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Unrestricted variable-step ratios amplify a vanishing BDF2 starter error

Statement refuted

For every family of variable-step grids with maximum step tending to zero, applying BDF2 to y′=0 with any starter errors tending to zero produces maximum grid error tending to zero, without any bound on adjacent step ratios.

Facts & Assumptions

Given: The variable-step BDF2 procedure Variable-step BDF2 with an explicit local implicit-branch rule applied to y′=0, and its homogeneous increment recurrence The variable-step BDF2 parasitic increment contracts below the sharp ratio threshold.

[L1]

The variable-step BDF2 parasitic increment contracts below the sharp ratio threshold gives Δn+1=rn21+2rnΔn for f=0 and every positive ratio.

Counterexample

For each integer m≥2, take T=1 and grid increments

h0=m−2,h1=m−1,h2=⋯=hm−1=m−1,hm=m−1−m−2.

They sum to one and have maximum Hm=1/m→0, but the first adjacent ratio is r1=m. For the exact solution y=0, use starters Y0=0, Y1=1/m, whose error tends to zero.

For the branch input in Variable-step BDF2 with an explicit local implicit-branch rule, prescribe every ball to be the closed radius-two ball centered at zero. Supply the returning exact branch oracle that computes Z=((1+r)2Yn−r2Yn−1)/(1+2r) and returns unique-root with Z if Z is in the prescribed ball, and no-root otherwise. For f=0 the field is defined on every ball and the positive coefficient 1+2r excludes multiple roots.

1.1givenalgebra

Summing the increments gives m−2+m−1+(m−2)m−1+m−1−m−2=1, and every increment is positive for m≥2. The maximum is Hm=m−1.

1.2givenalgebra

The first ratio is r1=h1/h0=m and the starter increment is Δ1=1/m→0.

2.1L1step 1.1step 1.2algebra

For n≥2 the grid has rn≤1, so [L1] gives 0<q(rn)=rn2/(1+2rn)≤rn/2≤1/2. The increments from Δ2 onward are positive and their total is at most Δ2∑j≥02−j=2Δ2<1. Since Y1=1/m≤1/2, every computed value is less than 3/2. For f=0 the step equation has exactly one root because its coefficient 1+2rn is positive, so all roots lie in the prescribed balls and the algorithm completes.

2.2L1step 1.2algebra

By [L1], Δ2=m21+2m1m=m1+2m→12. Therefore Y2=Y1+Δ2→12, while t2=h0+h1→0 and the exact solution remains zero.

3.1step 1.1step 2.1step 2.2∎

Thus a vanishing starter perturbation produces an error bounded away from zero even though Hm→0. The claimed ratio-free uniform zero-stability fails.

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