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One-jump span in the nine-dimensional lowering model

Statement

Consider the purely finite-matrix model on C9 with the specified orthonormal basis eJ,m, J=0,1,2, m=−J,…,J, using the finite operator and adjoint conventions. Let γ>0, Δ∈R, and E0,E1,E2∈R. For J=1,2, let bJ,m,q be the normalized downward coefficients of the low-spin support lemma. Define HeJ,m=(EJ+ΔJm)eJ,m. For each q∈{−1,0,1}, define Lq by LqeJ,m=γbJ,m,qeJ−1,m+q when J∈{1,2} and ∣m+q∣≤J−1, and by LqeJ,m=0 otherwise, including J=0; extend these basis assignments complex-linearly. Put G=−iH−∑q=−11Lq†Lq/2, D(u)=euG. At every t>0, the complex linear span of D(t−s)LqD(s) for q=−1,0,1, 0<s<t, has dimension six if Δ=0, and twelve if Δ≠0.

Facts & Assumptions

[F1]

The coefficients are nonzero at every allowed downward entry and their squared sums equal one. Nonvanishing downward coefficients for spin one and two

[F2]

Distinct complex exponential profiles on any positive-length interval are independent. Distinct complex exponentials have full interval Gram rank

[F3]

The one-jump amplitude in the finite GKSL expansion is D(t−s)LqD(s). Finite no-jump and ordered-jump expansion

[F4]

The specified orthonormal coordinates identify operators with complex matrices; the adjoint is the conjugate transpose, and products use matrix multiplication. Finite operator and ket conventions

[F5]

An inner product on a complex vector space induces the norm ∥x∥=⟨x,x⟩. The induced length is a norm

[F6]

A real or complex normed space admitting an ordered basis of finite length is Banach. Every finite-dimensional normed space is Banach

[F7]

A linear map between normed spaces over the same scalar field is bounded when its domain admits an ordered basis of finite length. A linear map from a finite-dimensional normed space is bounded

[F8]

For a bounded linear operator A on a real or complex Banach space, euA=∑n=0∞unAn/n! converges absolutely in operator norm for real u, and these exponentials satisfy euAevA=e(u+v)A and e0A=I. The exponential series of a bounded operator

[F9]

In a complex vector space, the span of a family is the smallest complex linear subspace containing it. The dimension over C of a space with a finite basis is the number of vectors in such a basis. Linear combination of a finite list, and the span span(S) as the smallest linear subspace containing S Finite-dimensional vector space, and its dimension dim_F V; infinite-dimensional means having no finite basis

[F10]

For z∈C, write ez=exp⁡z=∑n=0∞zn/n!, using the complex exponential defined by its everywhere-convergent power series. The complex exponential by its power series

[F11]

If ∑an=A and ∑bn=B converge absolutely in C, their Cauchy product with coefficients cn=∑k=0nakbn−k converges absolutely to AB. The Cauchy product of two absolutely convergent complex series converges absolutely to the product of their sums

Proof

Given: The finite data and hypotheses in the Statement.

Goal: Establish the asserted complex span dimensions.

1.1givenF1F3F4algebra

In the matrix conventions [F4], the zero assignments exclude every forbidden transition. Orthogonality of the nonzero outputs at fixed q and [F1] give ∑qLq†Lq=γPexc, where Pexc projects onto J=1,2. Thus GeJ,m=gJ,meJ,m, where g0,0=−iE0 and gJ,m=−γ/2−i(EJ+ΔJm) for J=1,2. The real diagonal entries of H make it Hermitian, and the three Lq are finite matrices, as required by [F3].

2.1F4F5F6F7F8F10F11step 1.1algebra

Give X=C9 the induced norm ∥x∥2=∑J,m∣xJ,m∣2. This is a complex norm by [F4] and [F5], and the specified nine-vector ordered basis makes X Banach by [F6]. Matrix multiplication makes G:X→X complex-linear, so [F7] makes it bounded. Apply [F8] with A=G. Since GneJ,m=gJ,mneJ,m for every n≥0, evaluating its partial sums on eJ,m and passing to the limit gives D(u)eJ,m=eugJ,meJ,m for real u; evaluation is continuous because ∥BeJ,m∥2≤∥B∥ in the induced operator norm. For the scalar series, apply [F5]--[F8] to C with basis (1) and the complex-linear map Mz(w)=zw. Since ∥Mzn∥=∣z∣n, [F8] at real parameter 1 gives absolute convergence of ∑zn/n!, and evaluation of the operator partial sums at 1 identifies their limit with ez in [F10]. The group identity for Mz at real parameters 1,−1 gives eze−z=1. For arbitrary complex z,w, both scalar series converge absolutely by this specialization, so [F11] applies with an=zn/n! and bn=wn/n!. Its coefficient is cn=∑k=0nzkwn−k/(k!(n−k)!)=(z+w)n/n! by finite binomial expansion. Therefore ezew=∑n=0∞(z+w)n/n!=ez+w by [F10].

3.1givenF1F3F4step 1.1step 2.1algebra

Each allowed (J,m)→(J−1,m+q) coordinate of [F3] is γbJ,m,qegJ−1,m+qte(gJ,m−gJ−1,m+q)s, with nonzero prefactor. Indeed step 2.1 evaluates the two diagonal propagators, its scalar product identity combines their factors, and [F1] together with γ>0 makes the remaining coefficient nonzero.

4.1F1F2F4F9step 1.1step 3.1algebra∎

For a fixed q there is one J=1 entry, namely m=−q, with exponent of real part −γ/2. There are three J=2 entries, with m=−1−q,−q,1−q, each with exponent −i(E2−E1+Δ(m−q)) of real part zero. At Δ=0 the latter three share one exponent, distinct from the J=1 exponent by its real part, giving dimension two by [F2]. At Δ≠0 their imaginary parts are distinct, and all four exponents are distinct, giving dimension four. Different q have disjoint matrix-unit supports: the union of bases for their spans is independent and spans the full family. Its size gives dimension six or twelve in the sense of [F9].

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