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.
The chain rule for total derivatives:
Statement
Let be totally differentiable at and let be totally differentiable at . Then is totally differentiable at and
Facts & Assumptions
Given: The total first-order expansions of at and at .
The total-derivative definition supplies the normwise remainder estimate for every ; in positive source dimension this is equivalently the normalized remainder tending to zero as tends to zero (The total (Fréchet) derivative as the linear first-order approximation with remainder).
Total differentiability gives a local increment bound and therefore continuity (Total differentiability gives a local increment bound and therefore continuity).
Proof
If the source dimension is zero or , the derivative of the composite and the displayed composite of derivatives are the unique zero linear map, and the remainder estimate is identically zero. If the intermediate dimension , then is constant with value , , and is constant with zero derivative; again both sides agree. For the remaining proof all three dimensions are positive.
Write and , with both normalized remainders tending to zero.
By [L2], ; boundedness of and the two remainder limits show both and are , including the case .
Substitution into the two expansions leaves , and the composite of linear maps is linear.
Depends on
- The total (Fréchet) derivative $Df(a)$ as the linear first-order approximation with $o(\|h\|_2)$ remainder
- Total differentiability gives a local $O(\|h\|_2)$ increment bound and therefore continuity
- Every Euclidean linear map has a unique matrix and satisfies $\|Lh\|_2\le K\|h\|_2$ for some $K\ge0$
- A linear map $L:\mathbb{R}^m\to\mathbb{R}^n$ in Euclidean coordinates
Used by
- Finite-budget Levenberg-Marquardt with a trust-ratio safeguard Algorithm
- An everywhere-positive-definite Hessian implies strict convexity Corollary
- Cartesian and polar forms of the Cauchy–Riemann equations agree away from the origin Corollary
- Entire harmonic functions of sublinear growth are constant Corollary
- Interior gradient bound for Poisson solutions Corollary
- Poincare-Wirtinger on bounded convex domains by the direct pairwise argument Corollary
- Positive-degree Dolbeault vanishing on pseudoconvex domains Corollary
- PReLU fan-in and fan-out variance scales Corollary
- The finite-basis projector energy model supplies a C1 Hermitian response map Corollary
- Time reversal of the homogeneous wave equation Corollary
- A figure-eight curve is an immersed image but not an embedded submanifold Counterexample
- An inward cusp blocks W^1,3/2 extension Counterexample
- An isolated boundary point obstructs pointwise-zero Green data Counterexample
- Boundary H² regularity needs domain regularity Counterexample
- Exterior-sphere domains need not have global C2alpha Dirichlet solutions Counterexample
- Finite speed of propagation does not imply strong Huygens Counterexample
- Outward dilation defeats subcritical inclusion and homogeneous Poincare on Euclidean space Counterexample
- The fundamental Hessian is not absolutely locally integrable Counterexample
- The local conservation law need not integrate to a finite conserved energy Counterexample
- The W^1,p→ L^q bound fails for q>p^* by dilation Counterexample
- Wave energy need not be conserved through an open boundary Counterexample
- Differentiable stationary stochastic policies and score vectors Definition
- E-valued Dolbeault operators and their L2 structure Definition
- Geometry lift and transformed elliptic tensor Definition
- Measurable Beltrami coefficients and measurable conformal structures Definition
- Pathwise and reparameterized simulation-gradient estimators Definition
- Second-order Laplace-type operators on metric vector bundles Definition
- The finite-holonomy normal model of a compact leaf Definition
- The standard intertwining operator A(nu) Definition
- Wave equation, Cauchy data and wave speed Definition
- Weak solutions of the Beltrami equation Definition
- Wolfe and strong Wolfe line-search conditions Definition
- A curved double well has an exact circular minimum-energy path Example
- A cusp in a chosen exchange-correlation term violates the C2 hypothesis Example
- A radial three-dimensional wave reduces to one dimension Example
- A regularized logistic finite sum with an exact minimizer Example
- A two-interval shooting residual has a block-bidiagonal sensitivity Jacobian Example
- An explicitly treated stiff decay mode is unstable for a large step Example
- An isotropic Gaussian Wasserstein geodesic Example
- Analytic transport data Example
…and 290 more results.
Dependency tree · two levels
14 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
- J. Lebl, Basic Analysis I, §8.3 (standard reference, not scraped)