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Validated Hessian enclosures and a small gradient residual certify a nearby index-one saddle

Statement

Let d≥2, let V∈C4(U,R) on an open U⊆Rd, and let x∈U. Put H=∇2V(x) and ϵg=∥∇V(x)∥2. Suppose a validated ordered eigenvalue enclosure certifies index one with gap γ>0 in the sense of Validated ordered eigenvalue enclosures for an index-one Hessian. If ϵg=0, then x is an exact critical point with Hessian index one.

If ϵg>0, put ρ=2ϵg/γ. Assume B2(x,2ρ)⊂U, the Hessian is L-Lipschitz in the induced Euclidean operator norm there, and Lρ/γ≤1/2. Then there is exactly one critical point x∗ in B‾2(x,ρ), it satisfies ∥x∗−x∥2≤ρ, and its Hessian has exactly one negative eigenvalue and no zero eigenvalues. The reported residual ϵg, gap γ, conditioning bound 1/γ, Hessian Lipschitz constant L, and radius condition are part of the certificate; a residual or a Ritz value alone is not a certificate.

Facts & Assumptions

Given: The potential, point, gradient residual, interval evidence, gap, and local Hessian-Lipschitz hypotheses in the Statement.

[F1]

Validated ordered eigenvalue enclosures for an index-one Hessian: the validated intervals certify λ1(H)≤−γ and λj(H)≥γ for j≥2.

[F2]

Since V∈C4, it is C2, and The Hessian of a C2 scalar field is symmetric gives HT=H. In the standard Euclidean inner product this is a self-adjoint endomorphism, so Real spectral theorem: a self-adjoint endomorphism of a finite-dimensional real inner product space has an orthonormal eigenbasis gives an orthonormal eigenbasis.

[F3]

The Hessian matrix and critical points of a scalar field and The Jacobian matrix of partial derivatives and the gradient in the scalar-valued case define H and the gradient. Since V∈C4, the gradient's coordinate partials exist and are continuous; If all partial derivatives exist on a neighbourhood and are continuous at a point, then the map is totally differentiable there with Jacobian derivative at each point makes the gradient totally differentiable. Its derivative matrix is continuous and equals the gradient Jacobian by A total derivative computes every directional derivative, and its matrix is the Jacobian, and The Hessian of a C2 scalar field is symmetric identifies it with the Hessian. Thus ∇V is C1, and a critical point is its zero.

[F4]

A small residual gives a nearby root under a uniform inverse and Lipschitz bound: if DF(x) is invertible, has inverse norm at most β, and is L-Lipschitz on a sufficiently large ball, then ∥F(x)∥ small enough gives a unique nearby zero within 2β∥F(x)∥.

[F5]

Courant-Fischer min-max principle for self-adjoint endomorphisms on finite-dimensional real inner product spaces: the largest eigenvalue is the maximum Rayleigh quotient, and the second largest is at most the maximum Rayleigh quotient on the orthogonal complement of a leading eigenvector.

[F6]

The operator norm is 0 on the zero domain and otherwise equals the largest singular value, attained at a right-singular vector: the maximum defining the finite-dimensional Euclidean operator norm exists, and its definition bounds ∥Bw∥2 by ∥B∥op∥w∥2.

Given: The data in the Statement.

Proof

1.1F1F2F6givenalgebra

By [F1], the eigenvalues of H are all at least distance γ from zero. Using the orthonormal eigenbasis in [F2], H is invertible and each unit vector is expanded by H−1 by at most 1/γ; [F6] therefore gives ∥H−1∥op≤1/γ.

2.1F1F3F4givenstep 1.1algebra

If ϵg=0, [F3] says x is critical, and [F1] says its Hessian has exactly one negative eigenvalue. Suppose henceforth ϵg>0 and use the inverse bound β=1/γ from step 1.1. The radius in [F4] is then exactly 2βϵg=ρ, and its Lipschitz condition is βLρ=Lρ/γ≤1/2. Since B2(x,2ρ)⊂U, every hypothesis of [F4] holds on the stated ball, so there is exactly one zero x∗ of ∇V in B‾2(x,ρ) and ∥x∗−x∥2≤ρ.

3.1F1F2step 2.1givenalgebra

Set A=−H(x) and E=−(H(x∗)−H(x)). Then A is symmetric with largest eigenvalue at least γ and second-largest at most −γ. The Lipschitz hypothesis is in the induced Euclidean operator norm, so ∥E∥op≤Lρ≤γ/2 by step 2.1.

4.1F1F2F5F6F7step 2.1step 3.1algebra∎

Let q1 be a unit leading eigenvector of A. The maximum Rayleigh formula in [F5] yields λ1(A+E)≥q1T(A+E)q1≥λ1(A)−∥E∥op≥γ/2>0 by [F6, F7]. The second-eigenvalue min-max formula in [F5], applied to q1⊥, yields λ2(A+E)≤λ2(A)+∥E∥op≤−γ/2<0. Every later eigenvalue is at most the second, so A+E=−H(x∗) has exactly one positive eigenvalue and no zero eigenvalue. Thus H(x∗) has exactly one negative eigenvalue and no zero eigenvalues. Together with step 2.1 this proves the stated local certificate; if ϵg=0, step 2.1 already proved it.

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