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A computed natural-cubic reconstruction has a forward-error certificate

Statement

Let r≥2 and use the stored knots and values and the algorithm of Natural-cubic tridiagonal Cholesky solve with a residual certificate. Let s be the exact natural cubic interpolant of those data, supplied by Natural cubic interpolation at distinct knots. On a successful call, let M^ be the returned second-derivative vector, put m^=(M^2,…,M^r−1), and let s^ be the piecewise cubic reconstruction defined by the algorithm from M^, evaluated exactly. For r≥3, the success output is success⁡(M^,C,α,β,B). The algorithm computes H, δ, and Q=∥m^∥∞ internally when forming B; these are not separate returned fields. The returned certificate fields satisfy

∥s^−s∥L∞([x1,xr])≤B=H28δ(C+α∥m^∥∞+β).

Here α and β account for the differences between the exact natural-cubic system assembled from the stored input data and the rounded matrix and right-hand side used by the factorization. If those systems are exactly the same, then α=β=0 and B=H2C/(8δ). For r=2, both the natural interpolant and the algorithm-defined reconstruction are the straight line, and B=0.

The algorithm-defined reconstruction interpolates the stored data, but for r≥3 it need not be C1 at its knots and is not asserted to be an exact natural spline. The bound excludes floating-point error from evaluating the cubic pieces and makes no unconditional arithmetic-success or general natural-spline fourth-order claim.

Facts & Assumptions

Given: Strictly increasing stored knots and finite stored values, r≥2, and a successful algorithm call including its exact rational certificate.

[F1]

Natural-cubic tridiagonal Cholesky solve with a residual certificate defines the exact canonical system Am=b, the stored matrix T and right-hand side f used by the rounded solve, and the discrepancies α=max⁡k∑j∣Akj−Tkj∣ and β=max⁡k∣bk−fk∣. On a successful r≥3 call it returns M^,C,α,β,B and computes H, δ, and Q=∥m^∥∞ internally to form B=H2(C+αQ+β)/(8δ).

[F2]

A successful natural-cubic tridiagonal Cholesky solve has a certified residual gives ∥Tm^−f∥∞≤C on a full successful call.

[F3]

Natural cubic interpolation at distinct knots: for r≥3, the exact natural interpolant's interior second derivatives solve Am=b; for r=2 it is the straight line.

[F4]

A natural-spline tridiagonal residual bounds the spline value error: if ρ=Am^−b is the exact residual for the interior natural-cubic system and the endpoint second derivatives agree at zero, then the piecewise cubic reconstruction differs from the exact natural interpolant on the knot hull by at most H2∥ρ∥∞/(8δ).

[A1]

The data knots are exact stored real numbers with x1<⋯<xr; for r≥3, each hi>0 and δ>0.

Proof

1.1A1F1F2algebra

Suppose r≥3. Let M^ be the returned vector and m^=(M^2,…,M^r−1) its interior subvector. By [F2] and the exact identity Am^−b=(Tm^−f)+(A−T)m^+(f−b), each row satisfies ∣(Am^−b)k∣≤∣(Tm^−f)k∣+∑j∣Akj−Tkj∣ ∣m^j∣+∣fk−bk∣≤C+α∥m^∥∞+β. Taking the maximum proves ∥Am^−b∥∞≤C+α∥m^∥∞+β; these exact discrepancies account for all rounded system assembly.

2.1A1F1F4step 1.1algebra

The returned endpoint second derivatives and those of s are both zero. Apply [F4] to the exact residual from step 1.1 and the original widths. It gives ∥s^−s∥L∞([x1,xr])≤(H2/(8δ))∥Am^−b∥∞≤(H2/(8δ))(C+α∥m^∥∞+β)=B. The transfer theorem applies to any proposed interior derivatives with zero endpoint values; it does not require the algorithm-defined pieces to join with matching first derivatives.

3.1A1F1F3algebra∎

If r=2, the algorithm returns zero endpoint second derivatives and its associated reconstruction is the exact straight-line piece. By [F3] this is also s, and the algorithm defines B=0, so the stated bound holds with equality.

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