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A solvable Padé moment system gives the stated Taylor order

Statement

Let m,n≥0, R>0, and f(z)=∑k=0∞ckzk for ∣z∣<R, with the series convergent there. Suppose q0=1,q1,…,qn solve the full normalized Padé moment equations of Exact Padé coefficient matching with defect statuses. Define pk=∑j=0min⁡(k,n)qjck−j for 0≤k≤m, and p(z)=∑k=0mpkzk, q(z)=∑j=0nqjzj. Then

f(z)−p(z)q(z)=O(zm+n+1)as z→0.

This is a local Taylor-matching statement only; it gives no pole-location claim and no guarantee about analytic continuation beyond the neighborhood where f is given.

Here h(z)=O(zM) as z→0 means there are constants C,δ>0 such that ∣h(z)∣≤C∣z∣M whenever 0<∣z∣<δ.

Facts & Assumptions

Given: Integers m,n≥0, a radius R>0, a convergent power series f(z)=∑k=0∞ckzk for ∣z∣<R, and a normalized denominator solution q0=1,q1,…,qn.

[F1]

Exact Padé coefficient matching with defect statuses: the moment equations make coefficients of qf vanish in degrees m+1,…,m+n, while pk equals the coefficient of qf for 0≤k≤m.

[A1]

Since q(0)=q0=1, continuity gives a neighborhood of 0 on which ∣q(z)∣≥1/2, so 1/q is bounded there.

Proof

1.1givenF1algebra

Multiplication of the Taylor series of f by q gives coefficient ∑j=0min⁡(k,n)qjck−j at degree k. By [F1], for each 0≤k≤m this coefficient is pk, so the coefficients of qf−p through degree m vanish.

2.1givenF1step 1.1algebra

For each m<k≤m+n, write k=m+ℓ with 1≤ℓ≤n. The moment equation in [F1] says ∑j=1nqjck−j=−ck, exactly the assertion that the degree-k coefficient of qf is zero, because q0=1. Therefore every coefficient of qf−p through degree m+n vanishes.

3.1givenA1step 2.1algebra∎

Analyticity implies qf−p has a Taylor expansion whose first possibly nonzero term has degree at least m+n+1, so qf−p=O(zm+n+1). By [A1], divide by the nonvanishing q near zero to obtain the asserted local order for f−p/q. This proof uses only the solvable coefficient equations; it makes no claim about zeros of q away from 0.

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