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Dyadic annulus far-field estimates for the maximal function

Statement

Assume the Axiom of Countable Choice (The Axiom of Countable Choice (ACω)). Let f∈Lloc1(Rn), z∈Rn, r>0 and δ>0. Then ∫∣t−z∣≥r∣f(t)∣ ∣t−z∣−n−δ dt≤Cn,δ r−δMf(z), where M is the centred Hardy-Littlewood maximal function (The centered and uncentered Hardy-Littlewood maximal functions) and Cn,δ=22n(1−2−δ)−1 depends only on n and δ.

Facts & Assumptions

Given: Countable Choice, f∈Lloc1(Rn), z∈Rn, r>0 and δ>0.

[F1]

For every locally integrable f one has Mf(z)=sup⁡ρ>0λ(B(z,ρ))−1∫B(z,ρ)∣f∣ dλ, and each average is finite because f is integrable over balls (The centered and uncentered Hardy-Littlewood maximal functions, A locally integrable function on Rn).

[F2]

Every ball B(x,ρ) is Lebesgue measurable with 0<λ(B(x,ρ))<∞ (Euclidean balls have positive finite Lebesgue measure), the dilates of the unit ball satisfy λ(B(0,ρ))=vnρn with vn=λ(B(0,1))∈(0,∞) (For a nonzero real c, dilation by c multiplies Lebesgue outer measure by ∣c∣n, and reflection in the origin preserves it), and a ball is contained in the axis-parallel cube Q(z,ρ)=∏i(zi−ρ,zi+ρ) of measure (2ρ)n (A box in Rn with parameters ai≤bi is Lebesgue measurable of measure ∏i<n(bi−ai), whichever of its faces are included).

[F3]

For a sequence of nonnegative measurable functions increasing to g, the integrals increase to ∫g (Monotone convergence for the integral).

[F4]

If A⊆B are measurable then ∫A∣f∣≤∫B∣f∣ (Measures are monotone).

Proof

technique · Decompose the far field into dyadic annuli, bound each annulus by the maximal function through its measure, and sum the resulting geometric series
1.1F1F2F3given

The sets Ak={t:2kr≤∣t−z∣<2k+1r}, k≥0, are pairwise disjoint measurable sets whose union is {∣t−z∣≥r}. Each partial sum ∑k<K∣f∣ ∣t−z∣−n−δ1Ak increases with K to ∣f(t)∣∣t−z∣−n−δ1{∣t−z∣≥r}, so monotone convergence [F3] gives ∫∣t−z∣≥r∣f(t)∣∣t−z∣−n−δdt=∑k≥0∫Ak∣f(t)∣∣t−z∣−n−δdt, and every term is finite because (2kr)−n−δ∫B(z,2k+1r)∣f∣<∞ by [F1] and [F2].

2.1F1F2F4step 1.1algebra

For t∈Ak one has ∣t−z∣−n−δ≤(2kr)−n−δ, and Ak⊆B(z,2k+1r)⊆Q(z,2k+1r), so [F4] and [F2] give ∫Ak∣f(t)∣∣t−z∣−n−δdt≤(2kr)−n−δ∫B(z,2k+1r)∣f∣≤(2kr)−n−δλ(B(z,2k+1r))Mf(z)≤(2kr)−n−δ(2k+2r)nMf(z)=22n2−kδr−δMf(z).

3.1step 1.1step 2.1algebra∎

Summing the geometric series in step 2.1 with ratio 2−δ<1 gives ∫∣t−z∣≥r∣f(t)∣∣t−z∣−n−δdt≤22n(1−2−δ)−1r−δMf(z), which is the asserted inequality with Cn,δ=22n(1−2−δ)−1.

Why the exponent range is δ>0. The endpoint δ=0 is not available: for the locally integrable function f=1B(0,R), the point z=0 and r=1 one has Mf(0)=1, while ∫∣t∣≥1∣f(t)∣∣t∣−ndt=∫1≤∣t∣≤R∣t∣−ndt=∣Sn−1∣log⁡R grows without bound as R→∞, by Polar coordinates decompose Lebesgue measure into r^{n-1} dr d sigma and The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t. Hence no constant independent of R can bound that integral by Mf(0); the divergence of ∑k≥02−kδ at δ=0 is not removable, and only exponents δ>0 occur in the Hölder estimates for standard kernels used on this page.

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