Littlewood's First Principle: Difference between revisions
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Littlewood stated the principles in his 1944 ''Lectures on the Theory of Functions'' <ref> | Littlewood stated the principles in his 1944 ''Lectures on the Theory of Functions'' <ref> Littlewood, J. E. ''Lectures on the Theory of Functions''. Oxford University Press, 1944.: | ||
<blockquote> There are three principles, roughly expressible in the following terms: Every (measurable) set is nearly a finite sum of intervals; every function (of class ''L''<sup>p</sup>) is nearly continuous; every convergent sequence of functions is nearly uniformly convergent.}} </blockquote> | <blockquote> There are three principles, roughly expressible in the following terms: Every (measurable) set is nearly a finite sum of intervals; every function (of class ''L''<sup>p</sup>) is nearly continuous; every convergent sequence of functions is nearly uniformly convergent.}} </blockquote> |
Revision as of 23:05, 19 December 2020
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Approximation by Compact Sets
The main result is the following: Let </math> E </math> be a Borel measurable set. For every </math>\varepsilon > 0</math> there exists an open set </math> U </math> with </math> E\subset U </math> such that </math> m(E)>m(U)-\varepsilon </math>. Note that this implies </math> 0< m(U)-m(E)<\varepsilon </math> by monotonicity.
Proof: First suppose </math> E </math> is bounded. If </math> E </math> is also closed, then we're done; </math> E </math> is compact. Otherwise, the boundary </math> \partial{E}=\overline{E}\backslash E </math> is nonempty. Now, </math> \partial{E} </math> is a Borel measurable set, so we can approximate it from above by the previous section. That is, there exists an open set </math> U\supset \partial{E} </math> such that </math> m(U) < m(\overline{E}\backslash E) +\varepsilon = \varepsilon </math>. Now define </math> K= \overline{E} \backslash U </math>. By construction, this set is contained in </math> U </math>. Moreover, it is closed, being the intersection of two closed sets. Finally, </math> K </math> is bounded because </math> E </math> is bounded. By the Heine-Borel Theorem, </math> K </math> is compact, and </math> K </math> satisfies the constraints of the theorem because
Littlewood's First Principle
The previous two results imply the following formulation of Littlewood's First Principle: If </math> E </math> is a Borel measurable set and </math> m(E)<+\infty </math>, then for every </math> \varepsilon > 0</math> there is a set </math> A </math> that is a finite union of open intervals such that </math> m(A\delta E) < \varepsilon </math>, where </math> \delta </math> denotes symmetric difference.
Proof: Using the previous two sections find </math> K </math> and </math> U </math> such that </math> K\subset E \subset U </math> and </math> m(E)-\epsilon < m(K) </math> and </math> m(E)+\epsilon > m(U) </math>. As noted in the proof of the first section, </math> U </math> is really a countable union of open intervals. These intervals form an open cover for </math> K </math> and since </math> K </math> is compact, only finitely many cover </math> K </math>. Defining </math> A </math> to be the union of these finitely many intervals, the result follows, since </math> m(A/E) \leq m(U/E) </math> and </math> m(E/A) \leq m(E/K) </math>.
References
- ↑ Gerald B. Folland, Real Analysis: Modern Techniques and Their Applications, second edition, §2.3