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The A_p classes are open in the exponent

Statement

Assume the Axiom of Countable Choice (The Axiom of Countable Choice (ACω)). Let 1<p<∞ and w∈Ap (Muckenhoupt A_p and A_1 weights). Then there is ε=ε(n,p,[w]Ap)>0 with w∈Ap−ε and [w]Ap−ε bounded in terms of n,p,[w]Ap. More precisely, if the dual weight v:=w1/(1−p)=w−1/(p−1)∈Ap′ satisfies a reverse Hölder inequality with exponent q>1 and constant c (as supplied by the previous theorem), then one may take p−ε=1+p−1q<p,[w]Ap−ε≤cp−1[w]Ap. Hence Ap=⋃1<r<pAr.

Facts & Assumptions

Given: Countable Choice, 1<p<∞, w∈Ap, the dual weight v=w−1/(p−1), and a reverse Hölder pair (q,c) for v.

[F1]

Duality: v∈Ap′ with [v]Ap′=[w]Ap1/(p−1), where p′ is the conjugate exponent of p (Duality and nesting of the A_p classes, Conjugate exponents, including the endpoint conventions).

[F2]

The reverse Hölder theorem applied to v with a fixed 0<α<1 supplies q=1+γ>1 and c=C<∞, depending only on n,p′,[v]Ap′ and α, with (⟨vq⟩Q)1/q≤c⟨v⟩Q for every cube Q (Reverse Holder self-improvement for A_p weights).

[F3]

The Ap condition is the finiteness of ⟨w⟩Q⟨w−1/(p−1)⟩Qp−1 uniformly in Q; all averages are nonnegative and the exponents combine by the usual power laws (Muckenhoupt A_p and A_1 weights, Holder's inequality for integrals, including the endpoint cases).

Proof

technique · direct
1.1F1F2givenalgebra

By step [F1], v∈Ap′ with [v]Ap′=[w]Ap1/(p−1), so [F2] applies to v and yields q>1, c<∞ with (⟨vq⟩Q)1/q≤c⟨v⟩Q for every cube Q. Define ε by 1/(p−ε−1)=q/(p−1), i.e. p−ε=1+(p−1)/q; since q>1 one has p−ε<p and p−ε>1.

2.1F2step 1.1givenalgebra

With this choice, 1/(1−(p−ε))=−1/(p−ε−1)=−q/(p−1), so w1/(1−(p−ε))=w−q/(p−1)=(w−1/(p−1))q=vq. Therefore, for every cube Q, (⟨w1/(1−(p−ε))⟩Q)p−ε−1=(⟨vq⟩Q)(p−1)/q≤(c⟨v⟩Q)p−1=cp−1⟨v⟩Qp−1 by the reverse Hölder inequality and the exponent identity.

3.1F3step 2.1givenalgebra

Multiplying the estimate of step 2.1 by ⟨w⟩Q and inserting the Ap bound ⟨w⟩Q⟨v⟩Qp−1≤[w]Ap valid for every cube Q gives ⟨w⟩Q(⟨w1/(1−(p−ε))⟩Q)p−ε−1≤cp−1[w]Ap for every cube; this is exactly the Ap−ε condition with characteristic at most cp−1[w]Ap.

4.1F1step 1.1step 3.1givenalgebra∎

The monotonicity part of [F1] gives Ar⊆Ap for every 1<r<p; step 1.1 and step 3.1 exhibit, for each w∈Ap, an exponent p−ε<p with w∈Ap−ε, so every element of Ap lies in some Ar with r<p. Hence Ap=⋃1<r<pAr, and ε and the bound on [w]Ap−ε depend only on n,p,[w]Ap (through [v]Ap′ and the fixed α).

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