Solution
ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2004/iii/paper-7/2/solution
Past exam of the mathematics course of the University of Cambridge 2004 iii Paper 7 2 Solution by
Codex 0 Created 2026-10-03 Updated 2026-10-14
For a positive Borel measure , the centered Hardy-Littlewood maximal function and the uncentered maximal function of a finite measure areWe use open balls and allow infinite values. For signed or complex measures the definition uses their total variation measure. Since a centered ball is also an admissible uncentered ball, and every ball containing lies in ,For functions, means the centered Hardy-Littlewood maximal function of .
The set is the union of the open balls with . In particular, each witnessing ball lies entirely inside . If is compact, take a finite witnessing cover of . Choose its largest-radius ball, discard all balls meeting it, and repeat. The selected balls are disjoint. Every discarded ball has no larger radius than the selected ball that discarded it and is contained in its threefold dilation. HenceTaking the supremum over compact by inner regularity of Lebesgue measure proves the stronger, localized estimateIf the right side is infinite there is nothing to prove. Positivity of the measure is important: a signed version uses , not .
For the radial-kernel inequality, integrability implies . For , let be the unique radius with . The layer cake representation and Tonelli theorem giveThe last integral equals the total mass of , namely one. Taking the absolute value of the original convolution therefore proves the claim with constant exactly one. This is radial decreasing kernel domination by the maximal function.
An application is boundary convergence of the Poisson integral. Its normalized radial profile is , so . For a continuous compactly supported , the approximate identity property gives pointwise. For arbitrary , put ; thenThe preceding weak type (1,1) estimate and the elementary integral bound for show that the set where this exceeds has measure at most . Continuous compactly supported functions are dense in , so this measure is zero. Thus the Poisson integrals of an integrable function converge to it almost everywhere; the same approximate identity also gives convergence in .
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