Lecture 3 Measures

Total Page:16

File Type:pdf, Size:1020Kb

Lecture 3 Measures MA40042 Measure Theory and Integration The triple (X; Σ; µ) is called a measure space. Recall that a sequence (An) of sets is disjoint (or `pairwise disjoint') if Ai \ Aj Lecture 3 for i 6= j. Measures 3.2 Examples The following are measures. (Checking they really are measures is a homework • Definition of measure problem.) • Examples of measures • Let X be a nonempty set, and let Σ be its powerset. For A 2 Σ, the count- ing measure # is given by setting #(A) to be the cardinality of A. (Re- • Basic properties and call that a set A has cardinality n if its elements can be enumerated as continuity of measure A = fa1; a2; : : : ; ang, and has cardinality 1 otherwise. The empty set has cardinality 0.) • Probability, finite, and σ-finite measures • Let (X; Σ) be a measurable space, and let x 2 X. Then the Dirac measure (or δ measure or point measure) at x of a set A 2 Σ is given by ( 1 if x 2 A, 3.1 Definition δx(A) = 0 if x2 = A. Recall from Lecture 0 the properties we wanted a measure to have: • A measure is a function µ from measurable subsets of X to [0; 1]. (Here, • Let X be a countable set, and let Σ be its powerset. Associate with each [0; 1] := [0; 1) [ f1g.) x 2 X a `weight' wx 2 [0; 1]. Then the associated discrete measure is • µ( ) = 0. X X ? µ(A) = wx = wxδx(A): • For a finite or countably infinite sequence of disjoint measurable sets, x2A x2X S P µ ( An) = µ(An). n n • Let X be a nonempty set, and let Σ be the σ-algebra of countable and co- S • For a finite or countably infinite sequence of measurable sets, µ ( n An) ≤ countable sets. Then we can set P µ(A ). n n ( 0 if A is countable, • µ(A) + µ(Ac) = µ(X). µ(A) = 1 otherwise We take some of these as a definition, and prove the rest as properties later. Definition 3.1. Let (X; Σ) be a measurable space. Then a function µ:Σ ! [0; 1] • The Lebesgue measure on R is the unique measure λ on the measurable space is a measure on (X; Σ) if (R; B) such that λ [a; b) = b − a. Showing that this measure exists and is unique is highly nontrivial (and will take about four lectures' work). 1. µ(?) = 0; 2. µ is countably additive, in that if A1;A2;:::; is a countably infinite sequence 3.3 Properties of disjoint sets in Σ, then Let's start with some simple properties. 1 ! 1 [ X µ An = µ(An): Theorem 3.2. Let (X; Σ; µ) be a measure space. Then we have the following n=1 n=1 properties: (Finite additivity) For A1;A2;:::;AN a finite sequence of disjoint sets in Σ, we (Downward continuity) For A1 ⊃ A2 ⊃ · · · a countably infinite `contracting' se- have quence of sets in Σ with µ(A1) < 1, we have N ! N [ X 1 ! µ An = µ(An): \ lim µ(An) = µ An : n=1 n=1 n!1 n=1 (Monotonicity) For A; B 2 Σ with A ⊂ B, we have µ(A) ≤ µ(B). Proof. We'll prove upward continuity, and leave downward continuity for home- (Countable subadditivity) For A1;A2;:::; a countably infinite sequence of sets in work. Σ, we have Write B1 = A1, and Bn = An n An−1 for n ≥ 2. Then 1 ! 1 [ X N 1 1 µ An ≤ µ(An): [ [ [ Bn = AN and Bn = An; n=1 n=1 n=1 n=1 n=1 (Finite subadditivity) For A1;A2;:::;AN a finite sequence of sets in Σ, we have with the unions being disjoint. So by finite additivity we have N ! N N ! N [ X [ X µ An ≤ µ(An): µ(AN ) = µ Bn = µ(Bn): n=1 n=1 n=1 n=1 Hence, by countable additivity, Also, for A 2 Σ, we have µ(A) + µ(Ac) = µ(X). N 1 1 ! 1 ! Proof. Most of these are left for homework, but let's do monotonicity (assuming X X [ [ µ(AN ) = µ(Bn) ! µ(Bn) = µ Bn = µ An finite additivity) for an example. n=1 n=1 n=1 n=1 We can write B = A [ (B n A), where the set difference B n A was shown to as N ! 1. be measurable in Lecture 1. Note also that the A and B n A are disjoint. Hence by finite additivity we have µ(B) = µ(A) + µ(B n A). But µ(B n A) ≥ 0, as µ:Σ ! [0; 1]. Hence µ(B) ≥ µ(A). 3.4 Probability measures A probability measure fulfils the definition of a measure, but also `adds up to 1'. This proof illustrates a general rule: to prove a statement about measures, turn it into a statement about disjoint unions. Definition 3.4. Let (X; Σ; µ) be a measure space. The following properties are known as `continuity of measure', by analogy with • If µ(X) = 1, then we call µ a probability measure, and (X; Σ; µ) a probability the usual definition of continuity, that space. lim f(xn) = f lim xn : • If µ(X) < 1, then we call µ a finite measure. n!1 n!1 For the `limit' of a sequence of sets, we can think of the union of a sequence of • If X can be written as a countable union of sets in Σ with finite measure, then expanding sets (an `upward limit'), or the intersection of a sequence of contracting we call µ a σ-finite measure. sets (a `downward limit'). A probability space is usually written as (Ω; F; P). Note that it follows from Theorem 3.2 that (A) ≤ 1 and (Ac) = 1 − (A) for all A 2 F. Theorem 3.3. Let (X; Σ; µ) be a measure space. Then we have the following P P P Probability measures are well-behaved, and your intuition is useful in dealing properties: with them. Finite measure behave essentially the same as probability measures, (Upward continuity) For A1 ⊂ A2 ⊂ · · · a countably infinite `expanding' sequence and σ-finite measures are fairly well-behaved too. Measures that are not σ-finite of sets in Σ, we have can be pretty weird. 1 ! [ Matthew Aldridge lim µ(An) = µ An : n!1 [email protected] n=1.
Recommended publications
  • 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]
  • 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 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]
  • 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.
    [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]
  • Math 595: Geometric Measure Theory
    MATH 595: GEOMETRIC MEASURE THEORY FALL 2015 0. Introduction Geometric measure theory considers the structure of Borel sets and Borel measures in metric spaces. It lies at the border between differential geometry and topology, and services a variety of areas: partial differential equations and the calculus of variations, geometric function theory, number theory, etc. The emphasis is on sets with a fine, irregular structure which cannot be well described by the classical tools of geometric analysis. Mandelbrot introduced the term \fractal" to describe sets of this nature. Dynamical systems provide a rich source of examples: Julia sets for rational maps of one complex variable, limit sets of Kleinian groups, attractors of iterated function systems and nonlinear differential systems, and so on. In addition to its intrinsic interest, geometric measure theory has been a valuable tool for problems arising from real and complex analysis, harmonic analysis, PDE, and other fields. For instance, rectifiability criteria and metric curvature conditions played a key role in Tolsa's resolution of the longstanding Painlev´eproblem on removable sets for bounded analytic functions. Major topics within geometric measure theory which we will discuss include Hausdorff measure and dimension, density theorems, energy and capacity methods, almost sure di- mension distortion theorems, Sobolev spaces, tangent measures, and rectifiability. Rectifiable sets and measures provide a rich measure-theoretic generalization of smooth differential submanifolds and their volume measures. The theory of rectifiable sets can be viewed as an extension of differential geometry in which the basic machinery and tools of the subject (tangent spaces, differential operators, vector bundles) are replaced by approxi- mate, measure-theoretic analogs.
    [Show full text]
  • Measure Theory
    Measure Theory Mark Dean Lecture Notes for Fall 2015 PhD Class in Decision Theory - Brown University 1Introduction Next, we have an extremely rapid introduction to measure theory. Given the short time that we have to spend on this, we are really only going to be able to introduce the relevant concepts, and try to give an idea of why they are important. For more information, Efe Ok has an as-yet unpublished book available online here https://files.nyu.edu/eo1/public/ that covers the basics, and points the way to many other classic texts. For those of you who are thinking of taking decision theory more seriously, then a taking a course in measure theory is probably advisable. Take some underlying set . Measure theory is the study of functions that map subsets of into the real line, with the interpretation that this number is the ’measure’ or the ’size’ or the ’volume’ of that set. Of course, not every function defined on a subset of 2 is going to fitinto our intuitive notion of how a measure should behave. In particular, we would like a measure to have at least the following two properties: 1. () 0 \ ≥ 2. ( )= ∞ For any pairwise disjoint sets ∪∞=1 =1 P The first property says that we can’t have negatively measured sets, the second says, if we look at the measure of the union of disjoint sets should be equal to the sum of the measure of those sets. Both these properties should seem appealing if we think about what we intuitively mean by ’measure’.
    [Show full text]
  • Arxiv:1206.1727V1 [Math.GN] 8 Jun 2012 7 .8]Ta H Aoia Map Canonical the That C.182] [7, Aua Oooy ..Tetplg Fuiomconvergence Uniform of Topology the I.E
    Математичнi Студiї. Т.5, №1-2 Matematychni Studii. V.5, No.1-2 УДК 515.12 T.O. Banakh TOPOLOGY OF PROBABILITY MEASURE SPACES, II: BARYCENTERS OF PROBABILITY RADON MEASURES AND METRIZATION OF THE FUNCTORS Pτ AND Pˆ. T.Banakh. Topology of probability measure spaces, II: barycenters of probability Radon measures and metrization of the functors Pτ and Pˆ, Mat. Stud. 5:1-2 (1995) 88–106. This paper is a follow-up to the author’s work [1] devoted to investigation of the functors Pτ and Pˆ of spaces of probability τ-smooth and Radon measures. In this part, we study the barycenter map for spaces of Radon probability measures. The obtained results are applied to show that the functor Pˆ is monadic in the category of metrizable spaces. Also we show that the functors Pˆ and Pτ admit liftings to the category BMetr of bounded metric spaces and also to the category Unif of uniform spaces, and investigate properties of those liftings. Т.Банах. Топология пространств вероятностных мер, II: барицентры вероятностных радоновских мер и метризация функторов Pτ и Pˆ // Мат. Студiї. 1995. – Т.5, №1-2. C.88–106. This paper is a follow-up to the author’s article [1], where the functors Pτ and Pˆ of spaces of proba- bility τ-smooth and Radon measures were defined. We continue with the same numbering of chapters and propositions as in [1]. In this part, for spaces of Radon probability measures, the barycenter map is studied, this map will be used to show that the functor Pˆ is monadic in the category of metrizable spaces.
    [Show full text]
  • AN INTRODUCTION to GEOMETRIC MEASURE THEORY and an APPLICATION to MINIMAL SURFACES ( DRAFT DOCUMENT) Academic Year 2018/19 Francesco Serra Cassano
    AN INTRODUCTION TO GEOMETRIC MEASURE THEORY AND AN APPLICATION TO MINIMAL SURFACES ( DRAFT DOCUMENT) Academic Year 2018/19 Francesco Serra Cassano Contents I. Recalls and complements of measure theory. I.1 Measures and outer measures, approximation of measures I.2 Convergence and approximation of measurable functions: Severini- Egoroff's theorem and Lusin's theorem. I.3 Absolutely continuous and singular measures. Radon-Nikodym and Lebesgue decomposition theorems. I.4 Signed vector measures: Lebesgue decomposition theorem and polar decompo- sition for vector measures. I.5 Spaces Lp(X; µ) and their main properties. Riesz representation theorem. I.6 Operations on measures. I.7 Weak*-convergence of measures. Regularization of Radon measures on Rn. II. Differentiation of Radon measures. II.1 Covering theorems and Vitali-type covering property for measures on Rn. II.2 Derivatives of Radon measures on Rn. Lebesgue-Besicovitch differentiation theorem for Radon measures on Rn. II.3 Extensions to metric spaces. III. An introduction to Hausdorff measures, area and coarea formulas. III.1 Carath´eodory's construction and definition of Hausdorff measures on a metric space and their elementary properties; Hausdorff dimension. III.2 Recalls of some fundamental results on Lipschitz functions between Euclidean spaces and relationships with Hausdorff measures. III.3 Hausdorff measures in the Euclidean spaces; H1 and the classical notion of length in Rn; isodiametric inequality and identity Hn = Ln on Rn; k-dimensional densities. III.4 Area and coarea formulas in Rn and some applications. III.5 Extensions to metric spaces. IV. Rectifiable sets and blow-ups of Radon measures. IV.1 Rectifiable sets of Rn and their decomposition in Lipschitz images.
    [Show full text]
  • LIMITATIONS on the EXTENDIBILITY of the RADON-NIKODYM THEOREM 0. Notation and Basic Definitions Throughout the Paper X and Y
    PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 131, Number 8, Pages 2491{2500 S 0002-9939(03)07046-1 Article electronically published on March 11, 2003 LIMITATIONS ON THE EXTENDIBILITY OF THE RADON-NIKODYM THEOREM GERD ZEIBIG (Communicated by N. Tomczak-Jaegermann) Abstract. Given two locally compact spaces X; Y and a continuous map r : Y X the Banach lattice 0(Y ) is naturally a 0(X)-module. Following ! the Bourbaki approach to integrationC we define generalizedC measures as 0(X)- 1 linear functionals µ : 0(Y ) 0(X). The construction of an L (µ)-spaceC and ! the concepts of absoluteC continuityC and density still make sense. However we exhibit a counter-example to the natural generalization of the Radon-Nikodym Theorem in this context. 0. Notation and basic definitions Throughout the paper X and Y will denote locally compact spaces and r : Y X will be a fixed continuous function. ! We use standard notation as in [3, 5]. In particular (X) stands for the space of C0 all complex-valued continuous functions on X which vanish at infinity and b(X) is the space of all complex-valued bounded continuous functions on X. The injectiveC and the projective tensor products are respectively denoted ˇ and ^ .Themost relevant feature of the injective tensor product for the present⊗ work is⊗ that we can identify (X Y )with (X) ˇ (Y )[2]. C0 × C0 ⊗ C0 Recall that a Banach module M over the Banach algebra 0(X) (under the pointwise operations) is a Banach space together with a contractiveC bilinear action- : map 0(X) M M.IfX is compact this action is subject to the usual axioms: α.(β.mC)=(×αβ):m−! and 1:m = m for all `scalars' α, β in (X)andallelements C0 m of M.IfX is not compact, in which case the algebra 0(X)doesnothavea unit element, the second axiom is replaced by the non-degeneracyC requirement that ('j:m)j converges to m,where('j)j is any contractive approximate identity for 0(X).
    [Show full text]
  • Limiting Problems in Integration and an Extension of the Real Numbers System Tue Ngoc Ly
    Marshall University Marshall Digital Scholar Theses, Dissertations and Capstones 1-1-2008 Limiting Problems in integration and An Extension of The Real Numbers System Tue Ngoc Ly Follow this and additional works at: http://mds.marshall.edu/etd Recommended Citation Ly, Tue Ngoc, "Limiting Problems in integration and An Extension of The Real Numbers System" (2008). Theses, Dissertations and Capstones. Paper 714. This Thesis is brought to you for free and open access by Marshall Digital Scholar. It has been accepted for inclusion in Theses, Dissertations and Capstones by an authorized administrator of Marshall Digital Scholar. For more information, please contact [email protected]. LIMITING PROBLEMS IN INTEGRATION AND AN EXTENSION OF THE REAL NUMBERS SYSTEM Thesis submitted to the Graduate College of Marshall University In partial fulfillment of the requirements for the degree of Master of Arts in Mathematics by Tue Ngoc Ly Dr Ariyadasa Aluthge, Ph.D., Committee Chairperson Dr. Ralph Oberste-Vorth, Ph.D., Committee Member Dr. Bonita Lawrence, Ph.D., Committee Member Marshall University May 2008 Abstract When considering the limit of a sequence of functions, some properties still hold under the limit, but some do not. Unfortunately, the integration is among those not holding. There are only certain classes of functions that still hold the integrability, and the values of the integrals under the limiting process. Starting with Riemann integrals, the limiting integrations are restricted not only on the class of functions, but also on the set on which the integral is taken. By redefining the integration process, Lebesgue integrals successfully and significantly extend both the class of the functions integrated and the sets on which the integral is taken.
    [Show full text]
  • REAL ANALYSIS Rudi Weikard
    REAL ANALYSIS Lecture notes for MA 645/646 2018/2019 Rudi Weikard 1.0 0.8 0.6 0.4 0.2 0.0 0.0 0.2 0.4 0.6 0.8 1.0 Version of July 26, 2018 Contents Preface iii Chapter 1. Abstract Integration1 1.1. Integration of non-negative functions1 1.2. Integration of complex functions4 1.3. Convex functions and Jensen's inequality5 1.4. Lp-spaces6 1.5. Exercises8 Chapter 2. Measures9 2.1. Types of measures9 2.2. Construction of measures 10 2.3. Lebesgue measure on Rn 11 2.4. Comparison of the Riemann and the Lebesgue integral 13 2.5. Complex measures and their total variation 14 2.6. Absolute continuity and mutually singular measures 15 2.7. Exercises 16 Chapter 3. Integration on Product Spaces 19 3.1. Product measure spaces 19 3.2. Fubini's theorem 20 3.3. Exercises 21 Chapter 4. The Lebesgue-Radon-Nikodym theorem 23 4.1. The Lebesgue-Radon-Nikodym theorem 23 4.2. Integration with respect to a complex measure 25 Chapter 5. Radon Functionals on Locally Compact Hausdorff Spaces 27 5.1. Preliminaries 27 5.2. Approximation by continuous functions 27 5.3. Riesz's representation theorem 28 5.4. Exercises 31 Chapter 6. Differentiation 33 6.1. Derivatives of measures 33 6.2. Exercises 34 Chapter 7. Functions of Bounded Variation and Lebesgue-Stieltjes Measures 35 7.1. Functions of bounded variation 35 7.2. Lebesgue-Stieltjes measures 36 7.3. Absolutely continuous functions 39 i ii CONTENTS 7.4.
    [Show full text]