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Gauss-Newton contracts linearly under a controlled residual-curvature bound

Statement

Let m,n≥1, and let r:U→Rm be C2 on an open U⊆Rn, let ϕ=∥r∥22/2, J=Dr, A=JTJ, and S(x)=∑iri(x)∇2ri(x). Let x∗∈U satisfy J(x∗)Tr(x∗)=0, and let the closed ball B={x:∥x−x∗∥2≤R} lie in U, with R>0. Suppose on B:

  • J(x) has full column rank and smallest singular value at least σ>0;
  • ∥J(x)∥2≤M;
  • J is L-Lipschitz in the Euclidean induced matrix norm;
  • ∥S(x)∥2≤κ.

Define q=(κ+MLR)/σ2 and assume q<1. For the exact full-rank Gauss-Newton step p(x)=−A(x)−1J(x)Tr(x), supply an exact reduced QR factorization of J(x) to the exact branch of Gauss-Newton linearized least-squares step with QR/SVD rank safeguards at each x∈B; the full-column-rank hypothesis guarantees such a factorization. Every x∈B satisfies ∥x+p(x)−x∗∥2≤q∥x−x∗∥2. Consequently the exact iterates from any x0∈B stay in B and converge to x∗ at a linear rate no larger than q. The curvature hypothesis controls the residual term S; no quadratic rate is claimed when it is nonzero.

Facts & Assumptions

Given: The residual map, stationary point, ball, and quantitative bounds in the Statement.

[F1]

The nonlinear least-squares gradient and Hessian formulas: ∇ϕ=JTr and ∇2ϕ=JTJ+S.

[F2]

If f:[a,b]→Rm is differentiable with integrable f′ then ∫abf′=f(b)−f(a); and a bounded derivative makes f Lipschitz: for a vector-valued path differentiable on a closed interval with integrable derivative, the endpoint difference is the integral of that derivative.

[F3]

Induced matrix norms are compatible with matrix-vector multiplication, submultiplicative, and satisfy ||I|| = 1: the induced Euclidean matrix norm satisfies ∥Av∥2≤∥A∥2∥v∥2 and ∥AB∥2≤∥A∥2∥B∥2.

[F5]

The matrix norm induced by a published vector p-norm: the matrix 2-norm is induced by the Euclidean vector norm.

[F6]

The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a): the derivative of the path composition is the derivative of the outer map applied to its tangent.

[F8]

The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: the Euclidean norm is induced by the standard dot product and ∥v∥22=vTv.

[A1]

x∗ is stationary: J(x∗)Tr(x∗)=0.

[A2]

The bounds and strict contraction factor q<1 hold throughout the stated convex ball.

Proof

1.1givenA2F4F5F8algebra

For each x∈B, the SVD [F4] writes J(x)=U1ΣVT with every diagonal entry of Σ at least σ. Thus A(x)=VΣ2VT is invertible and A(x)−1=VΣ−2VT. By [F4]–[F5], ∥A(x)−1∥2≤σ−2.

1.2givenA1F1F2F6construct

Fix x∈B, put e=x−x∗, and set xt=x∗+te. The path t↦∇ϕ(xt) is continuously differentiable; [F1] and [F6] give derivative (A(xt)+S(xt))e. This derivative is continuous and hence componentwise integrable, so [F2] and [A1] yield J(x)Tr(x)=∫01(A(xt)+S(xt))e dt.

1.3givenA2F3F4algebra

For 0≤t≤1, write A(x)−A(xt)=J(x)T(J(x)−J(xt))+(J(x)T−J(xt)T)J(xt). An SVD of J(x)−J(xt) also gives an SVD of its transpose with the same singular values, so [F4] gives ∥J(x)T−J(xt)T∥2=∥J(x)−J(xt)∥2 and ∥J(x)T∥2=∥J(x)∥2. The Lipschitz and boundedness hypotheses, with [F3], now give ∥A(x)−A(xt)∥2≤2ML(1−t)∥e∥2.

2.1step 1.1step 1.2step 1.3A2F3F7F8algebra

The exact step satisfies x+p(x)−x∗=A(x)−1(A(x)e−J(x)Tr(x)). Step 1.2 makes the parenthesized term ∫01(A(x)−A(xt)−S(xt))e dt. By step 1.3, ∥S(xt)∥2≤κ, and [F7] bounds the integral norm by (ML∥e∥2+κ)∥e∥2. Step 1.1 therefore gives ∥x+p(x)−x∗∥2≤σ−2(ML∥e∥2+κ)∥e∥2≤q∥e∥2, since ∥e∥2≤R.

3.1step 2.1algebra∎

Because q<1, step 2.1 keeps every iterate in B and gives ∥xk−x∗∥2≤qk∥x0−x∗∥2, which tends to zero.

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