V. SUBSPACES AND ORTHOGONAL PROJECTION

Similar documents
I teach myself... Hilbert spaces

3 Orthogonality and Fourier series

Recall that any inner product space V has an associated norm defined by

4 Hilbert spaces. The proof of the Hilbert basis theorem is not mathematics, it is theology. Camille Jordan

A SYNOPSIS OF HILBERT SPACE THEORY

Finite-dimensional spaces. C n is the space of n-tuples x = (x 1,..., x n ) of complex numbers. It is a Hilbert space with the inner product

David Hilbert was old and partly deaf in the nineteen thirties. Yet being a diligent

Functional Analysis. Franck Sueur Metric spaces Definitions Completeness Compactness Separability...

CHAPTER II HILBERT SPACES

Projection Theorem 1

Analysis Preliminary Exam Workshop: Hilbert Spaces

Functional Analysis Review

Hilbert Spaces: Infinite-Dimensional Vector Spaces

1. Subspaces A subset M of Hilbert space H is a subspace of it is closed under the operation of forming linear combinations;i.e.,

Hilbert Spaces. Contents

MA677 Assignment #3 Morgan Schreffler Due 09/19/12 Exercise 1 Using Hölder s inequality, prove Minkowski s inequality for f, g L p (R d ), p 1:

Functional Analysis HW #5

Real Analysis Notes. Thomas Goller

MATH31011/MATH41011/MATH61011: FOURIER ANALYSIS AND LEBESGUE INTEGRATION. Chapter 2: Countability and Cantor Sets

Problem 1: Compactness (12 points, 2 points each)

THEOREMS, ETC., FOR MATH 515

NOTES ON FRAMES. Damir Bakić University of Zagreb. June 6, 2017

Vectors in Function Spaces

Notes on Integrable Functions and the Riesz Representation Theorem Math 8445, Winter 06, Professor J. Segert. f(x) = f + (x) + f (x).

HILBERT SPACES AND THE RADON-NIKODYM THEOREM. where the bar in the first equation denotes complex conjugation. In either case, for any x V define

Your first day at work MATH 806 (Fall 2015)

08a. Operators on Hilbert spaces. 1. Boundedness, continuity, operator norms

CHAPTER 3. Hilbert spaces

Math 5520 Homework 2 Solutions

Review and problem list for Applied Math I

ADJOINTS, ABSOLUTE VALUES AND POLAR DECOMPOSITIONS

Applied Analysis (APPM 5440): Final exam 1:30pm 4:00pm, Dec. 14, Closed books.

Orthonormal Bases Fall Consider an inner product space V with inner product f, g and norm

Inner Product Spaces An inner product on a complex linear space X is a function x y from X X C such that. (1) (2) (3) x x > 0 for x 0.

Math 350 Fall 2011 Notes about inner product spaces. In this notes we state and prove some important properties of inner product spaces.

Your first day at work MATH 806 (Fall 2015)

MATH 650. THE RADON-NIKODYM THEOREM

Kernel Method: Data Analysis with Positive Definite Kernels

RIESZ BASES AND UNCONDITIONAL BASES

Homework Assignment #5 Due Wednesday, March 3rd.

1 Compact and Precompact Subsets of H

Part V. 17 Introduction: What are measures and why measurable sets. Lebesgue Integration Theory

s P = f(ξ n )(x i x i 1 ). i=1

Theorem (4.11). Let M be a closed subspace of a Hilbert space H. For any x, y E, the parallelogram law applied to x/2 and y/2 gives.

Orthonormal Systems. Fourier Series

Fall TMA4145 Linear Methods. Exercise set 10

Math 61CM - Solutions to homework 6

THE PROBLEMS FOR THE SECOND TEST FOR BRIEF SOLUTIONS

ABSTRACT CONDITIONAL EXPECTATION IN L 2

Spectral Theory, with an Introduction to Operator Means. William L. Green

Functional Analysis (2006) Homework assignment 2

COMPLETION OF A METRIC SPACE

Tools from Lebesgue integration

1 Functional Analysis

The Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:

Operators with Closed Range, Pseudo-Inverses, and Perturbation of Frames for a Subspace

On Unitary Relations between Kre n Spaces

SPECTRAL THEOREM FOR COMPACT SELF-ADJOINT OPERATORS

Functional Analysis F3/F4/NVP (2005) Homework assignment 2

Linear Algebra. Paul Yiu. Department of Mathematics Florida Atlantic University. Fall A: Inner products

Chapter 3: Baire category and open mapping theorems

Hilbert Spaces. Hilbert space is a vector space with some extra structure. We start with formal (axiomatic) definition of a vector space.

j=1 u 1jv 1j. 1/ 2 Lemma 1. An orthogonal set of vectors must be linearly independent.

DEFINABLE OPERATORS ON HILBERT SPACES

Functional Analysis. Martin Brokate. 1 Normed Spaces 2. 2 Hilbert Spaces The Principle of Uniform Boundedness 32

NEW BOUNDS FOR TRUNCATION-TYPE ERRORS ON REGULAR SAMPLING EXPANSIONS

COMMON COMPLEMENTS OF TWO SUBSPACES OF A HILBERT SPACE

Analysis Finite and Infinite Sets The Real Numbers The Cantor Set

96 CHAPTER 4. HILBERT SPACES. Spaces of square integrable functions. Take a Cauchy sequence f n in L 2 so that. f n f m 1 (b a) f n f m 2.

Functional Analysis HW #1

Course 212: Academic Year Section 1: Metric Spaces

FUNCTIONAL ANALYSIS HAHN-BANACH THEOREM. F (m 2 ) + α m 2 + x 0

MATH 51H Section 4. October 16, Recall what it means for a function between metric spaces to be continuous:

FUNCTIONAL ANALYSIS LECTURE NOTES: COMPACT SETS AND FINITE-DIMENSIONAL SPACES. 1. Compact Sets

Hilbert spaces. 1. Cauchy-Schwarz-Bunyakowsky inequality

Brownian Motion and Conditional Probability

Def. A topological space X is disconnected if it admits a non-trivial splitting: (We ll abbreviate disjoint union of two subsets A and B meaning A B =

Functional Analysis, Math 7321 Lecture Notes from April 04, 2017 taken by Chandi Bhandari

Rudiments of Hilbert Space Theory

Metric Spaces and Topology

5 Compact linear operators

Introduction to Functional Analysis With Applications

Lecture 5: Hodge theorem

Elements of Convex Optimization Theory

Part III. 10 Topological Space Basics. Topological Spaces

Shift Invariant Spaces and Shift Generated Dual Frames for Local Fields

Functional Analysis I

Iowa State University. Instructor: Alex Roitershtein Summer Exam #1. Solutions. x u = 2 x v

1 The Projection Theorem

MAT 578 FUNCTIONAL ANALYSIS EXERCISES

Chapter 8 Integral Operators

Analysis II Lecture notes

Functional Analysis II held by Prof. Dr. Moritz Weber in summer 18

Functional Analysis Exercise Class

Analysis III Theorems, Propositions & Lemmas... Oh My!

OPERATOR THEORY ON HILBERT SPACE. Class notes. John Petrovic

MAT 257, Handout 13: December 5-7, 2011.

Linear Normed Spaces (cont.) Inner Product Spaces

Spectral theory for compact operators on Banach spaces

Fredholm Theory. April 25, 2018

Transcription:

V. SUBSPACES AND ORTHOGONAL PROJECTION In this chapter we will discuss the concept of subspace of Hilbert space, introduce a series of subspaces related to Haar wavelet, explore the orthogonal projection onto Hilbert subspaces. Definition 1. Let H be a Hilbert space, K be a linear subspace of H (i.e.,for any α, β C and any k 1, k 2 K, we have αk 1 + βk 2 K ). If K is also closed under the norm of H, ( i.e., any {k n } n=1 K, if {k n } n=1 converges in the norm of H to some k H, then k K.) Then K is called a closed subspace of H. We often omit closed and call such K a subspace of H. Now let us turn to the specific Hilbert space L 2 (R) and define a sequence of subspaces of L 2 (R) which are related to Haar wavelet.(the connection will not be clear until later chapters.) Example 1 For any n Z, define a subset of L 2 (R) as follows: Let V n = {f L 2 (R) for any j Z, f [ j 2 n, j+1 2 n ) is constant }. It is trivial to check that each V n is a linear subspace. To see that V n is closed under the L 2 (R) norm is beyond the scope of our course. We will accept this fact. Clearly, we see that for any n Z, V n V n+1, and f(x) V n f(2x) V n+1. We leave the proof of these fact to the reader. Several other properties are less trivial, we treat them in the following lemma. For any subset A of a Hilbert space H, we use A to denote the closure of A in H under the norm of H, (i.e., x A for any ε > 0, there is a y A such that x y H < ε.) Using this terminology, we can rephrase Lemma 3 of last chapter to say that V = L 2 (R). Lemma 1. For any n Z, let V n constant }. Then = {f L 2 (R) for any j Z, f [ j 2 n, j+1 2 n ) is (a)for any n Z, V n V n+1. (b)for any n Z, f(x) V n f(2x) V n+1. (c) n Z V n = L 2 (R), (d) n Z V n = {0}. 1 Typeset by AMS-TEX

2 V. SUBSPACES AND ORTHOGONAL PROJECTION (e)if ϕ(x) = { 1 0 x < 1 0 otherwise then ϕ(x) V 0 and {ϕ(x l) l Z} is a complete orthonormal system of V 0. Proof. (c)clearly n Z V n L 2 (R), so we only need to show L 2 (R) n Z V n. By Lemma 3 of Last chapter, for any f L 2 (R), any ε > 0, there is g V, such that f g < ε, where V is defined as in last chapter. For such g V, according to the definition of V, there is m Z, such that f [ j 2 m, j+1 2 m ) is constant for any j Z. This means f V m n Z V n. In short, for any f L 2 (R), any ε > 0, there is g n Z V n, such that f g < ε, so f n Z V n. (d)clearly {0} n Z V n, so we only need to show n Z V n {0}. Recall that for each pair of n, l Z, 2 n 2l 2l + 1 2 x [, 2n+1 2 n+1 ) H n,l (x) = 2 n 2 x [ 2l + 1 2l + 2, 2n+1 2 n+1 ) 0 otherwise. Observe that for any fixed n Z, the inner product of H n,l with any function in V n is 0 for any l Z. Now suppose f n Z V n, then f V n for each n Z. Hence For each n Z, f, H n,l = 0 for all l Z. Since we have already proved that {H n,l n, l Z} is a complete orthonormal system in L 2 (R), this means that f = 0. Hence n Z V n {0}. The proof of (e) is left to the reader. Generalizing above sequence of subspaces related to Haar wavelet, we have the concept of Multiresolution Analysis. Definition 2. For any n Z, let V n be a subspace of L 2 (R). Suppose {V n } n Z satisfies the following conditions: (a)for any n Z, V n V n+1 ; (b)for any n Z, f(x) V n f(2x) V n+1 ; (c) n Z V n = L 2 (R); (d) n Z V n = {0}; (e)there exists ϕ(x) V 0 such that {ϕ(x l) l Z} is a complete orthonormal system of V 0.

V. SUBSPACES AND ORTHOGONAL PROJECTION 3 Then {V n } n Z is called a Multiresolution Analysis. Multiresolution Analysis plays an important role in wavelet theory. In order to understand the mechanism involved, we need to know something about orthogonal projection and direct sum decomposition. Next we turn to general Hilbert space to introduce the concept of orthogonal projection. But first we state a simple lemma. Lemma 2. Lei H be a Hilbert space, f, g H. Then f + g 2 + f g 2 = 2 f 2 + g 2. The proof is simple and left to the reader. Proposition 1. Let K be a subspace of Hilbert space H, h H. Then there is a unique k 0 K, such that h k 0 = inf{ h k k K}. Proof. Since h k 0 for any k K, so d = inf{ h k k K} exists. By definition of inf we see that 1) h k d for any k K, 2)for any ε > 0, there is a k ε K such that d h k ε < d + ε. Thus it is not hard to find a sequence {k n } n=1 K such that lim n h k n = d. Hence lim n h k n 2 = d 2. So for any ε > 0, there exists N N, such that for any n > N, When n, m > N, according to Lemma 2, h k n 2 < d 2 + ε2 2. k m k n 2 = 2 h k n 2 + 2 h k m 2 4 h k n + k m 2 2 < d 2 + ε2 2 + d2 + ε2 2 4d2 = ε 2. Hence {k n } n=1 is a Cauchy sequence in H, so there is k 0 H, such that lim n k n k 0 = 0. Since {k n } n=1 K and K is a subspace, so k 0 K. Now d h k 0 = h k n + k n k 0 h k n + k n k 0, By taking limit to both side of inequality, we see that h k 0 = d.

4 V. SUBSPACES AND ORTHOGONAL PROJECTION To see the uniqueness of such k 0, we assume that there is k o K, such that h k 0 = h k 0 = d. Then since 2d 2(h k 0 + k 0 ) = h k 0 + h k 2 0 h k 0 + h k 0 = 2d, so by Lemma 2, k 0 k 0 2 = 2 h k 0 2 + 2 h k 0 2 h k 0 + h k 0 2 = 0. Therefore k 0 k 0. Recall from Chapter 1, when E is a subset of H, we say that f H is orthogonal to E if f is orthogonal to every element in E. We will use f E to denote this situation. Proposition 2. Let K be a subspace of Hilbert space H, h H, k 0 K. Then the following are equivalent: (a) h k 0 = inf{ h k k K}. (b)h k 0 K. Proof. (a)= (b) Let d = inf{ h k k K}, then h k0 = d. 0 k K, since K is a subspace, certainly k 0 k K. So For any So d 2 h k 0 + k 2 = h k 0 + k, h k 0 + k = h k 0 2 + 2Re h k 0, k + k 2 = d 2 + 2Re h k 0, k + k 2. 2Re h k 0, k k 2 1. In the argument above, if we replace k with εk for any ε > 0, the computation still holds, and we get or 2Re h k 0, εk εk 2 1 2Re h k 0, k k 2 ε. Hence Re h k 0, k = 0. Likewise, we can replace k with iεk, similarly, we get Im h k 0, k = 0. So h k 0, k = 0 for all k K. (b)= (a)for any k K, since K is a subspace, certainly k 0 k K. Hence h k 0, k 0 k = 0. Thus h k 2 = h k 0 + k 0 k 2 = h k 0 2 + k 0 k 2 h k 0 2. Thus it is easily checked that h k 0 = inf{ h k k K}.

V. SUBSPACES AND ORTHOGONAL PROJECTION 5 Remark When K is a subspace of Hilbert space H, for any h H, there is a unique k 0 K such that h k 0 K and h = k 0 + h k 0. If we consider the subset of H defined by M = {x H x K}, then it can be checked that M is a linear subspace of H. Furthermore, if a sequence {x n } n=1 M and lim n x n x = 0 for some x H, then x M. In other words, M is closed under the norm of H. Hence M is a (closed) subspace of H. The above two proposition says that for any h H, there is a unique k 0 K, a unique m 0 = h k 0 M and h = k 0 + m 0. Definition 3. Suppose that K is a subspace of Hilbert space H, h H. Then the unique element k 0 K satisfying h k 0 K ( equivalently h k 0 = inf{ h k k K}.) is call the orthogonal projection of h onto subspace K. We denote P K h = k 0. The (closed) subspace M = {x H x K} is called the orthogonal complement of K in H. We denote M = H K. Remark When K is a subspace of Hilbert space H, M = H K, let us investigate the subspace H M. For any h H, by definition of orthogonal complement, h H M if and only if h M. By definition of M, certainly for any k K, we have k M. This means K H M. For H M K, consider any h H with h M, since there is a unique h K K, a unique h M M such that h = h K + h M, we see that 0 = h, h M = h K, h M + h M, h M = h M 2. So h M = 0 and h = h K K. Thus K = H M = H (H K). Thus orthogonal complement is a symmetric relation. Definition 4. Suppose that K, M are subspace of Hilbert space H. If K, M are orthogonal complement of each other in H, then we say H is the direct sum of K and M. We denote H = K M. Lastly, we consider the problem of how to calculate the orthogonal projection of h onto any subspace K of Hilbert space H. We will see, once we have a complete orthonormal system of K, this can be easily done. Proposition 3. Let H be a Hilbert space with subspace K, {e j } j J is a complete orthonormal system of K, where J is any countable index set. Then for h H, P K h = j J h, e j e j. Proof. First of all, according to Bessel s inequality in Chapter 1, h, e n 2 <. j J

6 V. SUBSPACES AND ORTHOGONAL PROJECTION Hence by Corollary 1 in Chapter 1, j J h, e j e j converges in H. Furthermore, since K is subspace of H, {e j } j J K, so actually j J h, e j e j converges in some element in H. Let us denote g = j J h, e j e j. see Now we do some computations using Lemma 3 of Chapter 1. For any j J, we g, e l = j J h, e j e j, e l = h, e l. This means that for any j J, h g, e j = h, e j g, e j = 0. Since h g is orthogonal to each element of a complete orthonormal system of K, we see that h g K. According to Proposition 2, g is the unique element such that h g = inf{ h k k K}. That is to say, g = P K h. Sometimes we need to compute orthogonal projection of some elements onto different subspaces. The following is a case often encountered. Proposition 4. Let H be a Hilbert space with subspace K 1, K 2. If K 1 K 2, then for h H, P K1 h = P K1 (P K2 h). Proof. Let {e j } j J is a complete orthonormal system of K 1, where J is any countable index set. According to Proposition 3, we have for h H, P K1 h = j J h, e j e j, P K1 (P K2 h) = j J P K2 h, e j e j. Note that h P K2 h K 2. Since K 1 K 2, we have h P K2 h K 1. Since {e j } j J is a complete orthonormal system of K 1, so j J, we have h P K2 h, e j = 0. So h, e j = P K2 h, e j for any j J. Hence P K1 h = P K1 (P K2 h). This brings Chapter 5 to the end. In next chapter we will apply what we have learned here to a specific structure in L 2 (R), namely the so called Multiresolution Analysis.