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RNP and almost-everywhere differentiability of Lipschitz curves

Statement

Assume the Axiom of Choice. A Banach space X has the Radon--Nikodym property if and only if every Lipschitz map F:[0,1]X is norm differentiable at Lebesgue-almost every t(0,1); that is, for almost every such t there is an F(t)X for which

limh0F(t+h)F(t)hF(t)=0.

Facts & Assumptions

[A1]

The Axiom of Choice holds (The Axiom of Choice).

[L1]

In ZF, AC implies Dependent Choice and Countable Choice (AC supplies the countable and dependent choices used in Banach integration).

[L2]

Under Countable Choice, based Lipschitz curves correspond to interval vector measures dominated in variation by Lebesgue measure (Lipschitz curves and dominated interval vector measures).

[L3]

Under AC, RNP is equivalent to the Bochner-density property for bounded-variation vector measures on the Lebesgue interval (RNP may be tested on the Lebesgue interval).

[L4]

Bochner integrability is L1 approximation by integrable simple functions (Bochner-integrable function), and for strongly measurable functions it is equivalent to integrability of the norm (Bochner integrability criterion, Strongly measurable Banach-valued function).

[L5]

Scalar Lloc1 functions are recovered almost everywhere by small interval averages, and countable unions of Lebesgue-null sets are null under Countable Choice (Lebesgue differentiation theorem on Rn, A countable union of measure-zero sets has measure zero, by countable choice).

[L6]

A Bochner density induces a vector measure whose variation is the integral of its norm (A Bochner density defines an absolutely continuous vector measure).

[L7]

Bounded linear maps commute with Bochner integration (Bounded linear maps commute with Bochner integration).

[L8]

The variation of a bounded-variation vector measure is a finite positive measure (Bounded variation of a vector measure is a finite measure), and under AC a finite absolutely continuous scalar measure has an integrable Radon--Nikodym density (A sigma-finite signed measure that is absolutely continuous with respect to a sigma-finite positive measure has a unique almost-everywhere density).

[L9]

Real Lipschitz functions are absolutely continuous, and under Countable Choice and Dependent Choice the scalar FTC recovers an absolutely continuous function from its derivative (C1 implies Lipschitz, Lipschitz implies absolutely continuous, and absolutely continuous implies continuous and bounded variation, Fundamental theorem of calculus for absolutely continuous functions).

[L10]

The continuous dual separates distinct vectors (The dual space separates points of a normed space).

[L11]

Under Countable Choice, dominated pointwise convergence implies L1 and integral convergence for strongly measurable Banach-valued functions (Bochner dominated convergence theorem).

Proof

technique · direct

Given: A Banach space X and AC.

1.1

Make the inherited choice assumptions explicit. By [L1], [A1] supplies both Countable Choice and Dependent Choice. Countable Choice is used in [L2], [L5], and [L11]; both principles are hypotheses of the scalar FTC in [L9].

givenA1L1
1.2

Associate a dominated vector measure to a Lipschitz curve. Suppose first that X has RNP, let F:[0,1]X be L-Lipschitz, and put G(t)=F(t)F(0). Then G(0)=0 and [L2] gives a vector measure νG with νGLλ and νG((a,b])=G(b)G(a).

givenL2construct
1.3

Reduce an arbitrary interval vector measure to bounded-density levels. For the converse direction, let ν be a bounded-variation vector measure on [0,1] with νλ. If λ(E)=0, every member of every finite partition of E is null and has ν-value zero, so ν(E)=0. Thus νλ. By [L8] and AC there is an integrable scalar density g with ν(E)=Egdλ. Positivity of ν makes g0 almost everywhere: applying the representation to {g1/m} for each m1 makes each such set null. Replace g by zero on their null union. Put An={n1g<n} for n1 and Z={g=+}. The An are disjoint, Z is null, and they cover [0,1]Z. Define νn(E)=ν(EAn). Directly from finite partitions, νn(E)=ν(EAn)nλ(E).

givenA1L8construct
2.1

Obtain a Bochner density in the RNP-to-differentiability direction. The interval test [L3] applied to νG supplies a Bochner-integrable f:[0,1]X with νG(E)=Efdλ. Hence G(b)G(a)=(a,b]fdλ for every a<b.

A1L3step 1.1step 1.2
2.2

Turn each bounded level measure into a Lipschitz curve. For each n, set Fn(t)=νn((0,t]). The converse part of [L2] and the bound in step 1.3 show that Fn(0)=0 and that Fn is n-Lipschitz.

L2step 1.1step 1.3
3.1

Prepare a common set of vector Lebesgue points. Choose integrable simple sm with fsm0 as in [L4]. Passing to a subsequence if necessary, the scalar errors em=fsm converge to zero almost everywhere: choose least indices with L1 errors below 22m, and the sets where the corresponding pointwise error exceeds 2m have summable measures, so their tail unions decrease to a null set. Extend em and the finitely many indicator functions of the level sets of sm by zero outside [0,1]. Apply [L5] to every one of this countable family and remove the union of their exceptional null sets. At each remaining interior point t, every em differentiates by interval averages, em(t)0, and

L4L5step 2.1choose

limr0+12rtrt+rsm(u)sm(t)du=0

for every m; the last equality follows by writing the finite-valued sm on its level sets and differentiating their indicators.

3.2

Construct measurable derivative fields for the bounded level curves. By the assumed differentiability property, for each n there is a measurable null set Nn off which Fn exists in norm. For k2 put qn,k(t)=k(Fn(t+1/k)Fn(t)) when t11/k, and put it equal to zero on the remaining interval. On the first piece qn,k is 2nk-Lipschitz; a finite interval partition of sufficiently small mesh, together with the constant-zero last piece, therefore gives a measurable simple function within 1/k uniformly of qn,k. These simple functions converge to Fn off Nn. Define fn=Fn there and fn=0 on Nn. This proves strong measurability in the sense of [L4]. Difference quotients give fnn off Nn, so [L4] makes fn Bochner integrable.

L4step 2.2construct
4.1

Differentiate the indefinite Bochner integral in norm. At a point t retained in step 3.1, for fixed m the triangle inequality gives

L5step 2.1step 3.1

lim supr0+12rtrt+rf(u)f(t)du2em(t).

Indeed the three terms are the average of em(u), the average of sm(u)sm(t), and em(t). Letting m makes the right side zero. For nonzero h small enough that t+h[0,1], step 2.1 now yields

F(t+h)F(t)hf(t)1hmin(t,t+h)max(t,t+h)f(u)f(t)du,

which is at most twice the corresponding centred average and tends to zero. Thus F(t)=f(t) at almost every t(0,1).

4.2

Show that each derivative field represents its level measure. Fix n and xX. The real-valued function xFn in the real case, and its real and imaginary parts in the complex case, are Lipschitz and hence absolutely continuous by [L9]. Their derivatives agree almost everywhere with the corresponding scalar parts of xfn. The scalar FTC, whose choice hypotheses were supplied in step 1.1, and commutation in [L7] give

L2L6L7L9L10step 1.1step 2.2step 3.2

x(Fn(b)Fn(a))=x ⁣((a,b]fndλ).

By [L10], νn((a,b])=(a,b]fndλ. The measure induced by fn has variation at most nλ by [L6], so uniqueness in [L2] makes it equal to νn on every Lebesgue set. Finally put hn=1Anfn. Restricting simple approximants shows Ehn=EAnfn=νn(E), so hn is another density of νn, now supported on An.

5.1

Complete the forward implication, including its boundary cases. Step 4.1 proves almost-everywhere norm differentiability of every Lipschitz curve when X has RNP. Adding the constant F(0) does not affect difference quotients. If L=0, the curve is constant and has derivative zero everywhere; the endpoints are excluded from the derivative assertion and have measure zero. The zero Banach space and the one-point interval cause no exception.

step 1.2step 2.1step 4.1
5.2

Paste the bounded derivative fields into one density. Define h(t)=hn(t) on An and h=0 on Z. The explicit simple approximants from step 3.2, multiplied by 1An and summed for nk, form a simple sequence converging to h off the countable union of the Nn and Z; [L5] makes that union null. Hence h is strongly measurable. Moreover hn1n1Ang+1, so [L4] makes h Bochner integrable. Let HN=n=1Nhn. Then HNh pointwise and HNg+1. Applying [L11] to 1EHN for any measurable E gives EHNEh. Finite linearity follows by combining the simple approximations in [L4], so step 4.2 gives EHN=n=1Nν(EAn). Norm countable additivity of ν and ν(EZ)=0 make the latter sums converge to ν(E). Thus h is a Bochner density of ν.

L4L5L11step 1.1step 1.3step 4.2
6.1

Conclude the equivalence and record the exact AC use. [A1, L3, step 5.1, step 5.2] Step 5.1 proves RNP implies almost-everywhere differentiability. Conversely, step 5.2 gives a density for every vector measure in the interval test [L3], so X has RNP. AC is used by the scalar Radon--Nikodym theorem, the interval RNP test, and through step 1.1 for countable null-set, dominated-convergence, and scalar-FTC suppliers. Empty and zero measures give the zero density, and both directions of the equivalence have been proved.

A1L3step 5.1step 5.2

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