Primbs, MS&E345 1 Measure Theory in a Lecture. Primbs, MS&E345 2 Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem.

Slides:



Advertisements
Similar presentations
Completeness and Expressiveness
Advertisements

Approximating the area under a curve using Riemann Sums
Lecture 7 Surreal Numbers. Lecture 7 Surreal Numbers.
Gibbs sampler - simple properties It’s not hard to show that this MC chain is aperiodic. Often is reversible distribution. If in addition the chain is.
1 Theory of Differentiation in Statistics Mohammed Nasser Department of Statistics.
INTEGRALS 5. INTEGRALS We saw in Section 5.1 that a limit of the form arises when we compute an area.  We also saw that it arises when we try to find.
Theory of Integration in Statistics
T. Mhamdi, O. Hasan and S. Tahar, HVG, Concordia University Montreal, Canada July 2010 On the Formalization of the Lebesgue Integration Theory in HOL On.
Chapter 5 Integral. Estimating with Finite Sums Approach.
The importance of sequences and infinite series in calculus stems from Newton’s idea of representing functions as sums of infinite series.  For instance,
Lecture 2: Measures and Data Collection/Cleaning CS 6071 Big Data Engineering, Architecture, and Security Fall 2015, Dr. Rozier.
استاد : دکتر گلبابایی In detail this means three conditions:  1. f has to be defined at c.  2. the limit on the left hand side of that equation has.
Chapter 3 – Set Theory  .
Pareto Linear Programming The Problem: P-opt Cx s.t Ax ≤ b x ≥ 0 where C is a kxn matrix so that Cx = (c (1) x, c (2) x,..., c (k) x) where c.
Chapter 3 L p -space. Preliminaries on measure and integration.
Integrals  In Chapter 2, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.  In much the.
Statistical Decision Theory Bayes’ theorem: For discrete events For probability density functions.
Chapter 4 Hilbert Space. 4.1 Inner product space.
1 3. Random Variables Let ( , F, P) be a probability model for an experiment, and X a function that maps every to a unique point the set of real numbers.
AGC DSP AGC DSP Professor A G Constantinides©1 Signal Spaces The purpose of this part of the course is to introduce the basic concepts behind generalised.
12 INFINITE SEQUENCES AND SERIES. In general, it is difficult to find the exact sum of a series.  We were able to accomplish this for geometric series.
CS 103 Discrete Structures Lecture 13 Induction and Recursion (1)
1.6 Change of Measure 1. Introduction We used a positive random variable Z to change probability measures on a space Ω. is risk-neutral probability measure.
Random Variables. Numerical Outcomes Consider associating a numerical value with each sample point in a sample space. (1,1) (1,2) (1,3) (1,4) (1,5) (1,6)
Lecture 4 Infinite Cardinals. Some Philosophy: What is “2”? Definition 1: 2 = 1+1. This actually needs the definition of “1” and the definition of the.
In Chapters 6 and 8, we will see how to use the integral to solve problems concerning:  Volumes  Lengths of curves  Population predictions  Cardiac.
INTEGRALS We saw in Section 5.1 that a limit of the form arises when we compute an area. We also saw that it arises when we try to find the distance traveled.
5 INTEGRALS.
Summary of the Last Lecture This is our second lecture. In our first lecture, we discussed The vector spaces briefly and proved some basic inequalities.
Basic Probability. Introduction Our formal study of probability will base on Set theory Axiomatic approach (base for all our further studies of probability)
Sequences Lecture 11. L62 Sequences Sequences are a way of ordering lists of objects. Java arrays are a type of sequence of finite size. Usually, mathematical.
INTEGRALS 5. INTEGRALS In Chapter 3, we used the tangent and velocity problems to introduce the derivative—the central idea in differential calculus.
Math 3121 Abstract Algebra I Lecture 6 Midterm back over+Section 7.
MA4229 Lectures 13, 14 Week 12 Nov 1, Chapter 13 Approximation to periodic functions.
INFINITE SEQUENCES AND SERIES In general, it is difficult to find the exact sum of a series.  We were able to accomplish this for geometric series and.
1-1 Copyright © 2013, 2005, 2001 Pearson Education, Inc. Section 2.4, Slide 1 Chapter 2 Sets and Functions.
7.3 Linear Systems of Equations. Gauss Elimination
Trigonometric Identities
Ch 11.6: Series of Orthogonal Functions: Mean Convergence
Mathematical Formulation of the Superposition Principle
Chapter 2 Sets and Functions.
CHAPTER 3 SETS, BOOLEAN ALGEBRA & LOGIC CIRCUITS
Chapter 3 The Real Numbers.
The Language of Sets If S is a set, then
Functions of Complex Variable and Integral Transforms
Lecture 3 B Maysaa ELmahi.
Copyright © Cengage Learning. All rights reserved.
Set, Combinatorics, Probability & Number Theory
represents the Empty set, or the set that contains nothing
CONTINUOUS RANDOM VARIABLES
AP Physics C.
Lebesgue measure: Lebesgue measure m0 is a measure on i.e., 1. 2.
Definite Integrals Finney Chapter 6.2.
Trigonometric Identities
Quantum One.
Chapter 1 Section 1.
Precalculus Mathematics for Calculus Fifth Edition
Copyright © Cengage Learning. All rights reserved.
The aim of education is to teach students how to think rather than what to think. Sets The set is the fundamental discrete structure on which all other.
What LIMIT Means Given a function: f(x) = 3x – 5 Describe its parts.
Copyright © Cengage Learning. All rights reserved.
The Fundamental Theorem of Calculus
Maths for Signals and Systems Linear Algebra in Engineering Lecture 6, Friday 21st October 2016 DR TANIA STATHAKI READER (ASSOCIATE PROFFESOR) IN SIGNAL.
3. Random Variables Let (, F, P) be a probability model for an experiment, and X a function that maps every to a unique point.
8. One Function of Two Random Variables
Inequalities Some problems in algebra lead to inequalities instead of equations. An inequality looks just like an equation, except that in the place of.
Experiments, Outcomes, Events and Random Variables: A Revisit
Linear Vector Space and Matrix Mechanics
8. One Function of Two Random Variables
Presentation transcript:

Primbs, MS&E345 1 Measure Theory in a Lecture

Primbs, MS&E345 2 Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E345 3 A little perspective: Riemann did this......

Primbs, MS&E345 4 A little perspective: Lebesgue did this...

Primbs, MS&E345 5 A little perspective: Lebesgue did this... Why is this better????

Primbs, MS&E345 6 A little perspective: Lebesgue did this... Why is this better???? Consider the function: If we follow Lebesgue’s reasoning, then the integral of this function over the set [0,1] should be: (Height) x (width of irrationals) = 1 x (measure of irrationals) Height Width of Irrationals If we can “measure” the size of sublevel sets, we can integrate a lot of function!

Primbs, MS&E345 7 Measure Theory begins from this simple motivation. If you remember a couple of simple principles, measure and integration theory becomes quite intuitive. The first principle is this... Integration is about functions. Measure theory is about sets. The connection between functions and sets is sub-level sets.

Primbs, MS&E345 8 Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E345 9 Measure theory is about measuring the size of things. In math we measure the size of sets. Set A How big is the set A?

Primbs, MS&E “Size” should have the following property: The size of the union of disjoint sets should equal the sum of the sizes of the individual sets. Makes sense.... but there is a problem with this... Consider the interval [0,1]. It is the disjoint union of all real numbers between 0 and 1. Therefore, according to above, the size of [0,1] should be the sum of the sizes of a single real number. If the size of a singleton is 0 then the size of [0,1] is 0. If the size of a singleton is non-zero, then the size of [0,1] is infinity! This shows we have to be a bit more careful.

Primbs, MS&E Sigma Algebras (  -algebra) Consider a set  Let F be a collection of subsets of  F is a  -algebra if: An algebra of sets is closed under finite set operations. A  -algebra is closed under countable set operations. In mathematics,  often refers to “countable”. 1) 2) 3) 4)

Primbs, MS&E Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E Algebras are what we need for sublevel sets of a vector space of indicator functions. Sublevel Sets

Primbs, MS&E Sublevel Sets  algebras let us take limits of these. That is more interesting!! Simple Functions Simple functions are finite linear combinations of of indicator functions.

Primbs, MS&E Measurable Functions Given a Measurable Space ( ,F) We say that a function: is measurable with respect to F if: This simply says that a function is measurable with respect to the  -algebra if all its sublevel sets are in the  -algebra. Hence, a measurable function is one that when we slice it like Lebesgue, we can measure the “width” of the part of the function above the slice. Simple...right?

Primbs, MS&E Another equivalent way to think of measurable functions is as the pointwise limit of simple functions. In fact, if a measurable function is non-negative, we can say it is the increasing pointwise limit of simple functions. This is simply going back to Lebesgue’s picture...

Primbs, MS&E Intuition behind measurable functions. They are “constant on the sets in the sigma algebra.” What do measurable functions look like? Yes No Intuitively speaking, Measurable functions are constant on the sets in the  -alg. More accurately, they are limits of functions are constant on the sets in the  - algebra. The  in  -algebra gives us this.

Primbs, MS&E “Information” and  -Algebras. Since measurable functions are “constant” on the  -algebra, if I am trying to determine information from a measurable function, the  -algebra determines the information that I can obtain. I measure What is the most information that I determine about  ?  -algebras determine the amount of information possible in a function. The best possible I can do is to say that with

Primbs, MS&E Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E Measures and Integration A measurable space (  F) defines the sets can be measured. Now we actually have to measure them... What are the properties that “size” should satisfy. If you think about it long enough, there are really only two...

Primbs, MS&E Definition of a measure: Given a Measurable Space ( ,F), A measure is a function satisfying two properties: 1) 2) (2) is known as “countable additivity”. However, I think of it as “linearity and left continuity for sets”.

Primbs, MS&E Fundamental properties of measures (or “size”): Left Continuity: This is a trivial consequence of the definition! Right Continuity: Depends on boundedness! (Here is why we need boundedness. Consider then ) Let then Let and for some i then

Primbs, MS&E Now we can define the integral. Since positive measurable functions can be written as the increasing pointwise limit of simple functions, we define the integral as Simple Functions: Positive Functions: For a general measurable function write

Primbs, MS&E This picture says everything!!!! A f This is a set! and the integral is measuring the “size” of this set! Integrals are like measures! They measure the size of a set. We just describe that set by a function. Therefore, integrals must satisfy the properties of measures. How should I think about

Primbs, MS&E Measures and integrals are different descriptions of of the same concept. Namely, “size”. Therefore, they must satisfy exactly the same properties!! This leads us to another important principle... Lebesgue defined the integral so that this would be true!

Primbs, MS&E Left Continuous Bdd Right Cont. etc... Measures are: Integrals are: and (Monotone Convergence Thm.) (Bounded Convergence Thm.) etc... (Fatou’s Lemma, etc...)

Primbs, MS&E The L p Spaces A function is in L p ( ,F,  ) if The L p spaces are Banach Spaces with norm: L 2 is a Hilbert Space with inner product:

Primbs, MS&E Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E Given a Measurable Space ( ,F), There exist many measures on F. If  is the real line, the standard measure is “length”. That is, the measure of each interval is its length. This is known as “Lebesgue measure”. The  -algebra must contain intervals. The smallest  - algebra that contains all open sets (and hence intervals) is call the “Borel”  -algebra and is denoted B. A course in real analysis will deal a lot with the measurable space.

Primbs, MS&E Given a Measurable Space ( ,F), A measurable space combined with a measure is called a measure space. If we denote the measure by , we would write the triple: ( ,F  Given a measure space ( ,F  if we decide instead to use a different measure, say  then we call this a “change of measure”. (We should just call this using another measure!) Let  and  be two measures on ( ,F), then (Notation )  is “absolutely continuous” with respect to  if  and  are “equivalent” if

Primbs, MS&E The Radon-Nikodym Theorem If  <<  then  is actually the integral of a function wrt . g is known as the Radon- Nikodym derivative and denoted:

Primbs, MS&E The Radon-Nikodym Theorem If  <<  then  is actually the integral of a function wrt . Consider the set function (this is actually a signed measure) Then is the  -sublevel set of g. Idea of proof: Create the function through its sublevel sets Chooseand letbe the largest set such that for all (You must prove such an A  exists.) Now, given sublevel sets, we can construct a function by:

Primbs, MS&E Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E The Riesz Representation Theorem: All continuous linear functionals on L p are given by integration against a function with That is, letbe a cts. linear functional. Then: Note, in L 2 this becomes:

Primbs, MS&E The Riesz Representation Theorem: All continuous linear functionals on L p are given by integration against a function with What is the idea behind the proof: Linearity allows you to break things into building blocks, operate on them, then add them all together. What are the building blocks of measurable functions. Indicator functions! Of course! Let’s define a set valued function from indicator functions:

Primbs, MS&E The Riesz Representation Theorem: All continuous linear functionals on L p are given by integration against a function with A set valued function How does L operate on simple functions This looks like an integral with  the measure! But, it is not too hard to show that  is a (signed) measure. (countable additivity follows from continuity). Furthermore,  <<  Radon-Nikodym then says d  =gd 

Primbs, MS&E The Riesz Representation Theorem: All continuous linear functionals on L p are given by integration against a function with A set valued function How does L operate on simple functions This looks like an integral with  the measure! For measurable functions it follows from limits and continuity. The details are left as an “easy” exercise for the reader...

Primbs, MS&E The Riesz Representation Theorem and the Radon- Nikodym Theorem are basically equivalent. You can prove one from the other and vice-versa. We will see the interplay between them in finance... How does any of this relate to probability theory...

Primbs, MS&E Perspective  -Algebras Measurable Functions Measure and Integration Radon-Nikodym Theorem Riesz Representation Theorem Measure Theory Probability Theory

Primbs, MS&E A random variable is a measurable function. The expectation of a random variable is its integral: A density function is the Radon-Nikodym derivative wrt Lebesgue measure: A probability measure P is a measure that satisfies That is, the measure of the whole space is 1.

Primbs, MS&E In finance we will talk about expectations with respect to different measures. A probability measure P is a measure that satisfies That is, the measure of the whole space is 1. whereor And write expectations in terms of the different measures: