How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Fixed-memory L-Bfgs curvature and scale bounds imply uniform spectral bounds
Statement
Fix , constants , , and . Suppose every stored pair in a limited-memory BFGS state satisfies and each base scale satisfies . Then the implicit SPD matrix represented by the two-loop recursion of Limited-memory Bfgs two-loop recursion with curvature filtering has uniform bounds Here means for all . If the stored list is nonempty, the usual scale lies in .
Facts & Assumptions
Given: , the stored-pair bounds, and the L-BFGS state in the Statement.
The L-Bfgs two-loop recursion equals the stored inverse updates and costs linear memory work: the implicit matrix is obtained by at most sequential inverse BFGS updates from .
Bfgs updates preserve the secant equations, symmetry, and positive definiteness: each positive-curvature inverse update preserves positive definiteness and is reciprocal to its Hessian update.
Bfgs trace and determinant identities give a matrix potential inequality: for , one update adds at most to and multiplies by .
In an orthonormal basis, self-adjoint means conjugate-transpose symmetry and normal means commuting with the conjugate transpose and Real spectral theorem: a self-adjoint endomorphism of a finite-dimensional real inner product space has an orthonormal eigenbasis: a real symmetric matrix represents a self-adjoint endomorphism of Euclidean and has an orthonormal eigenbasis. If the matrix is SPD, each eigenvalue is positive by evaluating its quadratic form on a unit eigenvector.
Limited-memory Bfgs two-loop recursion with curvature filtering: the scale from the newest pair is .
The basis-independent characteristic polynomial of an endomorphism of a finite-dimensional space, including in dimension zero, For , the characteristic polynomial is when , with for the unique matrix, and The determinant of a triangular matrix is the product of its diagonal entries: in an eigenbasis with diagonal matrix , . If in , then : trace is the sum of the eigenvalues counted with algebraic multiplicity and If in , then : determinant is the product of the eigenvalues counted with algebraic multiplicity then give the trace and determinant as and ; The basis-independent trace of an endomorphism of a finite-dimensional vector space and The determinant of an endomorphism of a finite-dimensional vector space: its matrix determinant in an ordered basis in positive dimension, and on the zero space identify these with the represented matrix's trace and determinant. The triangular-determinant rule also gives .
Proof
Given: , the stored-pair bounds, and the L-BFGS state in the Statement.
[F1] The L-Bfgs two-loop recursion equals the stored inverse updates and costs linear memory work: the implicit matrix is obtained by at most sequential inverse BFGS updates from .
[F2] Bfgs updates preserve the secant equations, symmetry, and positive definiteness: each positive-curvature inverse update preserves positive definiteness and is reciprocal to its Hessian update.
[F3] Bfgs trace and determinant identities give a matrix potential inequality: for , one update adds at most to and multiplies by .
[F4] In an orthonormal basis, self-adjoint means conjugate-transpose symmetry and normal means commuting with the conjugate transpose and Real spectral theorem: a self-adjoint endomorphism of a finite-dimensional real inner product space has an orthonormal eigenbasis: a real symmetric matrix represents a self-adjoint endomorphism of Euclidean and has an orthonormal eigenbasis. If the matrix is SPD, each eigenvalue is positive by evaluating its quadratic form on a unit eigenvector.
[F5] Limited-memory Bfgs two-loop recursion with curvature filtering: the scale from the newest pair is .
[F6] The basis-independent characteristic polynomial of an endomorphism of a finite-dimensional space, including in dimension zero, For , the characteristic polynomial is when , with for the unique matrix, and The determinant of a triangular matrix is the product of its diagonal entries: in an eigenbasis with diagonal matrix , . If in , then : trace is the sum of the eigenvalues counted with algebraic multiplicity and If in , then : determinant is the product of the eigenvalues counted with algebraic multiplicity then give the trace and determinant as and ; The basis-independent trace of an endomorphism of a finite-dimensional vector space and The determinant of an endomorphism of a finite-dimensional vector space: its matrix determinant in an ordered basis in positive dimension, and on the zero space identify these with the represented matrix's trace and determinant. The triangular-determinant rule also gives .
Let . By [F1] and [F2], this is an SPD matrix obtained from by at most direct BFGS updates. Its initial trace satisfies . Each update adds at most to trace by [F3] and the pair bound. Hence .
By [F4], choose an orthonormal eigenbasis for and let its positive eigenvalues be . In this basis the characteristic polynomial factors as , so [F6] gives and . By step 1.1 each , and expanding in this orthonormal basis gives . The determinant ratio in [F3] and the lower pair bound therefore give Since and there are at most updates, while , it follows that .
Let be the smallest eigenvalue. By step 2.1, is the product of the positive eigenvalues, and the other eigenvalues are at most . Thus , while every eigenvalue is at most . The eigenvalues of are the reciprocals, so they lie in . The spectral theorem translates these bounds into the asserted quadratic-form inequalities.
If the stored list is nonempty, take its newest pair. For the standard scale, [F5] and the upper curvature bound give . By Cauchy–Schwarz and the lower curvature bound, , so and . The other pair bound gives , hence .
Depends on
- Limited-memory Bfgs two-loop recursion with curvature filtering
- The L-Bfgs two-loop recursion equals the stored inverse updates and costs linear memory work
- Bfgs updates preserve the secant equations, symmetry, and positive definiteness
- Bfgs trace and determinant identities give a matrix potential inequality
- Real spectral theorem: a self-adjoint endomorphism of a finite-dimensional real inner product space has an orthonormal eigenbasis
- In an orthonormal basis, self-adjoint means conjugate-transpose symmetry and normal means commuting with the conjugate transpose
- The basis-independent characteristic polynomial $\chi_T$ of an endomorphism of a finite-dimensional space, including $\chi_T=1$ in dimension zero
- For $A\in M_n(F)$, the characteristic polynomial is $\chi_A(x)=\det(xI_n-A)$ when $n\geq1$, with $\chi_A(x)=1$ for the unique $0\times0$ matrix
- The determinant of a triangular matrix is the product of its diagonal entries
- If $\chi_T(x)=\prod_{i<n}(x-\lambda_i)$ in $F[x]$, then $\operatorname{tr}(T)=\sum_{i<n}\lambda_i$: trace is the sum of the eigenvalues counted with algebraic multiplicity
- If $\chi_T(x)=\prod_{i<n}(x-\lambda_i)$ in $F[x]$, then $\det(T)=\prod_{i<n}\lambda_i$: determinant is the product of the eigenvalues counted with algebraic multiplicity
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- The determinant of an endomorphism of a finite-dimensional vector space: its matrix determinant in an ordered basis in positive dimension, and $1$ on the zero space
Used by
Dependency tree · two levels
39 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Dong C. Liu and Jorge Nocedal, On the limited memory BFGS method for large scale optimization (standard reference, not scraped)
- Jorge Nocedal and Stephen J. Wright, Numerical Optimization, 2nd ed. (standard reference, not scraped)