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The factorized zero-state step is well-defined, nonnegative, conservative, and locally first order

Statement

Let a finite conservative PDS have a source-factored representation on an open neighborhood U⊆Ω of a compact set K⊆[0,∞)m, with factors that are multivariable C2 on U and nonnegative on U∩[0,∞)m, as in Source-factored transfer rates for zero compartments. For every yn∈K and h>0, Zero-compatible modified Patankar Euler in rate-factor form has a unique output yn+1≥0 and conserves ∑iyi. For the accuracy clause, fix a compact set K∗⊂U containing K and all exact solution segments under consideration, and define the C2 extension F~i(y):=∑j≠i(yjaij(y)−yiaji(y)) on U. If those exact segments remain in K∗∩[0,∞)m, then the exact-start local defect is uniformly O(h2) as h↓0, including when some coordinates of yn are zero. The claim is local; no global error bound at the boundary is asserted.

Facts & Assumptions

Given: A finite conservative PDS, a source-factored representation on a neighborhood of K, yn∈K⊆[0,∞)m, h>0, and the fixed compact tube K∗⊂U from the defect clause when local accuracy is asserted.

[F1]

Finite conservative production destruction systems: Fi(y)=∑j≠i(pij(y)−dij(y)) and the pair rates satisfy pij=dji.

[F2]

Source-factored transfer rates for zero compartments: pij(y)=yjaij(y) and dij(y)=yiaji(y) with C2 factors that are nonnegative on admissible nonnegative states, including at zero coordinates.

[F3]

Zero-compatible modified Patankar Euler in rate-factor form: the output solves (I−hB(yn))yn+1=yn, where Bij=aij for i≠j and Bjj=−∑i≠jaij.

[F4]

Strict column dominance gives an entrywise nonnegative inverse: a strict column-diagonally-dominant matrix with positive diagonal and nonpositive off-diagonal entries has an entrywise nonnegative inverse.

[F5]

First-order systems, initial value problems, and solutions on intervals: an exact trajectory satisfies y′=F(y) on its interval.

[F7]

Chain sum product and composition rules for Banach derivatives and The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a): products of differentiable coordinate maps obey the bounded-bilinear product rule, and composition obeys the total chain rule.

[F8]

Multivariable Taylor formula with a Lagrange remainder along a line segment: a C2 solution curve on a time interval has a first-order Taylor expansion with remainder bounded by its second derivative on that interval.

[F9]

One-step ODE methods, local defect, uniform order, and step stability: the exact-start local defect is the method output minus the exact next state.

Proof

1.1givenF2F3F4algebra

For each column j, Bjj=−∑i≠jaij≤0, Bij=aij≥0 off the diagonal, and ∑iBij=0. Therefore M:=I−hB(yn) has Mjj=1+h∑i≠jaij(yn)>0, Mij=−haij(yn)≤0 for i≠j, and Mjj−∑i≠j∣Mij∣=1. By [F4], M−1≥0; hence the unique solution yn+1=M−1yn exists and is nonnegative, including for zero coordinates in yn.

2.1F3step 1.1algebra

The column sums of M equal one, so ∑iyin=∑i(Myn+1)i=∑j(∑iMij)yjn+1=∑jyjn+1.

2.2F1F2F3algebra

The factorization [F2] gives B(y)y=F(y) for every y∈K: its i-th component is ∑j≠iaij(y)yj−yi∑j≠iaji(y)=∑j≠i(pij(y)−dij(y)). The matrix identity used in step 1.1 also gives (I−hB(y))−1=I+hB(y)+h2B(y)2(I−hB(y))−1.

3.1givenF2F5F6F7F8F9step 2.2algebra∎

The factors are C2 on U, so the coordinate products yjaij(y) and yiaji(y) have continuous partial derivatives through order two by applying the bounded-bilinear product rule [F7] twice. Applying the continuous-partials theorem [F6] to these components and their first partials shows that F~ is C2 and has continuous first total derivative on U. On the compact set [0,h0]×K of admissible nonnegative starting states, B is bounded and I−hB(yn) is invertible by step 1.1 for h>0 and equals I at h=0. Its inverse is continuous there, hence uniformly bounded for sufficiently small h. The matrix identity from step 2.2 then yields yn+1=yn+hF(yn)+O(h2) uniformly, without dividing by any coordinate of yn. On the nonnegative exact path, the PDS field equals the C2 extension F~ defined in the Statement, so [F5]–[F7] give y′=F~(y) and bounded y′′=DF~(y)F~(y) on K∗. Applying [F8] to the time curve gives the same expansion uniformly. Their difference is therefore O(h2) uniformly, which is the local-defect bound specified by [F9].

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