algebra

For t>0, differentiating the product in step 1.1 gives ddt(Tte−tL)=TtLe−tL−TtLe−tL=0; [F9] supplies the derivative and initial value of the matrix exponential. Continuity at zero gives T0e0=I, so Tte−tL=I and Tt=etL. Any generator of this semigroup must equal its right derivative at zero, so L is unique.

2.2givenF1F3step 1.1algebra

Each Tt preserves adjoints: it is positive by [F1], and every Hermitian matrix is a difference of two positive matrices by [F3]. Taking the right derivative at zero shows L(X∗)=L(X)∗. Differentiating Tr⁡(TtX)=Tr⁡X also gives Tr⁡(L(X))=0 for every X. Consequently J(L) is Hermitian: J(L)∗=∑i,jEji⊗L(Eij)∗=∑i,jEji⊗L(Eji)=J(L) after reindexing.

3.1givenF3F4F9step 2.1step 2.2algebra

Let Ω=∑i=1d∣i⟩⊗∣i⟩. By [F4], J(Tt)≥0, and step 2.1 together with the quadratic remainder in [F9] gives J(Tt)=∣Ω⟩⟨Ω∣+tJ(L)+o(t). For every v⊥Ω, dividing ⟨v,J(Tt)v⟩≥0 by t>0 and taking t↓0 gives ⟨v,J(L)v⟩≥0. Put e=Ω/d, Q=I−∣e⟩⟨e∣, M=QJ(L)Q, z=QJ(L)e, and a=⟨e,J(L)e⟩∈R. Then M≥0, and the block decomposition relative to Ce⊕e⊥ is J(L)=M+∣e⟩⟨z∣+∣z⟩⟨e∣+a∣e⟩⟨e∣.

4.1step 3.1F3F4algebra

By [F3], write M=∑b=1q∣wb⟩⟨wb∣, where q=rank⁡M≤d2−1, absorbing each positive eigenvalue into its eigenvector. Define Lb by wb=∑i∣i⟩⊗Lb∣i⟩, and define K by k:=∑i∣i⟩⊗K∣i⟩=z/d+(a/(2d))Ω. Direct expansion of J(Θ)=∑ijEij⊗Θ(Eij) gives J(X↦LbXLb∗)=∣wb⟩⟨wb∣, J(X↦KX)=∣k⟩⟨Ω∣, and J(X↦XK∗)=∣Ω⟩⟨k∣. The latter two sum to ∣e⟩⟨z∣+∣z⟩⟨e∣+a∣e⟩⟨e∣. Equality of Choi matrices gives equality on every input matrix unit because its (i,j) block is Θ(Eij); linearity then gives equality on all matrices. Thus L(X)=∑bLbXLb∗+KX+XK∗.

5.1givenF2F8step 4.1algebra

Taking traces in step 4.1 and using finite cyclicity [F8] gives Tr⁡(X(K+K∗+∑bLb∗Lb))=0 for every X. Testing on all matrix units forces K+K∗+∑bLb∗Lb=0. Set H=(iℏ/2)(K−K∗); then H=H∗ and K=−12∑bLb∗Lb−iH/ℏ. Substitution into step 4.1 gives the finite GKSL form in [F2] with at most d2−1 jumps.

6.1F5∎

Conversely, [F5] gives a norm-continuous channel semigroup from every finite GKSL generator.

Depends on

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