The Fundamental Theorem of Calculus for Lebesgue Integral
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[Math.FA] 3 Dec 1999 Rnfrneter for Theory Transference Introduction 1 Sas Ihnrah U Twl Etetdi Eaaepaper
Transference in Spaces of Measures Nakhl´eH. Asmar,∗ Stephen J. Montgomery–Smith,† and Sadahiro Saeki‡ 1 Introduction Transference theory for Lp spaces is a powerful tool with many fruitful applications to sin- gular integrals, ergodic theory, and spectral theory of operators [4, 5]. These methods afford a unified approach to many problems in diverse areas, which before were proved by a variety of methods. The purpose of this paper is to bring about a similar approach to spaces of measures. Our main transference result is motivated by the extensions of the classical F.&M. Riesz Theorem due to Bochner [3], Helson-Lowdenslager [10, 11], de Leeuw-Glicksberg [6], Forelli [9], and others. It might seem that these extensions should all be obtainable via transference methods, and indeed, as we will show, these are exemplary illustrations of the scope of our main result. It is not straightforward to extend the classical transference methods of Calder´on, Coif- man and Weiss to spaces of measures. First, their methods make use of averaging techniques and the amenability of the group of representations. The averaging techniques simply do not work with measures, and do not preserve analyticity. Secondly, and most importantly, their techniques require that the representation is strongly continuous. For spaces of mea- sures, this last requirement would be prohibitive, even for the simplest representations such as translations. Instead, we will introduce a much weaker requirement, which we will call ‘sup path attaining’. By working with sup path attaining representations, we are able to prove a new transference principle with interesting applications. For example, we will show how to derive with ease generalizations of Bochner’s theorem and Forelli’s main result. -
Shape Analysis, Lebesgue Integration and Absolute Continuity Connections
NISTIR 8217 Shape Analysis, Lebesgue Integration and Absolute Continuity Connections Javier Bernal This publication is available free of charge from: https://doi.org/10.6028/NIST.IR.8217 NISTIR 8217 Shape Analysis, Lebesgue Integration and Absolute Continuity Connections Javier Bernal Applied and Computational Mathematics Division Information Technology Laboratory This publication is available free of charge from: https://doi.org/10.6028/NIST.IR.8217 July 2018 INCLUDES UPDATES AS OF 07-18-2018; SEE APPENDIX U.S. Department of Commerce Wilbur L. Ross, Jr., Secretary National Institute of Standards and Technology Walter Copan, NIST Director and Undersecretary of Commerce for Standards and Technology ______________________________________________________________________________________________________ This Shape Analysis, Lebesgue Integration and publication Absolute Continuity Connections Javier Bernal is National Institute of Standards and Technology, available Gaithersburg, MD 20899, USA free of Abstract charge As shape analysis of the form presented in Srivastava and Klassen’s textbook “Functional and Shape Data Analysis” is intricately related to Lebesgue integration and absolute continuity, it is advantageous from: to have a good grasp of the latter two notions. Accordingly, in these notes we review basic concepts and results about Lebesgue integration https://doi.org/10.6028/NIST.IR.8217 and absolute continuity. In particular, we review fundamental results connecting them to each other and to the kind of shape analysis, or more generally, functional data analysis presented in the aforeme- tioned textbook, in the process shedding light on important aspects of all three notions. Many well-known results, especially most results about Lebesgue integration and some results about absolute conti- nuity, are presented without proofs. -
An Introduction to Measure Theory Terence
An introduction to measure theory Terence Tao Department of Mathematics, UCLA, Los Angeles, CA 90095 E-mail address: [email protected] To Garth Gaudry, who set me on the road; To my family, for their constant support; And to the readers of my blog, for their feedback and contributions. Contents Preface ix Notation x Acknowledgments xvi Chapter 1. Measure theory 1 x1.1. Prologue: The problem of measure 2 x1.2. Lebesgue measure 17 x1.3. The Lebesgue integral 46 x1.4. Abstract measure spaces 79 x1.5. Modes of convergence 114 x1.6. Differentiation theorems 131 x1.7. Outer measures, pre-measures, and product measures 179 Chapter 2. Related articles 209 x2.1. Problem solving strategies 210 x2.2. The Radamacher differentiation theorem 226 x2.3. Probability spaces 232 x2.4. Infinite product spaces and the Kolmogorov extension theorem 235 Bibliography 243 vii viii Contents Index 245 Preface In the fall of 2010, I taught an introductory one-quarter course on graduate real analysis, focusing in particular on the basics of mea- sure and integration theory, both in Euclidean spaces and in abstract measure spaces. This text is based on my lecture notes of that course, which are also available online on my blog terrytao.wordpress.com, together with some supplementary material, such as a section on prob- lem solving strategies in real analysis (Section 2.1) which evolved from discussions with my students. This text is intended to form a prequel to my graduate text [Ta2010] (henceforth referred to as An epsilon of room, Vol. I ), which is an introduction to the analysis of Hilbert and Banach spaces (such as Lp and Sobolev spaces), point-set topology, and related top- ics such as Fourier analysis and the theory of distributions; together, they serve as a text for a complete first-year graduate course in real analysis. -
Generalizations of the Riemann Integral: an Investigation of the Henstock Integral
Generalizations of the Riemann Integral: An Investigation of the Henstock Integral Jonathan Wells May 15, 2011 Abstract The Henstock integral, a generalization of the Riemann integral that makes use of the δ-fine tagged partition, is studied. We first consider Lebesgue’s Criterion for Riemann Integrability, which states that a func- tion is Riemann integrable if and only if it is bounded and continuous almost everywhere, before investigating several theoretical shortcomings of the Riemann integral. Despite the inverse relationship between integra- tion and differentiation given by the Fundamental Theorem of Calculus, we find that not every derivative is Riemann integrable. We also find that the strong condition of uniform convergence must be applied to guarantee that the limit of a sequence of Riemann integrable functions remains in- tegrable. However, by slightly altering the way that tagged partitions are formed, we are able to construct a definition for the integral that allows for the integration of a much wider class of functions. We investigate sev- eral properties of this generalized Riemann integral. We also demonstrate that every derivative is Henstock integrable, and that the much looser requirements of the Monotone Convergence Theorem guarantee that the limit of a sequence of Henstock integrable functions is integrable. This paper is written without the use of Lebesgue measure theory. Acknowledgements I would like to thank Professor Patrick Keef and Professor Russell Gordon for their advice and guidance through this project. I would also like to acknowledge Kathryn Barich and Kailey Bolles for their assistance in the editing process. Introduction As the workhorse of modern analysis, the integral is without question one of the most familiar pieces of the calculus sequence. -
Stability in the Almost Everywhere Sense: a Linear Transfer Operator Approach ∗ R
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector J. Math. Anal. Appl. 368 (2010) 144–156 Contents lists available at ScienceDirect Journal of Mathematical Analysis and Applications www.elsevier.com/locate/jmaa Stability in the almost everywhere sense: A linear transfer operator approach ∗ R. Rajaram a, ,U.Vaidyab,M.Fardadc, B. Ganapathysubramanian d a Dept. of Math. Sci., 3300, Lake Rd West, Kent State University, Ashtabula, OH 44004, United States b Dept. of Elec. and Comp. Engineering, Iowa State University, Ames, IA 50011, United States c Dept. of Elec. Engineering and Comp. Sci., Syracuse University, Syracuse, NY 13244, United States d Dept. of Mechanical Engineering, Iowa State University, Ames, IA 50011, United States article info abstract Article history: The problem of almost everywhere stability of a nonlinear autonomous ordinary differential Received 20 April 2009 equation is studied using a linear transfer operator framework. The infinitesimal generator Available online 20 February 2010 of a linear transfer operator (Perron–Frobenius) is used to provide stability conditions of Submitted by H. Zwart an autonomous ordinary differential equation. It is shown that almost everywhere uniform stability of a nonlinear differential equation, is equivalent to the existence of a non-negative Keywords: Almost everywhere stability solution for a steady state advection type linear partial differential equation. We refer Advection equation to this non-negative solution, verifying almost everywhere global stability, as Lyapunov Density function density. A numerical method using finite element techniques is used for the computation of Lyapunov density. © 2010 Elsevier Inc. All rights reserved. 1. Introduction Stability analysis of an ordinary differential equation is one of the most fundamental problems in the theory of dynami- cal systems. -
Computing the Bayes Factor from a Markov Chain Monte Carlo
Computing the Bayes Factor from a Markov chain Monte Carlo Simulation of the Posterior Distribution Martin D. Weinberg∗ Department of Astronomy University of Massachusetts, Amherst, USA Abstract Computation of the marginal likelihood from a simulated posterior distribution is central to Bayesian model selection but is computationally difficult. The often-used harmonic mean approximation uses the posterior directly but is unstably sensitive to samples with anomalously small values of the likelihood. The Laplace approximation is stable but makes strong, and of- ten inappropriate, assumptions about the shape of the posterior distribution. It is useful, but not general. We need algorithms that apply to general distributions, like the harmonic mean approximation, but do not suffer from convergence and instability issues. Here, I argue that the marginal likelihood can be reliably computed from a posterior sample by careful attention to the numerics of the probability integral. Posing the expression for the marginal likelihood as a Lebesgue integral, we may convert the harmonic mean approximation from a sample statistic to a quadrature rule. As a quadrature, the harmonic mean approximation suffers from enor- mous truncation error as consequence . This error is a direct consequence of poor coverage of the sample space; the posterior sample required for accurate computation of the marginal likelihood is much larger than that required to characterize the posterior distribution when us- ing the harmonic mean approximation. In addition, I demonstrate that the integral expression for the harmonic-mean approximation converges slowly at best for high-dimensional problems with uninformative prior distributions. These observations lead to two computationally-modest families of quadrature algorithms that use the full generality sample posterior but without the instability. -
Chapter 6. Integration §1. Integrals of Nonnegative Functions Let (X, S, Μ
Chapter 6. Integration §1. Integrals of Nonnegative Functions Let (X, S, µ) be a measure space. We denote by L+ the set of all measurable functions from X to [0, ∞]. + Let φ be a simple function in L . Suppose f(X) = {a1, . , am}. Then φ has the Pm −1 standard representation φ = j=1 ajχEj , where Ej := f ({aj}), j = 1, . , m. We define the integral of φ with respect to µ to be m Z X φ dµ := ajµ(Ej). X j=1 Pm For c ≥ 0, we have cφ = j=1(caj)χEj . It follows that m Z X Z cφ dµ = (caj)µ(Ej) = c φ dµ. X j=1 X Pm Suppose that φ = j=1 ajχEj , where aj ≥ 0 for j = 1, . , m and E1,...,Em are m Pn mutually disjoint measurable sets such that ∪j=1Ej = X. Suppose that ψ = k=1 bkχFk , where bk ≥ 0 for k = 1, . , n and F1,...,Fn are mutually disjoint measurable sets such n that ∪k=1Fk = X. Then we have m n n m X X X X φ = ajχEj ∩Fk and ψ = bkχFk∩Ej . j=1 k=1 k=1 j=1 If φ ≤ ψ, then aj ≤ bk, provided Ej ∩ Fk 6= ∅. Consequently, m m n m n n X X X X X X ajµ(Ej) = ajµ(Ej ∩ Fk) ≤ bkµ(Ej ∩ Fk) = bkµ(Fk). j=1 j=1 k=1 j=1 k=1 k=1 In particular, if φ = ψ, then m n X X ajµ(Ej) = bkµ(Fk). j=1 k=1 In general, if φ ≤ ψ, then m n Z X X Z φ dµ = ajµ(Ej) ≤ bkµ(Fk) = ψ dµ. -
Problem Set 6
Richard Bamler Jeremy Leach office 382-N, phone: 650-723-2975 office 381-J [email protected] [email protected] office hours: office hours: Mon 1:00pm-3pm, Thu 1:00pm-2:00pm Thu 3:45pm-6:45pm MATH 172: Lebesgue Integration and Fourier Analysis (winter 2012) Problem set 6 due Wed, 2/22 in class (1) (20 points) Let X be an arbitrary space, M a σ-algebra on X and λ a measure on M. Consider an M-measurable function ρ : X ! [0; 1] which only takes non-negative values. (a) Show that the function, Z µ : M! [0; 1];A 7! (ρχA)dλ is a measure on M. We will also denote this measure by µ = (ρλ). (b) Show that any M-measurable function f : X ! R is integrable with respect to µ if and only if fρ is integrable with respect to λ. In this case we have Z Z Z fdµ = fd(ρλ) = fρdλ. (Hint: Show first that this is true for simple functions, then for non-negative functions, then for general functions). (c) Show that if A 2 M is a nullset with respect to λ, then it is also a nullset with respect to µ = ρλ. (Remark: A measure µ with this property is called absolutely continuous with respect to λ in symbols µ λ.) (d) Assume that X = Rn, M = L and λ is the Lebesgue measure. Give an example for a measure µ0 on M such that there is no non-negative, M- measurable function ρ : X ! [0; 1] with µ0 = ρλ. -
2. Convergence Theorems
2. Convergence theorems In this section we analyze the dynamics of integrabilty in the case when se- quences of measurable functions are considered. Roughly speaking, a “convergence theorem” states that integrability is preserved under taking limits. In other words, ∞ if one has a sequence (fn)n=1 of integrable functions, and if f is some kind of a limit of the fn’s, then we would like to conclude that f itself is integrable, as well R R as the equality f = limn→∞ fn. Such results are often employed in two instances: A. When we want to prove that some function f is integrable. In this case ∞ we would look for a sequence (fn)n=1 of integrable approximants for f. B. When we want to construct and integrable function. In this case, we will produce first the approximants, and then we will examine the existence of the limit. The first convergence result, which is somehow primite, but very useful, is the following. Lemma 2.1. Let (X, A, µ) be a finite measure space, let a ∈ (0, ∞) and let fn : X → [0, a], n ≥ 1, be a sequence of measurable functions satisfying (a) f1 ≥ f2 ≥ · · · ≥ 0; (b) limn→∞ fn(x) = 0, ∀ x ∈ X. Then one has the equality Z (1) lim fn dµ = 0. n→∞ X Proof. Let us define, for each ε > 0, and each integer n ≥ 1, the set ε An = {x ∈ X : fn(x) ≥ ε}. ε Obviously, we have An ∈ A, ∀ ε > 0, n ≥ 1. One key fact we are going to use is the following. -
Lecture 26: Dominated Convergence Theorem
Lecture 26: Dominated Convergence Theorem Continuation of Fatou's Lemma. + + Corollary 0.1. If f 2 L and ffn 2 L : n 2 Ng is any sequence of functions such that fn ! f almost everywhere, then Z Z f 6 lim inf fn: X X Proof. Let fn ! f everywhere in X. That is, lim inf fn(x) = f(x) (= lim sup fn also) for all x 2 X. Then, by Fatou's lemma, Z Z Z f = lim inf fn 6 lim inf fn: X X X If fn 9 f everywhere in X, then let E = fx 2 X : lim inf fn(x) 6= f(x)g. Since fn ! f almost everywhere in X, µ(E) = 0 and Z Z Z Z f = f and fn = fn 8n X X−E X X−E thus making fn 9 f everywhere in X − E. Hence, Z Z Z Z f = f 6 lim inf fn = lim inf fn: X X−E X−E X χ Example 0.2 (Strict inequality). Let Sn = [n; n + 1] ⊂ R and fn = Sn . Then, f = lim inf fn = 0 and Z Z 0 = f dµ < lim inf fn dµ = 1: R R Example 0.3 (Importance of non-negativity). Let Sn = [n; n + 1] ⊂ R and χ fn = − Sn . Then, f = lim inf fn = 0 but Z Z 0 = f dµ > lim inf fn dµ = −1: R R 1 + R Proposition 0.4. If f 2 L and X f dµ < 1, then (a) the set A = fx 2 X : f(x) = 1g is a null set and (b) the set B = fx 2 X : f(x) > 0g is σ-finite. -
MEASURE and INTEGRATION: LECTURE 3 Riemann Integral. If S Is Simple and Measurable Then Sdµ = Αiµ(
MEASURE AND INTEGRATION: LECTURE 3 Riemann integral. If s is simple and measurable then N � � sdµ = αiµ(Ei), X i=1 �N where s = i=1 αiχEi . If f ≥ 0, then � �� � fdµ = sup sdµ | 0 ≤ s ≤ f, s simple & measurable . X X Recall the Riemann integral of function f on interval [a, b]. Define lower and upper integrals L(f, P ) and U(f, P ), where P is a partition of [a, b]. Set − � � f = sup L(f, P ) and f = inf U(f, P ). P P − A function f is Riemann integrable ⇐⇒ − � � f = f, − in which case this common value is � f. A set B ⊂ R has measure zero if, for any � > 0, there exists a ∞ ∞ countable collection of intervals { Ii}i =1 such that B ⊂ ∪i =1Ii and �∞ i=1 λ(Ii) < �. Examples: finite sets, countable sets. There are also uncountable sets with measure zero. However, any interval does not have measure zero. Theorem 0.1. A function f is Riemann integrable if and only if f is discontinuous on a set of measure zero. A function is said to have a property (e.g., continuous) almost ev erywhere (abbreviated a.e.) if the set on which the property does not hold has measure zero. Thus, the statement of the theorem is that f is Riemann integrable if and only if it is continuous almost everywhere. Date: September 11, 2003. 1 2 MEASURE AND INTEGRATION: LECTURE 3 Recall positive measure: a measure function µ: M → [0, ∞] such ∞ �∞ that µ (∪i=1Ei) = i=1 µ(Ei) for Ei ∈ M disjoint. -
Lecture Notes for Math 522 Spring 2012 (Rudin Chapter
Lebesgue integral We will define a very powerful integral, far better than Riemann in the sense that it will allow us to integrate pretty much every reasonable function and we will also obtain strong convergence results. That is if we take a limit of integrable functions we will get an integrable function and the limit of the integrals will be the integral of the limit under very mild conditions. We will focus only on the real line, although the theory easily extends to more abstract contexts. In Riemann integral the basic block was a rectangle. If we wanted to integrate a function that was identically 1 on an interval [a; b], then the integral was simply the area of that rectangle, so 1×(b−a) = b−a. For Lebesgue integral what we want to do is to replace the interval with a more general subset of the real line. That is, if we have a set S ⊂ R and we take the indicator function or characteristic function χS defined by ( 1 if x 2 S, χ (x) = S 0 else. Then the integral of χS should really be equal to the area under the graph, which should be equal to the \size" of S. Example: Suppose that S is the set of rational numbers between 0 and 1. Let us argue that its size is 0, and so the integral of χS should be 0. Let fx1; x2;:::g = S be an enumeration of the points of S. Now for any > 0 take the sets −j−1 −j−1 Ij = (xj − 2 ; xj + 2 ); then 1 [ S ⊂ Ij: j=1 −j The \size" of any Ij should be 2 , so it seems reasonable to say that the \size" of S is less than the sum of the sizes of the Ij's.