Real Analysis II, Winter 2018

Total Page:16

File Type:pdf, Size:1020Kb

Real Analysis II, Winter 2018 Real Analysis II, Winter 2018 From the Finnish original “Moderni reaalianalyysi”1 by Ilkka Holopainen adapted by Tuomas Hytönen February 22, 2018 1Version dated September 14, 2011 Contents 1 General theory of measure and integration 2 1.1 Measures . 2 1.11 Metric outer measures . 4 1.20 Regularity of measures, Radon measures . 7 1.31 Uniqueness of measures . 9 1.36 Extension of measures . 11 1.45 Product measure . 14 1.52 Fubini’s theorem . 16 2 Hausdorff measures 21 2.1 Basic properties of Hausdorff measures . 21 2.12 Hausdorff dimension . 24 2.17 Hausdorff measures on Rn ...................... 25 3 Compactness and convergence of Radon measures 30 3.1 Riesz representation theorem . 30 3.13 Weak convergence of measures . 35 3.17 Compactness of measures . 36 4 On the Hausdorff dimension of fractals 39 4.1 Mass distribution and Frostman’s lemma . 39 4.16 Self-similar fractals . 43 5 Differentiation of measures 52 5.1 Besicovitch and Vitali covering theorems . 52 1 Chapter 1 General theory of measure and integration 1.1 Measures Let X be a set and P(X) = fA : A ⊂ Xg its power set. Definition 1.2. A collection M ⊂ P (X) is a σ-algebra of X if 1. ? 2 M; 2. A 2 M ) Ac = X n A 2 M; S1 3. Ai 2 M, i 2 N ) i=1 Ai 2 M. Example 1.3. 1. P(X) is the largest σ-algebra of X; 2. f?;Xg is the smallest σ-algebra of X; 3. Leb(Rn) = the Lebesgue measurable subsets of Rn; 4. If M is a σ-algebra of X and A ⊂ X, then MjA = fB \ A : B 2 Mg is a σ-algebra of A. 5. If M is a σ-algebra of X and A 2 M, then MA = fB ⊂ X : B \ A 2 Mg is a σ-algebra of X. Definition 1.4. If F ⊂ P(X) is any family of subsets of X, then \ σ(F) = fM : M is a σ-algebra of X; F ⊂ Mg is the σ-algebra generated by F. It is the smallest σ-algebra that contains F. 2 Example 1.5. A subset I ⊂ Rn is an open n-interval if it has the form I = f(x1; : : : ; xn): aj < xj < bjg; where −∞ ≤ aj < bj ≤ +1. Then n n σ(fI : I is an n-intervalg) = σ(fA : A ⊂ R is openg) =: Bor(R ) is the σ-algebra of Borel sets of Rn. (Think why there is equality on the left.) n We observe that, in R , all open sets, closed sets, Gδ sets (countable inter- sections of open sets), Fσ sets (countable unions of closed sets), Fσδ sets, Gδσ sets, etc., are Borel sets. Thus e.g. the set Q of rational numbers is a Borel set. Remark 1.6. In every topological space X, one can define the Borel sets Bor(X) = σ(fA : A ⊂ X openg: Definition 1.7. Let M be a σ-algebra of X. A mapping µ : M! [0; +1] is a measure, if 1. µ(?) = 0, S1 P1 2. µ( i=1 Ai) = i=1 µ(Ai), if Ai 2 M are disjoint. The triplet (X; M; µ) is called a measure space and the elements of M measur- able sets. Condition (2) above is called countable additivity. The definition implies the monotonicity of the meusure: If A; B 2 M and A ⊂ B, then µ(A) ≤ µ(B). Remark 1.8. 1. If µ(X) < 1, the measure µ is finite. 2. If µ(X) = 1, then µ is a probability measure. S1 3. If X = i=1 Ai, where µ(Ai) < 1 for all i, the measure µ is σ-finite. We also say that X is σ-finite with respect to µ. 4. If A 2 M and µ(A) = 0, then A has (or is of) measure zero. 5. If X is a topological space and Bor(X) ⊂ M (i.e., every Borel set is measurable), then µ is a Borel measure. n n Example 1.9. 1. X = R , M = Leb R , µ = mn = Lebesgue measure. n n n 2. X = R , M = Bor R , µ = mnj Bor R = the restriction of the Lebesgue measure on Borel sets. 3. Let X 6= ? be any set. Fix x 2 X and define for all A ⊂ X ( 1; if x 2 A; µ(A) = 0; if x2 = A: Then µ : P(X) ! [0; +1] is a measure (so called Dirac measure at x). It is often denoted by µ = δx. 3 4. If f : Rn ! [0; 1] is Lebesgue measurable, then µ : Leb(Rn) ! [0; 1] defined by µ(E) = f(x)dmn(x) ˆE is a measure. (See course “Measure and integral”.) 5. If (X; M; µ) is a measure space and A 2 M, then µxA : MA ! [0; 1] defined by (µxA)(B) = µ(B \ A) is a measure. It is called the restriction of µ on A. Theorem 1.10. Let (X; M; µ) be a measure space and A1;A2;::: 2 M. 1 [ 1. If A1 ⊂ A2 ⊂ :::, then µ( Ai) = lim µ(Ai). i!1 i=1 1 \ 2. If A1 ⊃ A2 ⊃ ::: and µ(Ak) < 1 for some k, then µ( Ai) = lim µ(Ai). i!1 i=1 Proof. Measure and integral. 1.11 Metric outer measures Definition 1.12. A mapping µ~ : P(X) ! [0; +1] is an outer measure (or exterior measure) on X if 1. µ~(?) = 0; P1 S1 2. µ~(A) ≤ i=1 µ~(Ai), if A ⊂ i=1 Ai ⊂ X. Remark 1.13. 1. The outer measure is thus defined on all subsets of X. 2. Condition (2) implies the monotonicity of the outer measure, i.e., µ~(A) ≤ µ~(B) if A ⊂ B ⊂ X. 3. Many books (e.g. Evans–Gariepy, Mattila, . ) refer to outer measures simply as measures. 4. Let µ~ be an outer measure on X and A ⊂ X. Then its restriction to A, (~µxA)(B) =µ ~(B \ A); is an outer measure on X. Every outer measure defines a σ-algebra of “measurable” sets through the so called Carathéodory condition: 4 Definition 1.14. Let µ~ be an outer measure on X. A set E ⊂ X is µ~- measurable, or just measurable, if µ~(A) =µ ~(A \ E) +µ ~(A n E) for all A ⊂ X. Theorem 1.15. Let µ~ be an outer measure on X and M = Mµ~ = fE ⊂ X : E is µ~-measurableg: Then 1. M is a σ-algebram and 2. µ =µ ~jM is a measure (i.e., µ is countably additive). Proof. Measure and integral. Definition 1.16. An outer measure µ~ on a topological space X is called a Borel outer measure if every Borel set of X is µ~-measurable (i.e., the measure determined by µ~ is a Borel measure). We next investigate, when a given outer measure on a topological space X has this property. Definition 1.17 (Carathéodory). An outer measure µ~ on a metric space (X; d) is a metric outer measure if µ~(A [ B) =µ ~(A) +µ ~(B) for all A; B ⊂ X such that dist(A; B) = inffd(a; b): a 2 A; b 2 Bg > 0. Theorem 1.18. An outer measure µ~ on a metric space (X; d) is a Borel outer measure, if and only if µ~ is a metric outer measure. We begin with a lemma: Lemma 1.19. Let µ~ be a metric outer measure and A ⊂ G ⊂ X, where G is open. If c Ak = fx 2 A : dist(x; G ) ≥ 1=kg; k 2 N; then µ~(A) = limk!1 µ~(Ak). S1 Proof. Since G is open, we have A = k=1 Ak. Let Bk = Ak+1 n Ak: Then 1 1 [ [ A = A2n [ B2k [ B2k+1 ; k=n k=n so that 1 1 X X µ~(A) ≤ µ~(A2n) + µ~(B2k) + µ~(B2k+1) =µ ~(A2n) + (I)n + (II)n: k=n k=n 5 Consider the limit n ! 1. (1) If (I)n; (II)n ! 0 as n ! 1, then µ~(A) ≤ lim µ~(A2n) ≤ lim µ~(A2n+1) ≤ µ~(A); n!1 n!1 and the claim of the lemma is true. X (2) If (I)n 6! 0 as n ! 1, then µ~(B2n) = 1. n n−1 [ On the other hand, A ⊃ A2n ⊃ B2k; where k=1 1 1 dist(B ;B ) ≥ − > 0: 2k 2k+2 2k + 1 2k + 2 Since µ~ is a metric outer measure, it follows that n−1 n−1 X [ µ~(B2k) =µ ~ B2k ≤ µ~(A2n) ≤ µ~(A2n+1) ≤ µ~(A): k=1 k=1 As n ! 1, we deduce that µ~(A) = limk!1 µ~(Ak) = 1, and the claim of the lemma is true again. If (II)n 6! 0 as n ! 1, the argument is entirely similar. Proof of Theorem 1.18. Let us first assume that µ~ is a metric outer measure and prove that µ~ is a Borel outer measure. Since Bor(X) = σ(fF : F ⊂ X closedg) and Mµ~ is a σ-algebra, it suffices to prove that every closed set F ⊂ X is µ~-measurable. Let E ⊂ X be an arbitrary set, for which we check the Carathéodory condi- tion µ~(E) =µ ~(E \ F ) +µ ~(E n F ). We apply Lemma 1.19 with A = E n F ⊂ X n F = G: When Ak ⊂ A is as in the lemma, we have dist(Ak;F \ E) ≥ dist(Ak;F ) ≥ 1=k > 0; lim µ~(Ak) =µ ~(A) =µ ~(E n F ): k!1 By the assumption that µ~ is a metric outer measure and observing that Ak ⊂ A ⊂ E, we have µ~(Ak) +µ ~(F \ E) =µ ~(Ak [ (F \ E)) ≤ µ~(E): When k ! 1, the left-hand side tends to µ~(E n F ) +µ ~(F \ E), and we get the Carathéodory condition.
Recommended publications
  • Integral Representation of a Linear Functional on Function Spaces
    INTEGRAL REPRESENTATION OF LINEAR FUNCTIONALS ON FUNCTION SPACES MEHDI GHASEMI Abstract. Let A be a vector space of real valued functions on a non-empty set X and L : A −! R a linear functional. Given a σ-algebra A, of subsets of X, we present a necessary condition for L to be representable as an integral with respect to a measure µ on X such that elements of A are µ-measurable. This general result then is applied to the case where X carries a topological structure and A is a family of continuous functions and naturally A is the Borel structure of X. As an application, short solutions for the full and truncated K-moment problem are presented. An analogue of Riesz{Markov{Kakutani representation theorem is given where Cc(X) is replaced with whole C(X). Then we consider the case where A only consists of bounded functions and hence is equipped with sup-norm. 1. Introduction A positive linear functional on a function space A ⊆ RX is a linear map L : A −! R which assigns a non-negative real number to every function f 2 A that is globally non-negative over X. The celebrated Riesz{Markov{Kakutani repre- sentation theorem states that every positive functional on the space of continuous compactly supported functions over a locally compact Hausdorff space X, admits an integral representation with respect to a regular Borel measure on X. In symbols R L(f) = X f dµ, for all f 2 Cc(X). Riesz's original result [12] was proved in 1909, for the unit interval [0; 1].
    [Show full text]
  • Measure and Integration (Under Construction)
    Measure and Integration (under construction) Gustav Holzegel∗ April 24, 2017 Abstract These notes accompany the lecture course ”Measure and Integration” at Imperial College London (Autumn 2016). They follow very closely the text “Real-Analysis” by Stein-Shakarchi, in fact most proofs are simple rephrasings of the proofs presented in the aforementioned book. Contents 1 Motivation 3 1.1 Quick review of the Riemann integral . 3 1.2 Drawbacks of the class R, motivation of the Lebesgue theory . 4 1.2.1 Limits of functions . 5 1.2.2 Lengthofcurves ....................... 5 1.2.3 TheFundamentalTheoremofCalculus . 5 1.3 Measures of sets in R ......................... 6 1.4 LiteratureandFurtherReading . 6 2 Measure Theory: Lebesgue Measure in Rd 7 2.1 Preliminaries and Notation . 7 2.2 VolumeofRectanglesandCubes . 7 2.3 Theexteriormeasure......................... 9 2.3.1 Examples ........................... 9 2.3.2 Propertiesoftheexteriormeasure . 10 2.4 Theclassof(Lebesgue)measurablesets . 12 2.4.1 The property of countable additivity . 14 2.4.2 Regularity properties of the Lebesgue measure . 15 2.4.3 Invariance properties of the Lebesgue measure . 16 2.4.4 σ-algebrasandBorelsets . 16 2.5 Constructionofanon-measurableset. 17 2.6 MeasurableFunctions ........................ 19 2.6.1 Some abstract preliminary remarks . 19 2.6.2 Definitions and equivalent formulations of measurability . 19 2.6.3 Properties 1: Behaviour under compositions . 21 2.6.4 Properties 2: Behaviour under limits . 21 2.6.5 Properties3: Behaviourof sums and products . 22 ∗Imperial College London, Department of Mathematics, South Kensington Campus, Lon- don SW7 2AZ, United Kingdom. 1 2.6.6 Thenotionof“almosteverywhere”. 22 2.7 Building blocks of integration theory .
    [Show full text]
  • On Stochastic Distributions and Currents
    NISSUNA UMANA INVESTIGAZIONE SI PUO DIMANDARE VERA SCIENZIA S’ESSA NON PASSA PER LE MATEMATICHE DIMOSTRAZIONI LEONARDO DA VINCI vol. 4 no. 3-4 2016 Mathematics and Mechanics of Complex Systems VINCENZO CAPASSO AND FRANCO FLANDOLI ON STOCHASTIC DISTRIBUTIONS AND CURRENTS msp MATHEMATICS AND MECHANICS OF COMPLEX SYSTEMS Vol. 4, No. 3-4, 2016 dx.doi.org/10.2140/memocs.2016.4.373 ∩ MM ON STOCHASTIC DISTRIBUTIONS AND CURRENTS VINCENZO CAPASSO AND FRANCO FLANDOLI Dedicated to Lucio Russo, on the occasion of his 70th birthday In many applications, it is of great importance to handle random closed sets of different (even though integer) Hausdorff dimensions, including local infor- mation about initial conditions and growth parameters. Following a standard approach in geometric measure theory, such sets may be described in terms of suitable measures. For a random closed set of lower dimension with respect to the environment space, the relevant measures induced by its realizations are sin- gular with respect to the Lebesgue measure, and so their usual Radon–Nikodym derivatives are zero almost everywhere. In this paper, how to cope with these difficulties has been suggested by introducing random generalized densities (dis- tributions) á la Dirac–Schwarz, for both the deterministic case and the stochastic case. For the last one, mean generalized densities are analyzed, and they have been related to densities of the expected values of the relevant measures. Ac- tually, distributions are a subclass of the larger class of currents; in the usual Euclidean space of dimension d, currents of any order k 2 f0; 1;:::; dg or k- currents may be introduced.
    [Show full text]
  • Dirichlet Is Natural Vincent Danos, Ilias Garnier
    Dirichlet is Natural Vincent Danos, Ilias Garnier To cite this version: Vincent Danos, Ilias Garnier. Dirichlet is Natural. MFPS 31 - Mathematical Foundations of Program- ming Semantics XXXI, Jun 2015, Nijmegen, Netherlands. pp.137-164, 10.1016/j.entcs.2015.12.010. hal-01256903 HAL Id: hal-01256903 https://hal.archives-ouvertes.fr/hal-01256903 Submitted on 15 Jan 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. MFPS 2015 Dirichlet is natural Vincent Danos1 D´epartement d'Informatique Ecole normale sup´erieure Paris, France Ilias Garnier2 School of Informatics University of Edinburgh Edinburgh, United Kingdom Abstract Giry and Lawvere's categorical treatment of probabilities, based on the probabilistic monad G, offer an elegant and hitherto unexploited treatment of higher-order probabilities. The goal of this paper is to follow this formulation to reconstruct a family of higher-order probabilities known as the Dirichlet process. This family is widely used in non-parametric Bayesian learning. Given a Polish space X, we build a family of higher-order probabilities in G(G(X)) indexed by M ∗(X) the set of non-zero finite measures over X. The construction relies on two ingredients.
    [Show full text]
  • (Measure Theory for Dummies) UWEE Technical Report Number UWEETR-2006-0008
    A Measure Theory Tutorial (Measure Theory for Dummies) Maya R. Gupta {gupta}@ee.washington.edu Dept of EE, University of Washington Seattle WA, 98195-2500 UWEE Technical Report Number UWEETR-2006-0008 May 2006 Department of Electrical Engineering University of Washington Box 352500 Seattle, Washington 98195-2500 PHN: (206) 543-2150 FAX: (206) 543-3842 URL: http://www.ee.washington.edu A Measure Theory Tutorial (Measure Theory for Dummies) Maya R. Gupta {gupta}@ee.washington.edu Dept of EE, University of Washington Seattle WA, 98195-2500 University of Washington, Dept. of EE, UWEETR-2006-0008 May 2006 Abstract This tutorial is an informal introduction to measure theory for people who are interested in reading papers that use measure theory. The tutorial assumes one has had at least a year of college-level calculus, some graduate level exposure to random processes, and familiarity with terms like “closed” and “open.” The focus is on the terms and ideas relevant to applied probability and information theory. There are no proofs and no exercises. Measure theory is a bit like grammar, many people communicate clearly without worrying about all the details, but the details do exist and for good reasons. There are a number of great texts that do measure theory justice. This is not one of them. Rather this is a hack way to get the basic ideas down so you can read through research papers and follow what’s going on. Hopefully, you’ll get curious and excited enough about the details to check out some of the references for a deeper understanding.
    [Show full text]
  • Probability Measures on Metric Spaces
    Probability measures on metric spaces Onno van Gaans These are some loose notes supporting the first sessions of the seminar Stochastic Evolution Equations organized by Dr. Jan van Neerven at the Delft University of Technology during Winter 2002/2003. They contain less information than the common textbooks on the topic of the title. Their purpose is to present a brief selection of the theory that provides a basis for later study of stochastic evolution equations in Banach spaces. The notes aim at an audience that feels more at ease in analysis than in probability theory. The main focus is on Prokhorov's theorem, which serves both as an important tool for future use and as an illustration of techniques that play a role in the theory. The field of measures on topological spaces has the luxury of several excellent textbooks. The main source that has been used to prepare these notes is the book by Parthasarathy [6]. A clear exposition is also available in one of Bour- baki's volumes [2] and in [9, Section 3.2]. The theory on the Prokhorov metric is taken from Billingsley [1]. The additional references for standard facts on general measure theory and general topology have been Halmos [4] and Kelley [5]. Contents 1 Borel sets 2 2 Borel probability measures 3 3 Weak convergence of measures 6 4 The Prokhorov metric 9 5 Prokhorov's theorem 13 6 Riesz representation theorem 18 7 Riesz representation for non-compact spaces 21 8 Integrable functions on metric spaces 24 9 More properties of the space of probability measures 26 1 The distribution of a random variable in a Banach space X will be a probability measure on X.
    [Show full text]
  • Some Undecidability Results Concerning Radon Measures by R
    transactions of the american mathematical society Volume 259, Number 1, May 1980 SOME UNDECIDABILITY RESULTS CONCERNING RADON MEASURES BY R. J. GARDNER AND W. F. PFEFFER Abstract. We show that in metalindelöf spaces certain questions about Radon measures cannot be decided within the Zermelo-Fraenkel set theory, including the axiom of choice. 0. Introduction. All spaces in this paper will be Hausdorff. Let A be a space. By § and Q we shall denote, respectively, the families of all open and compact subsets of X. The Borel o-algebra in X, i.e., the smallest a-algebra in X containing ê, will be denoted by <®. The elements of 9> are called Borel sets. A Borel measure in A' is a measure p on % such that each x G X has a neighborhood U G % with p( U) < + 00. A Borel measure p in X is called (i) Radon if p(B) = sup{ p(C): C G G, C c F} for each F G % ; (ii) regular if p(B) = inî{ p(G): G G @,B c G} for each fieS. A Radon space is a space X in which each finite Borel measure is Radon. The present paper will be divided into two parts, each dealing with one of the following questions. (a) Let A' be a locally compact, hereditarily metalindelöf space with the counta- ble chain condition. Is X a Radon space? (ß) Let A' be a metalindelöf space, and let p be a a-finite Radon measure in X. Is pa. regular measure? We shall show that neither question can be decided within the usual axioms of set theory.
    [Show full text]
  • Some Special Results of Measure Theory
    Some Special Results of Measure Theory By L. Le Cam1 U.C. Berkeley 1. Introduction The purpose of the present report is to record in writing some results of measure theory that are known to many people but do not seem to be in print, or at least seem to be difficult to find in the printed literature. The first result, originally proved by a consortium including R.M. Dudley, J. Feldman, D. Fremlin, C.C. Moore and R. Solovay in 1970 says something like this: Let X be compact with a Radon measure µ.Letf be a map from X to a metric space Y such that for every open set S ⊂ Y the inverse image, f −1(S) is Radon measurable. Then, if the cardinality of f(X)isnot outlandishly large, there is a subset X0 ⊂ X such that µ(X\X0)=0and f(X0) is separable. Precise definition of what outlandishly large means will be given below. The theorem may not appear very useful. However, after seeing it, one usually looks at empirical measures and processes in a different light. The theorem could be stated briefly as follows: A measurable image of a Radon measure in a complete metric space is Radon. Section 6 Theorem 7 gives an extension of the result where maps are replaced by Markov kernels. Sec- tion 8, Theorem 9, gives an extension to the case where the range space is paracompact instead of metric. The second part of the paper is an elaboration on certain classes of mea- sures that are limits in a suitable sense of “molecular” ones, that is measures carried by finite sets.
    [Show full text]
  • EXISTENCE of HAAR MEASURE Most of the Measure Theory We've Done in This Class Has Been Within Subsets of Rn, Even Though Measu
    EXISTENCE OF HAAR MEASURE ARUN DEBRAY NOVEMBER 19, 2015 Abstract. In this presentation, I will prove that every compact topological group has a unique left-invariant measure with total measure 1. This presentation is for UT’s real analysis prelim class. Most of the measure theory we’ve done in this class has been within subsets of Rn, even though measures are very general tools. Today, we will talk about a measure defined on a larger class of spaces, which generalizes the usual Lesbegue measure. I will define and prove its existence; Spencer will prove its uniqueness and provide some interesting examples; and Gill will talk about an application to harmonic analysis. Definition. A topological group is a topological space G with a group structure: an identity, an associative multiplication map, and an inverse map, such that multiplication G G G and inversion G G are both continuous. × ! ! There are many examples, including Rn under addition; all Lie groups; and all finite groups (with the discrete topology). Since a topological group G has a topology, we can talk about the σ-algebra of Borel sets on it, as usual generated by the open sets. But the group structure means we can also talk about left- and right-invariance: for every g G, we have continuous maps ` : G G and r : G G, sending x gx and x xg, respectively. 2 g ! g ! 7! 7! These should be read “left (resp. right) translation by g” (or “multiplication,” or “action”). Often, we want something to be invariant under these maps. Specifically, we say that a measure is left-invariant if µ(S) = µ(g S) for all g G, and define right-invariance similarly.
    [Show full text]
  • Measure and Integration
    Appendix Measure and Integration In this appendix we collect some facts from measure theory and integration which are used in the book. We recall the basic definitions of measures and integrals and give the central theorems of Lebesgue integration theory. Proofs may be found for instance in [Rud87]. A.1 Measurable Functions and Integration Let X be a set. A σ -algebra on X is a set A, whose elements are subsets of X, such that • the empty set lies in A and if A ∈ A, then its complement X A lies in A, • the set A is closed under countable unions. It follows that a σ -algebra is closed under countable sections and that with A,B the set A B lies in A. The set P(X) of all subsets of X is a σ -algebra and the intersection of arbitrary many σ -algebras is a σ -algebra. This implies that for an arbitrary set S ⊂ P(X) there exists a smallest σ -algebra A containing S. In this case we say that S gen- erates A. For a topological space X,theσ -algebra B = B(X) generated by the topology of X, is called the Borel σ -algebra of X. The elements of B(X) are called Borel sets.IfA is a σ -algebra on X, then the pair (X, A) is called a measurable space. The elements of A are called measurable sets. Amapf : X → Y between two measurable spaces is called a measurable map −1 if the preimage f (A) is measurable for every measurable set A ∈ AY .
    [Show full text]
  • 5.2 Complex Borel Measures on R
    MATH 245A (17F) (L) M. Bonk / (TA) A. Wu Real Analysis Contents 1 Measure Theory 3 1.1 σ-algebras . .3 1.2 Measures . .4 1.3 Construction of non-trivial measures . .5 1.4 Lebesgue measure . 10 1.5 Measurable functions . 14 2 Integration 17 2.1 Integration of simple non-negative functions . 17 2.2 Integration of non-negative functions . 17 2.3 Integration of real and complex valued functions . 19 2.4 Lp-spaces . 20 2.5 Relation to Riemann integration . 22 2.6 Modes of convergence . 23 2.7 Product measures . 25 2.8 Polar coordinates . 28 2.9 The transformation formula . 31 3 Signed and Complex Measures 35 3.1 Signed measures . 35 3.2 The Radon-Nikodym theorem . 37 3.3 Complex measures . 40 4 More on Lp Spaces 43 4.1 Bounded linear maps and dual spaces . 43 4.2 The dual of Lp ....................................... 45 4.3 The Hardy-Littlewood maximal functions . 47 5 Differentiability 51 5.1 Lebesgue points . 51 5.2 Complex Borel measures on R ............................... 54 5.3 The fundamental theorem of calculus . 58 6 Functional Analysis 61 6.1 Locally compact Hausdorff spaces . 61 6.2 Weak topologies . 62 6.3 Some theorems in functional analysis . 65 6.4 Hilbert spaces . 67 1 CONTENTS MATH 245A (17F) 7 Fourier Analysis 73 7.1 Trigonometric series . 73 7.2 Fourier series . 74 7.3 The Dirichlet kernel . 75 7.4 Continuous functions and pointwise convergence properties . 77 7.5 Convolutions . 78 7.6 Convolutions and differentiation . 78 7.7 Translation operators .
    [Show full text]
  • 2.1 Examples
    2.1 Examples Definition 2.1.1. Let (X; B; υ) be a σ-finite measure space, and let Γ be a countable group, an action ΓyX such that γ−1(B) = B, for all γ 2 Γ is mea- sure preserving if for each measurable set A 2 B we have υ(γ−1A) = υ(A). Alternately, we will say that υ is an invariant measure for the action Γy(X; B). We'll say that Γ preserves the measure class of υ, or alternately, υ is a quasi- invariant measure, if for each γ 2 Γ, and A 2 B we have that υ(A) = 0 if and −1 only if υ(γ A) = 0, i.e., for each γ 2 Γ, the push-forward measure γ∗υ defined −1 by γ∗υ(A) = υ(γ A) for all A 2 B is absolutely continuous with respect to υ. Note, that since the action ΓyX is measurable we obtain an action σ : Γ ! Aut(M(X; B)) of Γ on the B-measurable functions by the formula σγ (f) = f ◦ γ−1. If Γy(X; B; υ) preserves the measure class of υ, then for each γ 2 Γ there dγ∗υ exists the Radon-Nikodym derivative dυ : X ! [0; 1), such that for each measurable set A 2 B we have Z dγ υ υ(γ−1A) = 1 ∗ dυ: A dυ The Radon-Nikodym derivative is unique up to measure zero for υ. If γ1; γ2 2 Γ, and A 2 B then we have Z −1 dγ2∗υ υ((γ1γ2) A) = 1γ−1A dυ 1 dυ Z dγ υ Z dγ υ dγ υ = 1 σ ( 2∗ ) dγ υ = 1 σ ( 2∗ ) 1∗ dυ: A γ1 dυ 1∗ A γ1 dυ dυ Hence, we have almost everywhere d(γ γ ) υ dγ υ dγ υ 1 2 ∗ = σ ( 2∗ ) 1∗ : dυ γ1 dυ dυ dγ∗υ × Or, in other words, the map (γ; x) 7! dυ (γx) 2 R is a cocycle almost every- where.
    [Show full text]