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Exercise 1.6.19 (Hardy-Littlewood maximal inequality II)
Let be an absolutely integrable function, and let . Then
Answers
We prove the Hardy-Littlewood inequality, which we will do with the constant . It suffices to verify the claim with strict inequality,
as the non-strict case then follows by perturbing slightly and then taking limits. Thus, fix and . By inner regularity (Exercise 1.2.15), it suffices to show that
and then takes supremum over . Hence, let be arbitrary. By definition of , for each there exists a such that
By the axiom of choice we construct a collection of such balls with . In other words, is an open cover of . By compactness, we then must be able to find a finite subcover of . We now introduce an algorithm (similar to the one provided in Vitali lemma to construct a disjoint subcollection of ) such that its doubled version covers . The trick is to introduce a tolerance of .
- (i)
- Around each consider the ball (notice the epsilon! - we have made the balls smaller than originally thought). Then obviously is an open cover of . Thus, by compactness of there exists a finite subcover which still covers all of the .
- (ii)
- If covers , then so does 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
of
such
that
and
We now argue that the constant can be improved to 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 were contained in and not just in .
- (iv)
- At this stage we employ the main trick. Instead of showing that
(which is not necessarily true in the middle), we give ourselves an epsilon of room and show instead that
Thus, pick an arbitrary from the original collection . By Vitali construction in the previous step, there exists a of minimal such that . Also by construction. By triangle inequality, this implies that the centre of the ball is contained inside :
From here we see that the smaller ball has a non-empty intersection with as well. Furthermore, we see that it paid off to take an epsilon of room as we obtain by triangle inequality:
We now integrate this into the proof of the Hardy-Littlewood theorem. We have shown
to be true.
We cannot take infimum as as and may explode; instead, we rewrite the above using an upper bound for measure without involving :
Now we can safely take to and obtain the desired result.