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.
Differentiation under the integral sign
Statement
Let be an open interval and let be such that:
- for every , the function is integrable;
- for almost every , the map is differentiable on ;
- for every , the function extended by zero where the derivative is undefined, is measurable;
- there are a measurable null set and a nonnegative measurable function with and for every and every .
Then is differentiable on , and with the same zero extension in the last integral.
Facts & Assumptions
Given: An open interval , a function satisfying the first three displayed hypotheses, and a measurable null set together with a nonnegative measurable majorant satisfying hypothesis 4. Choose a measurable null set outside which hypothesis 2 holds, and put .
Dominated convergence applies to integrable complex-valued functions under a single majorant (Dominated convergence).
The mean value theorem bounds difference quotients by a derivative bound on an interval (The mean value theorem, as the case of Cauchy's: for continuous on with and differentiable on there is with ).
The complex integral is linear on (The Lebesgue integral is linear on ).
The rationals are dense in the reals (The rationals embed densely in the reals).
Proof
Fix and let with and . Define For every , differentiability in gives . Give the derivative value zero on ; this measurable modification differs from the stated zero extension only on a null set, so it has the same integral.
For each , hypothesis 1 makes and integrable and therefore measurable, so is measurable. Fix and . If , then is immediate. Otherwise put so and Apply [L2] to the real-valued function on the segment joining to . For some interior point of that segment, Hypothesis 3 and the zero extension make the limit measurable. Therefore [L1] applies to .
By [L1], Linearity of the integral gives This holds for every supplied sequence of admissible nonzero increments.
The same mean-value estimate as in step 2.1, with any in place of , gives outside . Integrating yields , so is continuous. Consequently is continuous on the punctured interval of admissible increments. If failed to tend to as , there would be an and, for every , a nonzero admissible with and . Continuity of and [L4] give a rational admissible with and . Fix an enumeration of and take the first such rational for each ; this is a definable selection from a countable set and uses no Countable Choice. Then , contradicting step 3.1. Thus , which is precisely . Since was arbitrary, the theorem follows.
Depends on
Used by
- Diameter rigidity from toponogov under a sectional lower bound Corollary
- Heat-semigroup martingales Corollary
- Spatial smoothing of forcing separated from the observation time Corollary
- A non-Dini continuous Poisson source can destroy the continuity of the second derivatives Counterexample
- Finite speed of propagation does not imply strong Huygens Counterexample
- Wave energy need not be conserved through an open boundary Counterexample
- The standard intertwining operator A(nu) Definition
- A planar discontinuity and the space--time normal form of Rankine--Hugoniot Example
- Differentiating ∫₀^∞ e⁻ᵗˣsin x dx under the integral sign Example
- Finite and countable planar sets have zero logarithmic capacity Example
- Newton shell theorem from harmonic mean values Example
- The Gaussian attains equality in the Heisenberg inequality Example
- The positive-type Gaussian on the real line and its cyclic model Example
- Backward uniqueness for the heat equation on a bounded interval Lemma
- Compact capacity-zero sets and subharmonic minus-infinity loci Lemma
- Distributional Laplacian of a compact logarithmic potential Lemma
- Energy identity for the forced Dirichlet heat equation Lemma
- Euclidean Gaussian transform with the 2π normalization Lemma
- Heat-ball representation formula Lemma
- Maximum principle for a compact logarithmic potential Lemma
- Smoothing continuous families of formal immersions Lemma
- Smoothing continuous families of genuine immersions Lemma
- Spatial and time derivatives pass through heat convolution for positive time Lemma
- Stationary phase with a compactly supported amplitude Lemma
- Strict positivity of logarithmic energy for a zero-mass signed charge Lemma
- The fixed-support Cauchy transform and its Hölder bounds Lemma
- The local graph flux calculation Lemma
- First variation of volume for a normal variation Proposition
- Conservation of total wave energy in three admissible settings Theorem
- Continuous Dirichlet problem on a ball Theorem
- Convolution with a mollifier is smooth, and derivatives pass under the integral sign Theorem
- Duhamel principle for the whole-space heat equation Theorem
- Energy uniqueness for the homogeneous heat equation Theorem
- Harmonic functions are real analytic Theorem
- Hölder data give a classical Newtonian solution Theorem
- Interior derivative estimates for harmonic functions Theorem
- Knapp necessary condition for spherical L2 restriction Theorem
- Newtonian potentials solve the distributional Poisson equation Theorem
- Poisson kernel and bounded Dirichlet problem on a half-space Theorem
- The strong Huygens principle in odd spatial dimensions Theorem
…and 1 more result.
Dependency tree · two levels
25 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
- Gerald B. Folland, Real Analysis, 2nd ed., Theorem 2.27 (standard reference, not scraped)