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Exercise 1.6.19 (Hardy-Littlewood maximal inequality II)

Let f : d be an absolutely integrable function, and let λ > 0. Then

m ( {x d : sup r>0 1 m(B(x,r))B(x,r)|f|dm λ}) 2d λ d|f|dm.

Answers

We prove the Hardy-Littlewood inequality, which we will do with the constant Cd := 2d. It suffices to verify the claim with strict inequality,

m ( {x d : sup r>0 1 m(B(x,r))B(x,r)|f|dm > λ}) 2d λ d|f|dm

as the non-strict case then follows by perturbing λ slightly and then taking limits. Thus, fix f and λ. By inner regularity (Exercise 1.2.15), it suffices to show that

 compact K {x d : sup r>0 1 m(B(x,r))B(x,r)|f|dm > λ} : m(K) 2d λ d|f|dm

and then takes supremum over K. Hence, let K be arbitrary. By definition of K, for each x K there exists a r > 0 such that

1 m(B(x,r))B(x,r)|f|dm > λ

By the axiom of choice we construct a collection B(x,rx)xK of such balls with K r>0B(x,rx). In other words, B(x,rx)xK is an open cover of K. By compactness, we then must be able to find a finite subcover B1,,Bn of B(x,rx)xK. We now introduce an algorithm (similar to the one provided in Vitali lemma to construct a disjoint subcollection B1,,Bm of B1,,Bn) such that its doubled version covers K. The trick is to introduce a tolerance of 𝜖 (0,1).

(i)
Around each x K consider the ball B(x,𝜖rx)xK (notice the epsilon! - we have made the balls smaller than originally thought). Then obviously xKB(x,𝜖rx) is an open cover of K. Thus, by compactness of K there exists a finite subcover B(xi,𝜖ri)1in which still covers all of the K.
(ii)
If B(xi,𝜖ri)1in covers K, then so does B(xi,ri)1in as it is simply a larger cover.
(iii)
Using the same construction steps as we used for the Vitali covering lemma (Exercise 1.6.18) we construct a disjoint subcollection B(x(j),r(j))1jm of B(xi,ri)1in such that r(1) r(m) and
K j=1mB(x (j),3 r(j))

We now argue that the constant 3 can be improved to 2 in the above statement by noticing that in the construction used to prove the Vitali covering lemma (Exercise 1.6.18), the centres of the balls Bi,1 i n were contained in j=1m2Bj and not just in j=1m3Bj.

(iv)
At this stage we employ the main trick. Instead of showing that
K i=1nB(x i,ri) j=1mB(x (j),2r(j))

(which is not necessarily true in the middle), we give ourselves an epsilon of room and show instead that

K i=1nB(x i,𝜖ri) j=1mB(x (j),(2 + 𝜖)r(j)).

Thus, pick an arbitrary B(xi,𝜖ri) from the original collection B(xi,𝜖ri)1in. By Vitali construction in the previous step, there exists a B(x(j),r(j)) of minimal j m such that B(xi,ri) B(x(j),r(j)). Also r(j) ri by construction. By triangle inequality, this implies that the centre xi of the ball B(xi,ri) is contained inside B(x(j),2 r(j)):

for z Bi B(j) : d(xi,x(j)) d(xi,z) + d(z,x(j)) ri + r(j) 2r(j)

From here we see that the smaller ball B(xi,𝜖ri) has a non-empty intersection with B(x(j),2 r(j)) as well. Furthermore, we see that it paid off to take an epsilon of room as we obtain B(xi,𝜖ri) B(x(j),(2 + 𝜖)r(j)) by triangle inequality:

p B(xi,𝜖ri) : d(p,x(j)) d(p,xi) + d(xi,x(j)) 𝜖ri + 2r(j) r(j)(2 + 𝜖)

We now integrate this into the proof of the Hardy-Littlewood theorem. We have shown

𝜖 > 0 : K i=1n𝜖 B (xi,𝜖ri) j=1m𝜖 B (x(j),(2 + 𝜖)r(j))

to be true.

We cannot take infimum as 𝜖 0 as n and m may explode; instead, we rewrite the above using an upper bound for measure without involving m:

𝜖 > 0 : m (K) m ( i=1nB (x i,𝜖ri)) m ( j=1mB (x (j),(2 + 𝜖)r(j))) = (2 + 𝜖)d j=1mm (B (x (j),r(j))) (2 + 𝜖)d j=1m1 λB(x(j),r(j))|f|dm (2 + 𝜖)d λ d|f|dm.

Now we can safely take 𝜖 to 0 and obtain the desired result.

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2021-04-16 00:00
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