FUNCTIONAL ANALYSIS LECTURE NOTES CHAPTER 2. OPERATORS ON HILBERT SPACES

Size: px
Start display at page:

Download "FUNCTIONAL ANALYSIS LECTURE NOTES CHAPTER 2. OPERATORS ON HILBERT SPACES"

Transcription

1 FUNCTIONAL ANALYSIS LECTURE NOTES CHAPTER 2. OPERATORS ON HILBERT SPACES CHRISTOPHER HEIL 1. Elementary Properties and Examples First recall the basic definitions regarding operators. Definition 1.1 (Continuous and Bounded Operators). Let, Y be normed linear spaces, and let L: Y be a linear operator. (a) L is continuous at a point f if f n f in implies Lf n Lf in Y. (b) L is continuous if it is continuous at every point, i.e., if f n f in implies Lf n Lf in Y for every f. (c) L is bounded if there exists a finite K 0 such that f, Lf K f. Note that Lf is the norm of Lf in Y, while f is the norm of f in. (d) The operator norm of L is L = sup Lf. f =1 (e) We let B(, Y ) denote the set of all bounded linear operators mapping into Y, i.e., B(, Y ) = {L: Y : L is bounded and linear}. If = Y = then we write B() = B(, ). (f) If Y = F then we say that L is a functional. The set of all bounded linear functionals on is the dual space of, and is denoted = B(, F) = {L: F : L is bounded and linear}. We saw in Chapter 1 that, for a linear operator, boundedness and continuity are equivalent. Further, the operator norm is a norm on the space B(, Y ) of all bounded linear operators from to Y, and we have the composition property that if L B(, Y ) and K B(Y, Z), then KL B(, Z), with KL K L. Date: February 20, These notes closely follow and expand on the text by John B. Conway, A Course in Functional Analysis, Second Edition, Springer,

2 2 CHRISTOPHER HEIL Exercise 1.2. Suppose that L: Y is a bounded map of a Banach space into a Banach space Y. Prove that if there exists a c > 0 such that Lf c f for every f, then range(l) is a closed subspace of Y. Exercise 1.3. Let C b (R n ) be the set of all bounded, continuous functions f : R n F. Let C 0 (R n ) be the set of all continuous functions f : R n F such that lim x f(x) = 0 (i.e., for every ε > 0 there exists a compact set K such that f(x) < ε for all x / K). Prove that these are closed subspaces of L (R n ) (under the L -norm; note that for a continuous function we have f = sup f(x) ). Define δ : C b (R n ) F by δ(f) = f(0). Prove that δ is a bounded linear functional on C b (R n ), i.e., δ (C b ), and find δ. This linear functional is the delta distribution (see also Exercise 1.26 below). Example 1.4. In finite dimensions, all linear operators are given by matrices, this is just standard finite-dimensional linear algebra. Suppose that is an n-dimensional complex normed vector space and Y is an m- dimensional complex normed vector space. By definition of dimension, this means that there exists a basis B = {x 1,..., x n } for and a basis B Y = {y 1,..., y m } for Y. If x, then x = c 1 x c n x n for a unique choice of scalars c i. Define the coordinates of x with respect to the basis B to be [x] B = c 1. c n C n. The vector x is completely determined by its coordinates, and conversely each vector in C n is the coordinates of a unique x. The mapping x [x] B is a linear mapping of onto C n. We similarly define [y] BY C m for vectors y Y. Let A: Y be a linear map (it is automatically bounded since is finite-dimensional). Then A transforms vectors x into vectors Ax Y. The vector x is determined by its coordinates [x] B and likewise Ax is determined by its coordinates [Ax] BY. The vectors x and Ax are related through the linear map A; we will show that the coordinate vectors [x] B and [Ax] BY are related by multiplication by an m n matrix determined by A. We call this matrix the standard matrix of A with respect to B and B Y, and denote it by [A] B,B Y. That is, the standard matrix should satisfy [Ax] BY = [A] B,B Y [x] B, x. We claim that the standard matrix is the matrix whose columns are the coordinates of the vectors Ax k, i.e., [A] B,B Y = [Ax 1 ] BY [Ax n ] BY.

3 CHAPTER 2. OPERATORS ON HILBERT SPACES 3 To see this, choose any x and let x = c 1 x c n x n be its unique representation with respect to the basis B. Then c 1 [A] B,B Y [x] B = [Ax 1 ] BY [Ax n ] BY. c n = c 1 [Ax 1 ] BY + + c n [Ax n ] BY = [c 1 Ax c n Ax n ] BY = [A(c 1 x c n x n )] BY = [Ax] BY. Exercise 1.5. Extend the idea of the preceding example to show that that any linear mapping L: l 2 (N) l 2 (N) (and more generally, L: H K with H, K separable) can be realized in terms of multiplication by an (infinite but countable) matrix. Exercise 1.6. Let A be an m n complex matrix, which we view as a linear transformation A: C n C m. The operator norm of A depends on the choice of norm for C n and C m. Compute an explicit formula for A, in terms of the entries of A, when the norm on C n and C m is taken to be the l 1 norm. Then do the same for the l norm. Compare your results to the version of Schur s Lemma given in Theorem The following example is one that we will return to many times. Example 1.7. Let {e n } n N be an orthonormal basis for a separable Hilbert space H. Then we know that every f H can be written f = f, e n e n. n=1 Fix any sequence of scalars λ = (λ n ) n N, and formally define Lf = λ n f, e n e n. (1.1) n=1 This is a formal definition because we do not know a priori that the series above will converge in other words, equation (1.1) may not make sense for every f. Note that if H = l 2 (N) and {e n } n N is the standard basis, then L is given by the formula Lx = (λ 1 x 1, λ 2 x 2,... ), x = (x 1, x 2,... ) l 2 (N). We will show the following (the l -norm of the sequence λ is λ = sup n λ n ). (a) The series defining Lf in (1.1) converges for each f H if and only if λ l. In this case L is a bounded linear mapping of H into itself, and L = λ.

4 4 CHRISTOPHER HEIL (b) If λ / l, then L defines an unbounded linear mapping from the domain { } domain(l) = f H : λ n f, e n 2 < (which is dense in H) into H. Proof. (a) Suppose that λ l, i.e., λ is a bounded sequence. Then for any f we have λ n f, e n 2 λ 2 f, e n 2 = λ 2 f 2 <, n=1 n=1 n=1 (1.2) so the series defining Lf converges (because {e n } is an orthonormal sequence). Moreover, the preceding calculation also shows that Lf 2 = n=1 λ n f, e n 2 λ 2 f 2, so we see that L λ. On the other hand, by orthonormality we have Le n = λ n e n (i.e., each e n is an eigenvector for L with eigenvalue λ n ). Since e n = 1 and Le n = λ n e n = λ n we conclude that L = sup f =1 Lf sup n N Le n = sup λ n = λ. n N The converse direction will be covered by the proof of part (b). (b) Suppose that λ / l, i.e., λ is not a bounded sequence. Then we can find a subsequence (λ nk ) k N such that λ nk k for each k. Let c nk = 1 and define all other c k n to be zero. Then n c n 2 = 1 k <, so f = k 2 n c ne n converges (and c n = f, e n ). But the formal series Lf = n λ nc n e n does not converge, because c n λ n 2 = c nk λ nk 2 k 2 =. k 2 n=1 k=1 In fact, the series defining Lf in (1.1) only converges for those f which lie in the domain defined in (1.2). That domain is dense because it contains the finite span of {e n } n N, which we know is dense in H. Further, that domain is a subspace of H (exercise), so it is an innerproduct space. The map L: domain(l) H is a well-defined, linear map, so it remains only to show that it is unbounded. This follows from the facts that e n domain(l), e n = 1, and Le n = λ n e n = λ n. k=1 Exercise 1.8. Continuing Example 1.7, suppose that λ l and set δ = inf n λ n. Prove the following. (a) L is injective if and only if λ n 0 for every n. (b) L is surjective if and only if δ > 0 (if δ = 0, use an argument similar to the one used in part (b) of Example 1.7 to show that range(l) is a proper subset of H). (c) If δ = 0 but λ n 0 for every n then range(l) is a dense but proper subspace of H. (d) Prove that L is unitary if and only if λ n = 1 for every n.

5 CHAPTER 2. OPERATORS ON HILBERT SPACES 5 In Example 1.7, we saw an unbounded operator whose domain was a dense but proper subspace of H. This situation is typical for unbounded operators, and we often write L: Y even when L is only defined on a subset of, as in the following example. Example 1.9 (Differentiation). Consider the Hilbert space H = L 2 (0, 1), and define an operator D : L 2 (0, 1) L 2 (0, 1) by Df = f. Implicitly, we mean by this that D is defined on the largest domain that makes sense, namely, domain(d) = { f L 2 (0, 1) : f is differentiable and f L 2 (0, 1) }. Note that if f domain(d), then Df is well-defined, Df L 2 (0, 1), and Df 2 <. Thus every vector in domain(d) maps to a vector in L 2 (0, 1) which necessarily has finite norm. Yet D is unbounded. For example, if we set e n (x) = e inx then e n 2 = 1, but De n (x) = e n (x) = ineinx so De n 2 = n. While each vector De n has finite norm, there is no upper bound to these norms. Since the e n are unit vectors, we conclude that D =. The following definitions recall the basic notions of measures and measure spaces. For full details, consult a book on real analysis. 1 Definition 1.10 (σ-algebras, Measurable Sets and Functions). Let be a set, and let Ω be a collection of subsets of. Then Ω is a σ-algebra if (a) Ω, (b) If E Ω then \ E Ω (i.e., Ω is closed under complements), (c) If E 1, E 2, Ω then E k Ω (i.e., Ω is closed under countable unions) The elements of Ω are called the measurable subsets of. If we choose F = R then we usually allow functions on to take extended-real values, i.e., f(x) is allowed to take the values ±. An extended-real-valued function f : [, ] is called a measurable function if {x : f(x) > a} is measurable for each a R. If we choose F = C then we require functions on to take (finite) complex values there is no complex analogue of ±. A complex-valued function f : C is called a measurable function if its real and imaginary parts are measurable (real-valued) functions. Definition 1.11 (Measure Space). Let be a set and Ω a σ-algebra of subsets of. Then a function µ on Ω is a (positive) measure if (a) 0 µ(e) + for all E Ω, (b) If E 1, E 2,... is a countable family of disjoint sets in Ω, then ( ) µ E k = µ(e k ). k=1 1 For example, R. Wheeden and A. Zygmund, Measure and Integral, Marcel Dekker, 1977, or G. Folland, Real Analysis, Second Edition, Wiley, k=1

6 6 CHRISTOPHER HEIL In this case, (, Ω, µ) is called a measure space. If µ() <, then we say that µ is a finite measure. If there exist countably many subsets E 1, E 2,... such that = E k and µ(e k ) < for all k, then we say that µ is σ-finite. For example, Lebesgue measure on R n is σ-finite. It is often useful to allow measures to take negative values. Definition 1.12 (Signed Measure). Let be a set and Ω a σ-algebra of subsets of. Then a function µ on Ω is a signed measure if (a) µ(e) + for all E Ω and µ( ) = 0, (b) If E 1, E 2,... is a countable family of disjoint sets in Ω, then ( ) µ E k = µ(e k ). Definition 1.13 (Integration). Let (, Ω, µ) be a measure space. k=1 (a) If f : [0, ] is a nonnegative, measurable function, then the integral of f over with respect to µ is { ( f dµ = f(x) dµ(x) = sup inf f(x) ) } µ(e j ), x E j where the supremum is taken over all decompositions E = E 1 E N of E as the union of a finite number of disjoint measurable sets E k (and where we take the convention that 0 = 0 = 0). then (b) If f : [, ] and we define k=1 f + (x) = max{f(x), 0}, f (x) = min{f(x), 0}, f dµ = f + dµ j f dµ, as long as this does not have the form (in that case the integral would be undefined). Since f = f + +f and f dµ always exists (either as a finite number or as ), it follows that f dµ exists and is finite f dµ <. (c) If f : C, then f dµ = Re (f) dµ + i Im (f) dµ, as long as both integrals on the right are defined and finite. There are many other equivalent definitions of the integral.

7 CHAPTER 2. OPERATORS ON HILBERT SPACES 7 Definition 1.14 (L p Spaces). Let (, Ω, µ) be a measure space, and fix 1 p <. Then L p () consists of all measurable functions f : [, ] (if we choose F = R) or f : C (if we choose F = C) such that f p p = f(x) p dµ(x) <. Then L p () is a vector space under the operations of addition of functions and multiplication of a function by a scalar. Additionally, the function p defines a semi-norm on L p (). Usually we identify functions that are equal almost everywhere (we say that f = g a.e. if µ{x : f(x) g(x)} = 0), and then becomes a norm on L p (). For p = we define L () to be the set of measurable functions that are essentially bounded, i.e., for which there exists a finite constant M such that f(x) M a.e. Then f = ess sup f(x) = inf { M 0 : f(x) M a.e. } x is a semi-norm on L (), and is a norm if we identify functions that are equal almost everywhere. For each 1 p, the space L p () is a Banach space under the above norm. Exercise 1.15 (l p Spaces). Counting measure on a set is defined by µ() = card(e) if E is a finite subset of, and µ() = if E is an infinite subset. Let Ω = P() (the set of all subsets of ), and show that (, Ω, µ) is a measure space. Show that L p (, Ω, µ) = l p (). Show that µ is σ-finite if and only if is countable. Exercise 1.16 (The Delta Measure). Let = R n and Ω = P(). Define δ(e) = 1 if 0 E and δ(e) = 0 if 0 / E. Prove that δ is a measure, and find a formula for R n f(x) dδ(x). Sometimes this integral is written informally as R n f(x) δ(x) dx, but note that δ is a measure on R n, not a function on R n (see also Exercise 1.26 below). Exercise Fix 0 g L 1 (R n ), under Lebesgue measure. Prove that µ(e) = g(x) dx E defines a finite measure on R n. With this preparation, we can give some additional examples of operators on Banach or Hilbert spaces. Example 1.18 (Multiplication Operators). Let (, Ω, µ) be a measure space, and let φ L () be a fixed measurable function. Then for any f L 2 () we have that fφ is measurable, and fφ 2 2 = f(x) φ(x) 2 dx f(x) 2 φ 2 dx = φ 2 f 2 2 <,

8 8 CHRISTOPHER HEIL so fφ L 2 (). Therefore, the multiplication operator M φ : L 2 () L 2 () given by M φ f = fφ is well-defined, and the calculation above shows that M φ f 2 φ f 2. Therefore M φ is bounded, and M φ φ. If we assume that µ is σ-finite, then we can show that M φ = φ, as follows. Choose any ε > 0. Then by definition of L -norm, the set E = {x : φ(x) > φ ε} has positive measure. Since is σ-finite, we can write = F m where each µ(f m ) <. Since E = (E F m ) is a countable union, we must have µ(e F m ) > 0 for some m. Let F = E F m, and set f = 1 χ µ(f ) 1/2 F. Then f 2 = 1, but M φ f 2 ( φ ε) f 2. Hence M φ 2 φ ε. Exercise: Find an example of a measure µ that is not σ-finite and a function φ such that M φ < φ. Exercise Let (, Ω, µ) be a measure space, and let φ be a fixed measurable function. Prove that if fφ L 2 () for every f L 2 (), then we must have φ L (). Solution. Assume φ / L (). Set E k = {x : k φ(x) < k + 1}. The E k are measurable and disjoint, and since φ is not in L () there must be infinitely many E k with positive measure. Choose any E nk, k N, all with positive measure and let E = E nk. Define 1 f(x) = k µ(e nk ), x E 1/2 n k, 0, x / E. Then but which is a contradiction. f 2 dµ = fφ 2 dµ k=1 k=1 E nk 1 k 2 µ(e nk ) = Enk k 2 k 2 µ(e nk ) = Exercise Continuing Example 1.18, do the following. k=1 k=1 1 k 2 <, 1 =, (a) Determine a necessary and sufficient condition on φ which implies that M φ : L 2 () L 2 () is injective. (b) Determine a necessary and sufficient condition on φ which implies that M φ : L 2 () L 2 () is surjective. (c) Prove that if M φ is injective but not surjective then M 1 φ : range(m φ) L 2 () is unbounded. (d) Extend from the case p = 2 to any 1 p.

9 CHAPTER 2. OPERATORS ON HILBERT SPACES 9 Example 1.21 (Integral Operators). Let (, Ω, µ) be a σ-finite measure space. An integral operator is an operator of the form Lf(x) = k(x, y) f(y) dµ(y). (1.3) This is just a formal definition, we have to provide conditions under which this makes sense, and the following two theorems will provide such conditions. The function k that determines the operator is called the kernel of the operator (not to be confused with the kernel/nullspace of the operator!). Note that an integral operator is just a generalization of matrix multiplication. For, if A is an m n matrix with entries a ij and u C n, then Au C m, and its components are given by n (Au) i = a ij u j, i = 1,..., m. j=1 Thus, the values k(x, y) are analogous to the entries a ij of the matrix A, and the values Lf(x) are analogous to the entries (Au) i. The following result shows that if the kernel is square-integrable, then the corresponding integral operator is bounded. Later we will define the notion of a Hilbert Schmidt operator. For the case of integral operators mapping L 2 () into itself, it can be shown that L is a Hilbert Schmidt operator if and only if the kernel k belongs to L 2 ( ). Theorem 1.22 (Hilbert Schmidt Integral Operators). Let (, Ω, µ) be a σ-finite measure space, and choose a kernel k L 2 ( ). That is, assume that k 2 2 = k(x, y) 2 dµ(x) dµ(y) <. Then the integral operator given by (1.3) defines a bounded mapping of L 2 () into itself, and L k 2. Proof. Although a slight abuse of the order of logic (technically we should show Lf exists before trying to compute its norm), the following calculation shows that L is well-defined and is a bounded mapping of L 2 () into itself: Lf 2 2 = Lf(x) 2 dµ(x) = ( 2 k(x, y) f(y) dµ(y) dµ(x) ) ( ) k(x, y) 2 dµ(y) f(y) 2 dµ(y) dµ(x)

10 10 CHRISTOPHER HEIL = = k 2 2 f 2 2, k(x, y) 2 dµ(y) f 2 2 dµ(x) where the inequality follows by applying Cauchy Schwarz to the inner integral. Thus L is bounded, and L k 2. The following result is one version of Schur s Lemma. There are many forms of Schur s Lemma, this is one particular special case. Exercise: Compare the hypotheses of the following result to the operator norms you calculated in Exercise 1.6. Theorem Let (, Ω, µ) be a σ-finite measure space, and Assume that k is a measurable function on which satisfies the mixed-norm conditions C 1 = ess sup x k(x, y) dµ(y) < and C 2 = ess sup y k(x, y) dµ(x) <. Then the integral operator given by (1.3) defines a bounded mapping of L 2 () into itself, and L (C 1 C 2 ) 1/2. Proof. Choose any f L 2 (). Then, by applying the Cauchy Schwarz inequality, we have Lf 2 2 = Lf(x) 2 dµ(x) = ( = C 1 C 1 2 k(x, y) f(y) dµ(y) dµ(x) k(x, y) 1/2 ( k(x, y) 1/2 f(y) ) dµ(y)) 2 dµ(x) ( ) ( ) k(x, y) dµ(y) k(x, y) f(y) 2 dµ(y) dµ(x) C 1 k(x, y) f(y) 2 dµ(y) dµ(x) = C 1 C 2 f 2 2, f(y) 2 f(y) 2 C 2 dµ(y) k(x, y) dµ(x) dµ(y) where we have used Tonelli s Theorem to interchange the order of integration (here is where we needed the fact that µ is σ-finite). Thus L is bounded and L (C 1 C 2 ) 1/2.

11 CHAPTER 2. OPERATORS ON HILBERT SPACES 11 Exercise Consider what happens in the preceding example if we take 1 p instead of p = 2. In particular, in part b, show that if C 1, C 2 < then L: L p () L p () is a bounded mapping for each 1 p (try to do p = 1 or p = first). Exercise 1.25 (Volterra Operator). Define L: L 2 [0, 1] L 2 [0, 1] by Show directly that L is bounded. k : [0, 1] 2 F defined by Lf(x) = x 0 f(y) dy. Then show that L is an integral operator with kernel k(x, y) = { 1, y x, 0, y > x. Observe that k L 2 ([0, 1] 2 ), so L is compact. This operator is called the Volterra operator. Exercise 1.26 (Convolution). Convolution is one of the most important examples of integral operators. Consider the case of Lebesgue measure on R n. Given functions f, g on R n, their convolution is the function f g defined by (f g)(x) = f(y) g(x y) dy, R n provided that the integral makes sense. Note that with g fixed, the mapping f f g is an integral operator with kernel k(x, y) = g(x y). (a) Let g L 1 (R n ) be fixed. Use Schur s Lemma (Theorem 1.23) to show that Lf = f g is a bounded mapping of L 2 (R n ) into itself. In fact, use Exercise 1.24 to prove Young s Inequality: If f L p (R n ) (1 p ) and g L 1 (R n ), then f g L p (R n ), and f g p f p g 1. In particular, L 1 (R n ) is closed under convolution. (b) Note that we cannot use the Hilbert Schmidt condition (Theorem 1.22) to prove Young s Inequality, since g(x y) 2 dx dy =, R n R n even if we assume that g L 2 (R n ). (c) Prove that convolution is commutative, i.e., that f g = g f. (d) Prove that there is no identity element in L 1 (R n ), i.e., there is no function g L 1 (R n ) such that f g = f for all f L 1 (R n ). This is not trivial it is easier to do if you make use of the Fourier transform on R n, and in particular use the Riemann Lebesgue Lemma to derive a contradiction.

12 12 CHRISTOPHER HEIL (e) Some texts do talk informally about a delta function that is an identity element for convolution, defined by the conditions {, x = 0, δ(x) = and δ(x) dx = 1, 0, x 0, R n but no such function actually exists. In particular, the function δ defined on the left-hand side of the line above is equal to zero a.e., and hence is the zero function as far as Lebesgue integration is concerned. That is, we have δ(x) dx = 0, not 1. The delta function is R n really just an informal use of the delta distribution (see Exercise 1.3) or the delta measure (see Exercise 1.16). Show that if we define the convolution of a function f with the delta measure δ to be (f δ)(x) = f(x y) dδ(y), (1.4) R n then f δ = f for all f L 1 (R n ). Note that in the informal notation of Exercise 1.16, (1.4) reads (f δ)(x) = f(x y) δ(y) dy, R n which perhaps explains the use of the term delta function. Exercise Prove that L 1 (R n ) is not closed under pointwise multiplication. That is, prove that there exist f, g L 1 (R n ) such that the pointwise product h(x) = (fg)(x) = f(x)g(x) does not belong to to L 1 (R n ). Exercise 1.28 (Convolution Continued). (a) Consider the space L p [0, 1], where we think of functions in L p [0, 1] as being extended 1-periodically to the real line. Define convolution on the circle by (f g)(x) = 1 0 f(y) g(x y) dy, where the periodicity is used to define g(x y) when x y lies outside [0, 1] (equivalently, replace x y by x y mod 1, the fractional part of x y). Prove a version of Young s Inequality for L p [0, 1]. (b) Consider the sequence space l p (Z). Define convolution on Z by (x y) n = m Z x m y n m. Prove a version of Young s Inequality for l p (Z). Prove that l 1 (Z) contains an identity element with respect to convolution, i.e., there exists a sequence in l 1 (Z) (typically denoted δ) such that δ x = x for every x l p (Z). (c) Identify the essential features needed to define convolution on more general domains, and prove a version of Young s Inequality for that setting.

13 CHAPTER 2. OPERATORS ON HILBERT SPACES 13 Exercise 1.29 (Convolution and the Fourier Transform). Let F be the Fourier transform on the circle, i.e., it is the isomorphism F : L 2 [0, 1] l 2 (Z) given by Ff = ˆf = { ˆf(n)} n Z, where ˆf(n) = f, e n = 1 0 f(x) e 2πinx dx, e n (x) = e 2πinx. (a) Prove that the Fourier transform converts convolution in to multiplication. That is, prove that if f, g L 2 [0, 1], then (f g) = ˆf ĝ, i.e., (f g) (n) = ˆf(n) ĝ(n), n Z. (b) Note that if g L 2 [0, 1], then g L 1 [0, 1], so by Young s Inequality we have that f g L 2 [0, 1]. Holding g fixed, define an operator L: L 2 [0, 1] L 2 [0, 1] by Lf = f g. Since {e n } n Z is an orthonormal basis for L 2 [0, 1], we have f = n Z ˆf(n) e n, f L 2 [0, 1]. Show that Lf = f g = n Z ĝ(n) ˆf(n) e n, f L 2 [0, 1]. Thus, in the Fourier domain, convolution acts by changing or adjusting the amount that each component or frequency e n contributes to the representation of the function in this basis: the weight ˆf(n) for frequency n is replaced by the weight ĝ(n) ˆf(n). Explain why this says that L is analogous to multiplication by a diagonal operator. In engineering parlance, convolution is also referred to as filtering. Explain why this terminology is appropriate. Compare this operator L to Example The Adjoint of an Operator Example 2.1. Note that the dot product on R n is given by x y = x T y, while the dot product on C n is x y = x T ȳ. Let A be an m n real matrix. Then x Ax defines a linear map of R n into R m, and its transpose A T satisfies x R n, y R m, Ax y = (Ax) T y = x T A T y = x (A T y). Similarly, if A is an m n complex matrix, then its Hermitian or adjoint matrix A H = A T satisfies x C n, y C m, Ax y = (Ax) T ȳ = x T A T ȳ = x (A H y). Theorem 2.2 (Adjoint). Let H and K be Hilbert spaces, and let A: H K be a bounded, linear map. Then there exists a unique bounded linear map A : K H such that x H, y K, Ax, y = x, A y.

14 14 CHRISTOPHER HEIL Proof. Fix y K. Then Lx = Ax, y is a bounded linear functional on H. By the Riesz Representation Theorem, there exists a unique vector h H such that Ax, y = Lx = x, h. Define A y = h. Verify that this map A is linear (exercise). To see that it is bounded, observe that A y = h = sup x, h x =1 = sup Ax, y x =1 sup Ax y x =1 sup A x y = A y. x =1 We conclude that A is bounded, and that A A. Finally, we must show that A is unique. Suppose that B B(K, H) also satisfied Ax, y = x, By for all x H and y K. Then for each fixed y we would have that x, By A y = 0 for every x, which implies By A y = 0. Hence B = A. Exercise 2.3 (Properties of the adjoint). (a) If A B(H, K) then (A ) = A. (b) If A, B B(H, K) and α, β F, then (αa + βb) = ᾱa + βb. (c) If A B(H 1, H 2 ) and B B(H 2, H 3 ), then (BA) = A B. (d) If A B(H) is invertible in B(H) (meaning that there exists A 1 B(H) such that AA 1 = A 1 A = I), then A is invertible in B(H) and (A 1 ) = (A ) 1. Remark 2.4. Later we will prove the Open Mapping Theorem. A remarkable consequence of this theorem is that if and Y are Banach spaces and A: Y is a bounded bijection, then A 1 : Y is automatically bounded. Proposition 2.5. If A B(H, K), then A = A = A A 1/2 = AA 1/2. Proof. In the course of proving Theorem 2.2, we already showed that A A. If f H, then Af 2 = Af, Af = A Af, f A Af f A Af f. (2.1) Hence Af A f (even if Af = 0, this is still true). Since this is true for all f we conclude that A A. Therefore A = A. Next, we have A A A A = A 2. But also, from the calculation in (2.1), we have Af 2 A Af f. Taking the supremum over all unit vectors, we obtain A 2 = sup Af 2 sup A Af f = A A. f =1 f =1

15 CHAPTER 2. OPERATORS ON HILBERT SPACES 15 Consequently A 2 = A A. The final equality follows by interchanging the roles of A and A. Exercise 2.6. Prove that if U B(H, K), then U is an isomorphism if and only if U is invertible and U 1 = U. Exercise 2.7. (a) Let λ = (λ n ) n N l (N) be given and let L be defined as in Example 1.7. Find L. (b)prove that the adjoint of the multiplication operator M φ defined in Exercise 1.18 is the multiplication operator M φ. Exercise 2.8. Let L and R be the left- and right-shift operators on l 2 (N), i.e., L(x 1, x 2,... ) = (x 2, x 3,... ) and R(x 1, x 2,... ) = (0, x 1, x 2,... ). Prove that L = R. Example 2.9. Let L be the integral operator defined in (1.3), determined by the kernel function k. Assume that k is chosen so that L: L 2 () L 2 () is bounded. The adjoint is the unique operator L : L 2 () L 2 () which satisfies Lf, g = f, L g, f, g L 2 (). To find L, let A: L 2 () L 2 () be the integral operator with kernel k(y, x), i.e., Af(x) = k(y, x) f(y) dµ(y). Then, given any f and g L 2 (), we have f, L g = Lf, g = Lf(x) g(x) dµ(x) = = = = f(y) f(y) = f, Ag. k(x, y) f(y) dµ(y) g(x)dµ(x) k(x, y) g(x) dµ(x) dµ(y) k(x, y) g(x) dµ(x) dµ(y) f(y) Ag(y) dµ(y) By uniqueness of the adjoint, we must have L = A. Exercise: Justify the interchange in the order of integration in the above calculation, i.e., provide hypotheses under which the calculations above are justified.

16 16 CHRISTOPHER HEIL Exercise Let {e n } n N be an orthonormal basis for a separable Hilbert space H. Define T : H l 2 (N) by T (f) = { f, e n } n N. Find a formula for T : l 2 (N) H. Definition Let A B(H). (a) We say that A is self-adjoint or Hermitian if A = A. (b) We say that A is normal if AA = A A. Example A real n n matrix A is self-adjoint if and only if it is symmetric, i.e., if A = A T. A complex n n matrix A is self-adjoint if and only if it is Hermitian, i.e., if A = A H. Exercise Show that every self-adjoint operator is normal. Show that every unitary operator is normal, but that a unitary operator need not be self-adjoint. For H = C n, find examples of matrices that are not normal. Are the left- and right-shift operators on l 2 (N) normal? Exercise (a) Show that if A, B B(H) are self-adjoint, then AB is self-adjoint if and only if AB = BA. (b) Give an example of self-adjoint operators A, B such that AB is not self-adjoint. (c) Show that if A, B B(H) are self-adjoint then A + A, AA, A A, A + B, ABA, and BAB are all self-adjoint. What about A A or A B? Show that AA A A is self-adjoint. Exercise (a) Let λ = (λ n ) n N l (N) be given and let L be defined as in Example 1.7. Show that L is normal, find a formula for L, and prove that L is self-adjoint if and only if each λ n is real. (b) Determine a necessary and sufficient condition on φ so that the multiplication operator M φ defined in Exercise 1.18 is self-adjoint. (c) Determine a necessary and sufficient condition on the kernel k so that the integral operator L defined in (1.23) is self-adjoint. The following result gives a useful condition for telling when an operator on a complex Hilbert space is self-adjoint. Proposition Let H be a complex Hilbert space (i.e., F = C), and let A B(H) be given. Then: A is self-adjoint Af, f R f H.

17 CHAPTER 2. OPERATORS ON HILBERT SPACES 17 Proof.. Assume A = A. Then for any f H we have Therefore Af, f is real. Af, f = f, Af = A f, f = Af, f.. Assume that Af, f is real for all f. Choose any f, g H. Then A(f + g), f + g = Af, f + Af, g + Ag, f + Ag, g. Since A(f + g), f + g, Af, f, and Ag, g are all real, we conclude that Af, g + Ag, f is real. Hence it equals its own complex conjugate, i.e., Similarly, since we see that Af, g + Ag, f = Af, g + Ag, f = g, Af + f, Ag. (2.2) A(f + ig), f + ig = Af, f i Af, g + i Ag, f + Ag, g i Af, g + i Ag, f = i Af, g + i Ag, f = i g, Af i f, Ag. Multiplying through by i yields Adding (2.2) and (2.3) together, we obtain Af, g Ag, f = g, Af + f, Ag. (2.3) 2 Af, g = 2 f, Ag = 2 A f, g. Since this is true for every f and g, we conclude that A = A. Example The preceding result is false for real Hilbert spaces. After all, if F = R then Af, f is real for every f no matter what A is. Therefore, any non-self-adjoint operator provides a counterexample. For example, if H = R n then any non-symmetric matrix A is a counterexample. The next result provides a useful way of calculating the operator norm of a self-adjoint operator. Proposition If A B(H) is self-adjoint, then A = sup Af, f. f =1 Proof. Set M = sup f =1 Af, f. By Cauchy Schwarz and the definition of operator norm, we have M = sup Af, f f =1 sup Af f f =1 sup A f f = A. f =1 To get the opposite inequality, note that if f is any nonzero vector in H then f/ f is a unit vector, so A f, f f f M. Rearranging, we see that f H, Af, f M f 2. (2.4)

18 18 CHRISTOPHER HEIL Now choose any f, g H with f = g = 1. Then, by expanding the inner products, canceling terms, and using the fact that A = A, we see that A(f + g), f + g A(f g), f g = 2 Af, g + 2 Ag, f = 2 Af, g + 2 g, Af = 4 Re Af, g. Therefore, applying (2.4) and the Parallelogram Law, we have 4 Re Af, g A(f + g), f + g + A(f g), f g M f + g 2 + M f g 2 = 2M ( f 2 + g 2) = 4M. That is, Re Af, g M for every choice of unit vectors f and g. Write Af, g = Af, g e iθ. Then e iθ g is another unit vector, so M Re Af, e iθ g = Re e iθ Af, g = Af, g. Hence Af = sup Af, g M. g =1 Since this is true for every unit vector f, we conclude that A M. The following corollary is a very useful consequence. Corollary Assume that A B(H). (a) If F = R, A = A, and Af, f = 0 for every f, then A = 0. (b) If F = C and Af, f = 0 for every f, then A = 0. Proof. Assume the hypotheses of either statement (a) or statement (b). In the case of statement (a), we have by hypothesis that A is self-adjoint. In the case of statement (b), we can conclude that A is self-adjoint because Af, f = 0 is real for every f. Hence in either case we can apply Proposition 2.18 to conclude that A = sup Af, f = 0. f =1 Lemma If A B(H), then the following statements are equivalent. (a) A is normal, i.e., AA = A A. (b) Af = A f for every f H.

19 CHAPTER 2. OPERATORS ON HILBERT SPACES 19 Proof. (b) (a). Assume that (b) holds. Then for every f we have (A A AA )f, f = A Af, f AA f, f = Af, Af A f, A f = Af 2 A f 2 = 0. Since A A AA is self-adjoint, it follows from Corollary 2.19 that A A AA = 0. (a) (b). Exercise. Corollary If A B(H) is normal, then ker(a) = ker(a ). Exercise Suppose that A B(H) is normal. Prove that A is injective if and only if range(a) is dense in H. Exercise If A B(H), then the following statements are equivalent. (a) A is an isometry, i.e., Af = f for every f H. (b) A A = I. (c) Af, Ag = f, g for every f, g H. Exercise If H = C n and A, B are n n matrices, then AB = I implies BA = I. Give a counterexample to this for an infinite-dimensional Hilbert space. Consequently, the hypothesis A A = I in the preceding result does not imply that AA = I. Exercise If A B(H), then the following statements are equivalent. (a) A A = AA = I. (b) A is unitary, i.e., it is a surjective isometry. (c) A is a normal isometry. The following result provides a very useful relationship between the range of A and the kernel of A. Theorem Let A B(H, K). (a) ker(a) = range(a ). (b) ker(a) = range(a ). (c) A is injective if and only if range(a ) is dense in H.

20 20 CHRISTOPHER HEIL Proof. (a) Assume that f ker(a) and let h range(a ), i.e., h = A g for some g K. Then since Af = 0, we have f, h = f, A g = Af, g = 0. Thus f range(a ), so ker(a) range(a ). Now assume that f range(a ). Then for any h H we have Af, h = f, A h = 0. But this implies Af = 0, so f ker(a). Thus range(a ) ker(a). (b), (c) Exercises. 3. Projections and Idempotents: Invariant and Reducing Subspaces Definition 3.1. a. If E B(H) satisfies E 2 = E then E is said to be idempotent. b. If E B(H) satisfies E 2 = E and ker(e) = range(e) then E is called a projection. Exercise 3.2. If E B(H) is an idempotent operator, then ker(e) and range(e) are closed subspaces of H. Further, ker(e) = range(i E) and range(e) = ker(i E). Lemma 3.3 (Characterization of Orthogonal Projections). Let E B(H) be a nonzero idempotent operator. Then the following statements are equivalent. (a) E is a projection. (b) E is the orthogonal projection of H onto range(e). (c) E = 1. (d) E is self-adjoint. (e) E is normal. (f) E is positive, i.e., Ef, f 0 for every f H. Proof. (e) (a). Assume that E 2 = E and E is normal. Then from Lemma 2.20 we know that Ef = E f for every f H. Hence Ef = 0 if and only if E f = 0, or in other words, ker(e) = ker(e ). But we know from Theorem 2.26 that ker(e ) = range(e). Hence we conclude that ker(e) = range(e), and therefore E is a projection. The remaining implications are exercises. Definition 3.4 (Orthogonal Direct Sum of Subspaces). Let {M i } i I be a collection of closed subspaces of H such that M i M j whenever i j. Then the orthogonal direct sum of the M i is the smallest closed subspace which contains every M i. This space is ( = span M i ). M i i I i I

21 CHAPTER 2. OPERATORS ON HILBERT SPACES 21 Exercise 3.5. Suppose that M, N are closed subspaces of H such that M N. Prove that M + N = {m + n : m M, n N} is a closed subspace of H, and that M N = M + N. Show that every vector x M N can be written uniquely as x = m + n with m M and n N. Extend by induction to finite collections of closed, pairwise orthogonal subspaces. (Unfortunately, the analogous statement is not true for infinite collections.) Exercise 3.6. Show that if A B(H, K) then H = ker(a) range(a ). Definition 3.7. Let A B(H) and M H. (a) We say that M is invariant under A if A(M) M, where A(M) = {Ax : x M}. That is, M is invariant if x M implies Ax M. Note that it need not be the case that A(M) = M. (b) We say that M is a reducing subspace for A if both M and M are invariant under A, i.e., A(M) M and A(M ) M. Proposition 3.8. Let A B(H) and M H be given. Then the following statements are equivalent. (a) M is invariant under A. (b) P AP = AP, where P = P M is the orthogonal projection of H onto M. Exercise 3.9. Define L: l 2 (Z) l 2 (Z) by L(..., x 1, x 0, x 1,... ) = (...,, x 0, x 1, x 2,... ), where on the right-hand side the entry x 1 sits in the 0th component position. That is, L slides each component one unit to the left (L is called a bilateral shift). Find a closed subspace of l 2 (Z) that is invariant but not reducing under L. Exercise Assume that M H is invariant under L B(H). invariant under L. Prove that M is

22 22 CHRISTOPHER HEIL 4. Compact Operators Definition 4.1 (Compact and Totally Bounded Sets). Let be a Banach space, and let E be given. (a) We say that E is compact if every open cover of E contains a finite subcover. That is, E is compact if whenever {U α } α I is a collection of open sets whose union contains E, then there exist finitely many α 1,..., α N such that E U α1 U αn. (b) We say that E is sequentially compact if every sequence {f n } n N of points of E contains a convergent subsequence {f nk } k N whose limit belongs to E. (c) We say that E is totally bounded if for every ε > 0 there exist finitely many points f 1,..., f N E such that E N B(f k, ε), k=1 where B(f k, ε) is the open ball of radius ε centered at f k. That is, E is totally bounded if and only there exist finitely many points f 1,..., f N E such that every element of E is within ε of some f k. In finite dimensions, a set is compact if and only if it is closed and bounded. In infinite dimensions, all compact sets are closed and bounded, but the converse fails. Instead, we have the following characterization of compact sets. (this characterization actually holds in any complete metric space). Theorem 4.2. Let E be a subset of a Banach space. Then the following statements are equivalent. (a) E is compact. (b) E is sequentially compact. (c) E is closed and totally bounded. Proof. (b) (a). 2 Assume that E is sequentially compact. Our first step will be to prove the following claim, where the diameter of a set S is defined to be diam(s) = sup{ f g : f, g S}. Claim 1. For any open cover {U α } α I of E, there exists a number δ > 0 (called a Lebesgue number for the cover) such that if S E satisfies diam(s) < δ, then there is an α I such that S U α. To prove the claim, suppose that {U α } α I was an open cover of E such that no δ with the required property existed. Then for each n N, we could find a set S n E with diam(s n ) < 1 n such that S n is not contained in any U α. Choose any f n S n. Since E is sequentially compact, there must be a subsequence {f nk } k N that converges to an element of 2 This proof is adapted from one given in J. R. Munkres, Topology, Second Edition, Prentice Hall, 2000.

23 CHAPTER 2. OPERATORS ON HILBERT SPACES 23 E, say f nk a E. But we must have a U α for some α, and since U α is open there must exist some ε > 0 such that B(a, ε) U α. Now choose k large enough that we have both 1 < ε and a f nk < ε n k 2 2. The first inequality above implies that diam(s nk ) < ε. Therefore, using this and second 2 inequality, we have S nk B(a, ε) U α, which is a contradiction. Therefore the claim is proved. Next, we will prove the following claim. Claim 2. For any ε > 0, there exist finitely many f 1,..., f N E such that E N k=1 B(f k, ε). To prove this claim, assume that there is an ε > 0 such that E cannot be covered by finitely many ε-balls centered at points of E. Choose any f 1 E. Since E cannot be covered by a single ε-ball, we have E B(f 1, ε). Hence there exists f 2 E \ B(f 1, ε), i.e., f 2 E and f 2 f 1 ε. But E cannot be covered by two ε-balls, so there must exist an f 3 E \ ( B(f 1, ε) B(f 2, ε) ). In particular, we have f 3 f 1, f 3 f 2 ε. Continuing in this way we obtain a sequence of points {f n } n N in E which has no convergent subsequence, which is a contradiction. Hence the claim is proved. Finally, we show that E is compact. Let {U α } α I be any open cover of E. Let δ be the Lebesgue number given by Claim 1, and set ε = δ. By Claim 2, there exists a covering of E 3 by finitely many ε-balls. Each ball has diameter smaller than δ, so by Claim 1 is contained in some U α. Thus we find finitely many U α that cover E. (c) (b). Assume that E is closed and totally bounded, and let {f n } n N be any sequence of points in E. Since E is covered by finitely many balls of radius 1, one of those balls must 2 contain infinitely many f n, say {f n (1) } n N. Then we have m, n N, f (1) m f (1) n < 1. Since E is covered by finitely many balls of radius 1 4 {f n (1) } n N such that m, n N, f (1) m f (1) n < 1 2. By induction we keep constructing subsequences {f n (k) all m, n N. Now consider the diagonal subsequence {f (n) n that 1 N f (m) m < ε. If m n > N, then f (m) m = f (n) k. Then f (m) m f (n) n = f (n) (2), we can find a subsequence {f n } n N of } n N such that f (k) m f n (k) < 1 for k } n N. Given ε > 0, let N be large enough is one element of the sequence {f (n) k } k N, say k f (n) n < 1 n < ε. Thus {f (n) n } n N is Cauchy and hence converges. Since E is closed, it must converge to some element of E.

24 24 CHRISTOPHER HEIL (a) (c). Exercise. Exercise 4.3. Show that if E is a totally bounded subset of a Banach space, then its closure E is compact. A set whose closure is compact is said to be precompact. Notation 4.4. We let Ball H denote the closed unit sphere in H, i.e., Ball H = Ball(H) = {f H : f 1}. Exercise 4.5. Prove that if H is infinite-dimensional, then Ball H is not compact. Definition 4.6 (Compact Operators). Let H, K be Hilbert spaces. T : H K is compact if T (Ball H ) has compact closure in K. We define B 0 (H, K) = {T : H K : T is compact}, and set B 0 (H) = B 0 (H, H). A linear operator By definition, a compact operator is linear, and we will see that all compact operators are bounded. Thus it will turn out that B 0 (H, K) B(H, K). In fact, we will see that B 0 (H, K) is a closed subspace of B(H, K). The following result gives some useful reformulations of the definition of compact operator. Proposition 4.7 (Characterizations of Compact Operators). Let T : H K be linear. Then the following statements are equivalent. (a) T is compact. (b) T (Ball H ) is totally bounded. (c) If {f n } n N is a bounded sequence in H, then {T f n } n N contains a convergent subsequence. Proof. (a) (b). This follows from Theorem 4.2 and Exercise 4.3. (a) (c). Suppose that T is compact and that {f n } n N is a bounded sequence in H. By rescaling the sequence (i.e., multiplying by an appropriate scalar), we may assume that f n Ball H for every n. Therefore T f n T (Ball H ) T (Ball H ). Since T (Ball H ) is compact, it follows from Theorem 4.2 that {T f n } n N contains a subsequence which converges to an element of T (Ball H ). (c) (a). Exercise. Proposition 4.8. If T : H K is compact, then it is bounded. That is, B 0 (H, K) B(H, K). Proof. Assume that T : H K is linear but unbounded. Then there exist vectors f n H such that f n = 1 but T f n n. Therefore every subsequence of {T f n } n N is unbounded, and hence cannot converge. Therefore T is not compact by Proposition 4.7.

25 CHAPTER 2. OPERATORS ON HILBERT SPACES 25 Exercise 4.9. Show that if H is infinite-dimensional then the identity operator on H is not compact. Hence a bounded operator need be compact in general. The following exercise shows that a compact operator maps an orthonormal sequence to a sequence that converges to the zero vector. Exercise (a) Let {h n } n N be a sequence of vectors in H, and let h H. Suppose that every subsequence of {h n } n N contains a subsequence that converges to h. Prove that h n h. Hint: Proceed by contradiction. Suppose that h n does not converge to h. Show that this implies that there is an ε > 0 and a subsequence {h nk } k N such that h h nk ε for every k. (b) Suppose that T : H K is compact, and let {e n } n N be an orthonormal sequence in H. Show that T e n 0. Hint: Choose any subsequence {f n } n N. Since T is compact, this sequence has a subsequence {g n } n N such that {T g n } n N converges, say T g n h. Prove that T g n, h 0 (use Bessel s Inequality to find a bound for the l 2 -norm of { T g n, h } n N ). Use part (a) to complete the proof. The following exercise shows that a compact operator maps weakly convergent sequences to convergent sequences. Definition Let {f n } n N be a sequence of vectors in H and let f H. We say that f n converges weakly to f, written f n w f, if g H, f n, g f, g as n. Exercise (a) Show that if f n f, then f n w f. (b) Show that if {e n } n N is an orthonormal sequence in H, then e n w 0. (c) Suppose that T B(H) is compact. Show that if f n w f, then T f n T f. Exercise Let φ L (R n ) be fixed, with φ 0. Then by Exercise 1.18 we know that the multiplication operator M φ : L 2 (R n ) L 2 (R n ) given by M φ f = fφ is bounded. Show that M φ is not compact. Hint: There must exist an ε > 0 and a set E R n with positive measure such that φ(x) ε for all x E. Exhibit a measure space (, Ω, µ) and a bounded, nonzero φ L () such that M φ is compact. Hint: Consider Exercise Exercise Porve that if T : H K is compact and injective, then T 1 : range(t ) H is unbounded.

26 26 CHRISTOPHER HEIL Theorem 4.15 (Limits of Compact Operators). B 0 (H, K) is a closed subspace of B(H, K) (under the operator norm). That is, (a) if S, T B 0 (H, K) and α, β F, then αs + βt B 0 (H, K), (b) if T n B 0 (H, K), T B(H, K), and T T n 0, then T B 0 (H, K). Proof. (a) Exercise. (b) Assume that T n are compact operators and that T n T in operator norm. By Proposition 4.7, it suffices to show that T (Ball H ) is a totally bounded subset of K. Choose any ε > 0. Then there exists an n such that T T n < ε. Now, T 3 n is compact, so T n (Ball H ) is totally bounded. Hence there exist finitely many points h 1,..., h m Ball H such that T n (Ball H ) We will show that T (Ball H ) is totally bounded by showing that T (Ball H ) m j=1 m j=1 B ( T n h j, ε 3). (4.1) B ( T n h j, ε ). (4.2) Choose any element of T (Ball H ), i.e., any point T f with f 1. Then T n f T n (Ball H ), so by (4.1) there must be some j such that T n f T n h j < ε 3. Consequently, T f T h j T f T n f + T n f T n h j + T n h j T h j < T T n f + ε 3 + T n T h j < ε ε 3 + ε 3 1 = ε. Hence (4.2) follows, so T is compact. Exercise Another way to prove Theorem 4.15 is to apply a Cantor diagonalization argument. Fill in the details in the following sketch of this argument. Suppose that {f n } n N is a bounded sequence in H. Then since T 1 is compact, there exists a subsequence {f n (1) } n N of {f n } n N such that {T 1 f n (1) } n N converges. Then since T 2 is compact, there exists a subsequence {f n (2) } n N of {f n (1) } n N such that {T 2 f n (2) } n N converges (and note that {T 1 f n (2) } n N also converges!). Continue to construct subsequences in this way, and then show that the diagonal subsequence {T f n (n) } n N converges (use the fact that there exists a k such that T T k < ε). Therefore T is compact. Theorem 4.17 (Compositions and Compact Operators). Let H 1, H 2, H 3 be Hilbert spaces. (a) If A: H 1 H 2 is bounded and T : H 2 H 3 is compact, then T A: H 1 H 3 is compact.

27 CHAPTER 2. OPERATORS ON HILBERT SPACES 27 (b) If T : H 1 H 2 is compact and A: H 2 H 3 is bounded, then AT : H 1 H 3 is compact. Proof. (b) Assume that A is bounded and T is compact. Let {f n } n N be any bounded sequence in H 1. Then since T is compact, there is a subsequence {T f nk } k N that converges in H 2. Since A is bounded, the subsequence {AT f nk } k N therefore converges in H 3. Hence AT is compact. (a) Exercise. Exercise Prove that if T B 0 (H, K), then range(t ) is a separable subspace of K. Hints: Since T (Ball H ) is compact, it is totally bounded. Hence for each n N we can find finitely many balls of radius 1/n with centers in T (Ball H ) that cover T (Ball H ). If we consider all these balls for every n, we have countably many balls that cover T (Ball H ). Show that this implies that T (Ball H ) contains a countable, dense subset. Then do the same for each ball of radius k N instead of just k = 1. Combine all of these together to get a countable dense subset of range(t ). Definition 4.19 (Finite-Rank Operators). Recall that the rank of an operator T : H K is the dimension of range(t ). We say that T is a finite-rank operator if range(t ) is finitedimensional. We set and set B 00 (H) = B 00 (H, H). B 00 (H, K) = {T B(H, K) : T is finite-rank}, A linear, finite-rank operator need not be bounded (that is why we include the assumption of boundedness in the definition of B 00 (H, K) above). However, the following result shows that if a finite-rank operator is bounded, then it is actually compact. Proposition If T : H K is bounded, linear, and has finite rank, then T is compact. Thus, B 00 (H, K) B 0 (H, K). Proof. Since T is bounded, T (Ball H ) is a bounded subset of the finite-dimensional space range(t ). All finite-dimensional spaces are closed. Hence the closure of T (Ball H ) is a closed and bounded subset of range(t ), and therefore is compact. This gives us the following very useful way to show that a general operator T is compact: try to construct a sequence of finite-rank operators T n that converge to T in operator norm. Corollary Suppose that T n B(H, K) are finite-rank operators, T B(H, K), and T n T in operator norm. Then T is compact. Exercise Show that if E B(H) is compact and idempotent, then E has finite rank.

28 28 CHRISTOPHER HEIL Example Let {e n } n N be an orthonormal basis for a separable Hilbert space H, and let λ = (λ n ) n N be a bounded sequence of scalars. Then we know from Example 1.7 that Lf = λ n f, e n e n defines a bounded operator on H. Suppose that λ n 0 as n. Define L N f = n=1 N λ n f, e n e n. n=1 Since range(l N ) span{e 1,..., e N } (must it be equality?), we have that L N is finite-rank. (Exercise: Show that L is not finite-rank if there are infinitely many λ n 0.) Further, L N is a good approximation to L, because (using the Plancherel Theorem) we have 2 (L L N )f 2 = λ n f, e n e n = n=n+1 n=n+1 It follows that L N converges to L in operator norm: ( ) lim L L N 2 lim λ n 2 N N λ n 2 f, e n 2 ( ) sup λ n 2 f, e n 2 n>n n=n+1 ( ) sup λ n 2 f 2. n>n sup n>n = lim sup λ n 2 = 0. N Since each L N is compact, we conclude that L is compact as well. Exercise Continuing the preceding example, prove the following. (a) Prove that if λ n does not converge to zero then L is not compact. Hint: We know at least some of the eigenvectors of L. (b) Prove that, with only the assumption that λ l, we have f H, L N f Lf. (4.3) That is, for each individual vector f we have Lf L N f 0, where this is the norm in H. A sequence of operators which satisfies (4.3) is said to converge strongly or in the strong operator topology (SOT). Prove that strong convergence of operators does not imply convergence in operator norm, i.e., (4.3) does not imply that L L N 0. (c) Assuming that λ l, prove that L is self-adjoint if and only if every λ n is real.

BANACH AND HILBERT SPACE REVIEW

BANACH AND HILBERT SPACE REVIEW BANACH AND HILBET SPACE EVIEW CHISTOPHE HEIL These notes will briefly review some basic concepts related to the theory of Banach and Hilbert spaces. We are not trying to give a complete development, but

More information

FUNCTIONAL ANALYSIS LECTURE NOTES: QUOTIENT SPACES

FUNCTIONAL ANALYSIS LECTURE NOTES: QUOTIENT SPACES FUNCTIONAL ANALYSIS LECTURE NOTES: QUOTIENT SPACES CHRISTOPHER HEIL 1. Cosets and the Quotient Space Any vector space is an abelian group under the operation of vector addition. So, if you are have studied

More information

and s n (x) f(x) for all x and s.t. s n is measurable if f is. REAL ANALYSIS Measures. A (positive) measure on a measurable space

and s n (x) f(x) for all x and s.t. s n is measurable if f is. REAL ANALYSIS Measures. A (positive) measure on a measurable space RAL ANALYSIS A survey of MA 641-643, UAB 1999-2000 M. Griesemer Throughout these notes m denotes Lebesgue measure. 1. Abstract Integration σ-algebras. A σ-algebra in X is a non-empty collection of subsets

More information

Notes on metric spaces

Notes on metric spaces Notes on metric spaces 1 Introduction The purpose of these notes is to quickly review some of the basic concepts from Real Analysis, Metric Spaces and some related results that will be used in this course.

More information

Metric Spaces. Chapter 7. 7.1. Metrics

Metric Spaces. Chapter 7. 7.1. Metrics Chapter 7 Metric Spaces A metric space is a set X that has a notion of the distance d(x, y) between every pair of points x, y X. The purpose of this chapter is to introduce metric spaces and give some

More information

Section 6.1 - Inner Products and Norms

Section 6.1 - Inner Products and Norms Section 6.1 - Inner Products and Norms Definition. Let V be a vector space over F {R, C}. An inner product on V is a function that assigns, to every ordered pair of vectors x and y in V, a scalar in F,

More information

Finite dimensional C -algebras

Finite dimensional C -algebras Finite dimensional C -algebras S. Sundar September 14, 2012 Throughout H, K stand for finite dimensional Hilbert spaces. 1 Spectral theorem for self-adjoint opertors Let A B(H) and let {ξ 1, ξ 2,, ξ n

More information

MEASURE AND INTEGRATION. Dietmar A. Salamon ETH Zürich

MEASURE AND INTEGRATION. Dietmar A. Salamon ETH Zürich MEASURE AND INTEGRATION Dietmar A. Salamon ETH Zürich 12 May 2016 ii Preface This book is based on notes for the lecture course Measure and Integration held at ETH Zürich in the spring semester 2014. Prerequisites

More information

MATH 4330/5330, Fourier Analysis Section 11, The Discrete Fourier Transform

MATH 4330/5330, Fourier Analysis Section 11, The Discrete Fourier Transform MATH 433/533, Fourier Analysis Section 11, The Discrete Fourier Transform Now, instead of considering functions defined on a continuous domain, like the interval [, 1) or the whole real line R, we wish

More information

Chapter 5. Banach Spaces

Chapter 5. Banach Spaces 9 Chapter 5 Banach Spaces Many linear equations may be formulated in terms of a suitable linear operator acting on a Banach space. In this chapter, we study Banach spaces and linear operators acting on

More information

SOLUTIONS TO EXERCISES FOR. MATHEMATICS 205A Part 3. Spaces with special properties

SOLUTIONS TO EXERCISES FOR. MATHEMATICS 205A Part 3. Spaces with special properties SOLUTIONS TO EXERCISES FOR MATHEMATICS 205A Part 3 Fall 2008 III. Spaces with special properties III.1 : Compact spaces I Problems from Munkres, 26, pp. 170 172 3. Show that a finite union of compact subspaces

More information

Mathematical Methods of Engineering Analysis

Mathematical Methods of Engineering Analysis Mathematical Methods of Engineering Analysis Erhan Çinlar Robert J. Vanderbei February 2, 2000 Contents Sets and Functions 1 1 Sets................................... 1 Subsets.............................

More information

Mathematics Course 111: Algebra I Part IV: Vector Spaces

Mathematics Course 111: Algebra I Part IV: Vector Spaces Mathematics Course 111: Algebra I Part IV: Vector Spaces D. R. Wilkins Academic Year 1996-7 9 Vector Spaces A vector space over some field K is an algebraic structure consisting of a set V on which are

More information

Matrix Representations of Linear Transformations and Changes of Coordinates

Matrix Representations of Linear Transformations and Changes of Coordinates Matrix Representations of Linear Transformations and Changes of Coordinates 01 Subspaces and Bases 011 Definitions A subspace V of R n is a subset of R n that contains the zero element and is closed under

More information

Inner Product Spaces

Inner Product Spaces Math 571 Inner Product Spaces 1. Preliminaries An inner product space is a vector space V along with a function, called an inner product which associates each pair of vectors u, v with a scalar u, v, and

More information

Similarity and Diagonalization. Similar Matrices

Similarity and Diagonalization. Similar Matrices MATH022 Linear Algebra Brief lecture notes 48 Similarity and Diagonalization Similar Matrices Let A and B be n n matrices. We say that A is similar to B if there is an invertible n n matrix P such that

More information

Metric Spaces Joseph Muscat 2003 (Last revised May 2009)

Metric Spaces Joseph Muscat 2003 (Last revised May 2009) 1 Distance J Muscat 1 Metric Spaces Joseph Muscat 2003 (Last revised May 2009) (A revised and expanded version of these notes are now published by Springer.) 1 Distance A metric space can be thought of

More information

IRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL. 1. Introduction

IRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL. 1. Introduction IRREDUCIBLE OPERATOR SEMIGROUPS SUCH THAT AB AND BA ARE PROPORTIONAL R. DRNOVŠEK, T. KOŠIR Dedicated to Prof. Heydar Radjavi on the occasion of his seventieth birthday. Abstract. Let S be an irreducible

More information

MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS

MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS Systems of Equations and Matrices Representation of a linear system The general system of m equations in n unknowns can be written a x + a 2 x 2 + + a n x n b a

More information

1 Norms and Vector Spaces

1 Norms and Vector Spaces 008.10.07.01 1 Norms and Vector Spaces Suppose we have a complex vector space V. A norm is a function f : V R which satisfies (i) f(x) 0 for all x V (ii) f(x + y) f(x) + f(y) for all x,y V (iii) f(λx)

More information

T ( a i x i ) = a i T (x i ).

T ( a i x i ) = a i T (x i ). Chapter 2 Defn 1. (p. 65) Let V and W be vector spaces (over F ). We call a function T : V W a linear transformation form V to W if, for all x, y V and c F, we have (a) T (x + y) = T (x) + T (y) and (b)

More information

1 if 1 x 0 1 if 0 x 1

1 if 1 x 0 1 if 0 x 1 Chapter 3 Continuity In this chapter we begin by defining the fundamental notion of continuity for real valued functions of a single real variable. When trying to decide whether a given function is or

More information

1. Let P be the space of all polynomials (of one real variable and with real coefficients) with the norm

1. Let P be the space of all polynomials (of one real variable and with real coefficients) with the norm Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 005-06-15 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

More information

MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS. + + x 2. x n. a 11 a 12 a 1n b 1 a 21 a 22 a 2n b 2 a 31 a 32 a 3n b 3. a m1 a m2 a mn b m

MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS. + + x 2. x n. a 11 a 12 a 1n b 1 a 21 a 22 a 2n b 2 a 31 a 32 a 3n b 3. a m1 a m2 a mn b m MATRIX ALGEBRA AND SYSTEMS OF EQUATIONS 1. SYSTEMS OF EQUATIONS AND MATRICES 1.1. Representation of a linear system. The general system of m equations in n unknowns can be written a 11 x 1 + a 12 x 2 +

More information

1. Prove that the empty set is a subset of every set.

1. Prove that the empty set is a subset of every set. 1. Prove that the empty set is a subset of every set. Basic Topology Written by Men-Gen Tsai email: b89902089@ntu.edu.tw Proof: For any element x of the empty set, x is also an element of every set since

More information

NOTES ON LINEAR TRANSFORMATIONS

NOTES ON LINEAR TRANSFORMATIONS NOTES ON LINEAR TRANSFORMATIONS Definition 1. Let V and W be vector spaces. A function T : V W is a linear transformation from V to W if the following two properties hold. i T v + v = T v + T v for all

More information

Inner product. Definition of inner product

Inner product. Definition of inner product Math 20F Linear Algebra Lecture 25 1 Inner product Review: Definition of inner product. Slide 1 Norm and distance. Orthogonal vectors. Orthogonal complement. Orthogonal basis. Definition of inner product

More information

MA106 Linear Algebra lecture notes

MA106 Linear Algebra lecture notes MA106 Linear Algebra lecture notes Lecturers: Martin Bright and Daan Krammer Warwick, January 2011 Contents 1 Number systems and fields 3 1.1 Axioms for number systems......................... 3 2 Vector

More information

Linear Maps. Isaiah Lankham, Bruno Nachtergaele, Anne Schilling (February 5, 2007)

Linear Maps. Isaiah Lankham, Bruno Nachtergaele, Anne Schilling (February 5, 2007) MAT067 University of California, Davis Winter 2007 Linear Maps Isaiah Lankham, Bruno Nachtergaele, Anne Schilling (February 5, 2007) As we have discussed in the lecture on What is Linear Algebra? one of

More information

Vector and Matrix Norms

Vector and Matrix Norms Chapter 1 Vector and Matrix Norms 11 Vector Spaces Let F be a field (such as the real numbers, R, or complex numbers, C) with elements called scalars A Vector Space, V, over the field F is a non-empty

More information

LINEAR ALGEBRA W W L CHEN

LINEAR ALGEBRA W W L CHEN LINEAR ALGEBRA W W L CHEN c W W L Chen, 1997, 2008 This chapter is available free to all individuals, on understanding that it is not to be used for financial gain, and may be downloaded and/or photocopied,

More information

Linear Algebra I. Ronald van Luijk, 2012

Linear Algebra I. Ronald van Luijk, 2012 Linear Algebra I Ronald van Luijk, 2012 With many parts from Linear Algebra I by Michael Stoll, 2007 Contents 1. Vector spaces 3 1.1. Examples 3 1.2. Fields 4 1.3. The field of complex numbers. 6 1.4.

More information

Chapter 20. Vector Spaces and Bases

Chapter 20. Vector Spaces and Bases Chapter 20. Vector Spaces and Bases In this course, we have proceeded step-by-step through low-dimensional Linear Algebra. We have looked at lines, planes, hyperplanes, and have seen that there is no limit

More information

Undergraduate Notes in Mathematics. Arkansas Tech University Department of Mathematics

Undergraduate Notes in Mathematics. Arkansas Tech University Department of Mathematics Undergraduate Notes in Mathematics Arkansas Tech University Department of Mathematics An Introductory Single Variable Real Analysis: A Learning Approach through Problem Solving Marcel B. Finan c All Rights

More information

1 VECTOR SPACES AND SUBSPACES

1 VECTOR SPACES AND SUBSPACES 1 VECTOR SPACES AND SUBSPACES What is a vector? Many are familiar with the concept of a vector as: Something which has magnitude and direction. an ordered pair or triple. a description for quantities such

More information

Orthogonal Diagonalization of Symmetric Matrices

Orthogonal Diagonalization of Symmetric Matrices MATH10212 Linear Algebra Brief lecture notes 57 Gram Schmidt Process enables us to find an orthogonal basis of a subspace. Let u 1,..., u k be a basis of a subspace V of R n. We begin the process of finding

More information

Section 4.4 Inner Product Spaces

Section 4.4 Inner Product Spaces Section 4.4 Inner Product Spaces In our discussion of vector spaces the specific nature of F as a field, other than the fact that it is a field, has played virtually no role. In this section we no longer

More information

0 <β 1 let u(x) u(y) kuk u := sup u(x) and [u] β := sup

0 <β 1 let u(x) u(y) kuk u := sup u(x) and [u] β := sup 456 BRUCE K. DRIVER 24. Hölder Spaces Notation 24.1. Let Ω be an open subset of R d,bc(ω) and BC( Ω) be the bounded continuous functions on Ω and Ω respectively. By identifying f BC( Ω) with f Ω BC(Ω),

More information

Inner Product Spaces and Orthogonality

Inner Product Spaces and Orthogonality Inner Product Spaces and Orthogonality week 3-4 Fall 2006 Dot product of R n The inner product or dot product of R n is a function, defined by u, v a b + a 2 b 2 + + a n b n for u a, a 2,, a n T, v b,

More information

Metric Spaces. Chapter 1

Metric Spaces. Chapter 1 Chapter 1 Metric Spaces Many of the arguments you have seen in several variable calculus are almost identical to the corresponding arguments in one variable calculus, especially arguments concerning convergence

More information

GROUPS ACTING ON A SET

GROUPS ACTING ON A SET GROUPS ACTING ON A SET MATH 435 SPRING 2012 NOTES FROM FEBRUARY 27TH, 2012 1. Left group actions Definition 1.1. Suppose that G is a group and S is a set. A left (group) action of G on S is a rule for

More information

Linear Algebra Notes for Marsden and Tromba Vector Calculus

Linear Algebra Notes for Marsden and Tromba Vector Calculus Linear Algebra Notes for Marsden and Tromba Vector Calculus n-dimensional Euclidean Space and Matrices Definition of n space As was learned in Math b, a point in Euclidean three space can be thought of

More information

Linear Algebra Review. Vectors

Linear Algebra Review. Vectors Linear Algebra Review By Tim K. Marks UCSD Borrows heavily from: Jana Kosecka kosecka@cs.gmu.edu http://cs.gmu.edu/~kosecka/cs682.html Virginia de Sa Cogsci 8F Linear Algebra review UCSD Vectors The length

More information

Finite Dimensional Hilbert Spaces and Linear Inverse Problems

Finite Dimensional Hilbert Spaces and Linear Inverse Problems Finite Dimensional Hilbert Spaces and Linear Inverse Problems ECE 174 Lecture Supplement Spring 2009 Ken Kreutz-Delgado Electrical and Computer Engineering Jacobs School of Engineering University of California,

More information

I. GROUPS: BASIC DEFINITIONS AND EXAMPLES

I. GROUPS: BASIC DEFINITIONS AND EXAMPLES I GROUPS: BASIC DEFINITIONS AND EXAMPLES Definition 1: An operation on a set G is a function : G G G Definition 2: A group is a set G which is equipped with an operation and a special element e G, called

More information

3. INNER PRODUCT SPACES

3. INNER PRODUCT SPACES . INNER PRODUCT SPACES.. Definition So far we have studied abstract vector spaces. These are a generalisation of the geometric spaces R and R. But these have more structure than just that of a vector space.

More information

Continued Fractions and the Euclidean Algorithm

Continued Fractions and the Euclidean Algorithm Continued Fractions and the Euclidean Algorithm Lecture notes prepared for MATH 326, Spring 997 Department of Mathematics and Statistics University at Albany William F Hammond Table of Contents Introduction

More information

Let H and J be as in the above lemma. The result of the lemma shows that the integral

Let H and J be as in the above lemma. The result of the lemma shows that the integral Let and be as in the above lemma. The result of the lemma shows that the integral ( f(x, y)dy) dx is well defined; we denote it by f(x, y)dydx. By symmetry, also the integral ( f(x, y)dx) dy is well defined;

More information

Notes on Symmetric Matrices

Notes on Symmetric Matrices CPSC 536N: Randomized Algorithms 2011-12 Term 2 Notes on Symmetric Matrices Prof. Nick Harvey University of British Columbia 1 Symmetric Matrices We review some basic results concerning symmetric matrices.

More information

Lecture 1: Schur s Unitary Triangularization Theorem

Lecture 1: Schur s Unitary Triangularization Theorem Lecture 1: Schur s Unitary Triangularization Theorem This lecture introduces the notion of unitary equivalence and presents Schur s theorem and some of its consequences It roughly corresponds to Sections

More information

Lectures notes on orthogonal matrices (with exercises) 92.222 - Linear Algebra II - Spring 2004 by D. Klain

Lectures notes on orthogonal matrices (with exercises) 92.222 - Linear Algebra II - Spring 2004 by D. Klain Lectures notes on orthogonal matrices (with exercises) 92.222 - Linear Algebra II - Spring 2004 by D. Klain 1. Orthogonal matrices and orthonormal sets An n n real-valued matrix A is said to be an orthogonal

More information

Introduction to Topology

Introduction to Topology Introduction to Topology Tomoo Matsumura November 30, 2010 Contents 1 Topological spaces 3 1.1 Basis of a Topology......................................... 3 1.2 Comparing Topologies.......................................

More information

16.3 Fredholm Operators

16.3 Fredholm Operators Lectures 16 and 17 16.3 Fredholm Operators A nice way to think about compact operators is to show that set of compact operators is the closure of the set of finite rank operator in operator norm. In this

More information

Lecture Notes on Measure Theory and Functional Analysis

Lecture Notes on Measure Theory and Functional Analysis Lecture Notes on Measure Theory and Functional Analysis P. Cannarsa & T. D Aprile Dipartimento di Matematica Università di Roma Tor Vergata cannarsa@mat.uniroma2.it daprile@mat.uniroma2.it aa 2006/07 Contents

More information

Chapter 17. Orthogonal Matrices and Symmetries of Space

Chapter 17. Orthogonal Matrices and Symmetries of Space Chapter 17. Orthogonal Matrices and Symmetries of Space Take a random matrix, say 1 3 A = 4 5 6, 7 8 9 and compare the lengths of e 1 and Ae 1. The vector e 1 has length 1, while Ae 1 = (1, 4, 7) has length

More information

Inner products on R n, and more

Inner products on R n, and more Inner products on R n, and more Peyam Ryan Tabrizian Friday, April 12th, 2013 1 Introduction You might be wondering: Are there inner products on R n that are not the usual dot product x y = x 1 y 1 + +

More information

No: 10 04. Bilkent University. Monotonic Extension. Farhad Husseinov. Discussion Papers. Department of Economics

No: 10 04. Bilkent University. Monotonic Extension. Farhad Husseinov. Discussion Papers. Department of Economics No: 10 04 Bilkent University Monotonic Extension Farhad Husseinov Discussion Papers Department of Economics The Discussion Papers of the Department of Economics are intended to make the initial results

More information

University of Lille I PC first year list of exercises n 7. Review

University of Lille I PC first year list of exercises n 7. Review University of Lille I PC first year list of exercises n 7 Review Exercise Solve the following systems in 4 different ways (by substitution, by the Gauss method, by inverting the matrix of coefficients

More information

Separation Properties for Locally Convex Cones

Separation Properties for Locally Convex Cones Journal of Convex Analysis Volume 9 (2002), No. 1, 301 307 Separation Properties for Locally Convex Cones Walter Roth Department of Mathematics, Universiti Brunei Darussalam, Gadong BE1410, Brunei Darussalam

More information

MATH 304 Linear Algebra Lecture 9: Subspaces of vector spaces (continued). Span. Spanning set.

MATH 304 Linear Algebra Lecture 9: Subspaces of vector spaces (continued). Span. Spanning set. MATH 304 Linear Algebra Lecture 9: Subspaces of vector spaces (continued). Span. Spanning set. Vector space A vector space is a set V equipped with two operations, addition V V (x,y) x + y V and scalar

More information

1 Introduction to Matrices

1 Introduction to Matrices 1 Introduction to Matrices In this section, important definitions and results from matrix algebra that are useful in regression analysis are introduced. While all statements below regarding the columns

More information

Math 4310 Handout - Quotient Vector Spaces

Math 4310 Handout - Quotient Vector Spaces Math 4310 Handout - Quotient Vector Spaces Dan Collins The textbook defines a subspace of a vector space in Chapter 4, but it avoids ever discussing the notion of a quotient space. This is understandable

More information

3. Mathematical Induction

3. Mathematical Induction 3. MATHEMATICAL INDUCTION 83 3. Mathematical Induction 3.1. First Principle of Mathematical Induction. Let P (n) be a predicate with domain of discourse (over) the natural numbers N = {0, 1,,...}. If (1)

More information

Au = = = 3u. Aw = = = 2w. so the action of A on u and w is very easy to picture: it simply amounts to a stretching by 3 and 2, respectively.

Au = = = 3u. Aw = = = 2w. so the action of A on u and w is very easy to picture: it simply amounts to a stretching by 3 and 2, respectively. Chapter 7 Eigenvalues and Eigenvectors In this last chapter of our exploration of Linear Algebra we will revisit eigenvalues and eigenvectors of matrices, concepts that were already introduced in Geometry

More information

1. Let X and Y be normed spaces and let T B(X, Y ).

1. Let X and Y be normed spaces and let T B(X, Y ). Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: NVP, Frist. 2005-03-14 Skrivtid: 9 11.30 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok

More information

4: EIGENVALUES, EIGENVECTORS, DIAGONALIZATION

4: EIGENVALUES, EIGENVECTORS, DIAGONALIZATION 4: EIGENVALUES, EIGENVECTORS, DIAGONALIZATION STEVEN HEILMAN Contents 1. Review 1 2. Diagonal Matrices 1 3. Eigenvectors and Eigenvalues 2 4. Characteristic Polynomial 4 5. Diagonalizability 6 6. Appendix:

More information

MATH 304 Linear Algebra Lecture 20: Inner product spaces. Orthogonal sets.

MATH 304 Linear Algebra Lecture 20: Inner product spaces. Orthogonal sets. MATH 304 Linear Algebra Lecture 20: Inner product spaces. Orthogonal sets. Norm The notion of norm generalizes the notion of length of a vector in R n. Definition. Let V be a vector space. A function α

More information

Regression With Gaussian Measures

Regression With Gaussian Measures Regression With Gaussian Measures Michael J. Meyer Copyright c April 11, 2004 ii PREFACE We treat the basics of Gaussian processes, Gaussian measures, kernel reproducing Hilbert spaces and related topics.

More information

ISOMETRIES OF R n KEITH CONRAD

ISOMETRIES OF R n KEITH CONRAD ISOMETRIES OF R n KEITH CONRAD 1. Introduction An isometry of R n is a function h: R n R n that preserves the distance between vectors: h(v) h(w) = v w for all v and w in R n, where (x 1,..., x n ) = x

More information

MATH10212 Linear Algebra. Systems of Linear Equations. Definition. An n-dimensional vector is a row or a column of n numbers (or letters): a 1.

MATH10212 Linear Algebra. Systems of Linear Equations. Definition. An n-dimensional vector is a row or a column of n numbers (or letters): a 1. MATH10212 Linear Algebra Textbook: D. Poole, Linear Algebra: A Modern Introduction. Thompson, 2006. ISBN 0-534-40596-7. Systems of Linear Equations Definition. An n-dimensional vector is a row or a column

More information

Continuity of the Perron Root

Continuity of the Perron Root Linear and Multilinear Algebra http://dx.doi.org/10.1080/03081087.2014.934233 ArXiv: 1407.7564 (http://arxiv.org/abs/1407.7564) Continuity of the Perron Root Carl D. Meyer Department of Mathematics, North

More information

α = u v. In other words, Orthogonal Projection

α = u v. In other words, Orthogonal Projection Orthogonal Projection Given any nonzero vector v, it is possible to decompose an arbitrary vector u into a component that points in the direction of v and one that points in a direction orthogonal to v

More information

Linear Algebra. A vector space (over R) is an ordered quadruple. such that V is a set; 0 V ; and the following eight axioms hold:

Linear Algebra. A vector space (over R) is an ordered quadruple. such that V is a set; 0 V ; and the following eight axioms hold: Linear Algebra A vector space (over R) is an ordered quadruple (V, 0, α, µ) such that V is a set; 0 V ; and the following eight axioms hold: α : V V V and µ : R V V ; (i) α(α(u, v), w) = α(u, α(v, w)),

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.436J/15.085J Fall 2008 Lecture 5 9/17/2008 RANDOM VARIABLES

MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.436J/15.085J Fall 2008 Lecture 5 9/17/2008 RANDOM VARIABLES MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.436J/15.085J Fall 2008 Lecture 5 9/17/2008 RANDOM VARIABLES Contents 1. Random variables and measurable functions 2. Cumulative distribution functions 3. Discrete

More information

MA651 Topology. Lecture 6. Separation Axioms.

MA651 Topology. Lecture 6. Separation Axioms. MA651 Topology. Lecture 6. Separation Axioms. This text is based on the following books: Fundamental concepts of topology by Peter O Neil Elements of Mathematics: General Topology by Nicolas Bourbaki Counterexamples

More information

17. Inner product spaces Definition 17.1. Let V be a real vector space. An inner product on V is a function

17. Inner product spaces Definition 17.1. Let V be a real vector space. An inner product on V is a function 17. Inner product spaces Definition 17.1. Let V be a real vector space. An inner product on V is a function, : V V R, which is symmetric, that is u, v = v, u. bilinear, that is linear (in both factors):

More information

Chapter 6. Orthogonality

Chapter 6. Orthogonality 6.3 Orthogonal Matrices 1 Chapter 6. Orthogonality 6.3 Orthogonal Matrices Definition 6.4. An n n matrix A is orthogonal if A T A = I. Note. We will see that the columns of an orthogonal matrix must be

More information

Lebesgue Measure on R n

Lebesgue Measure on R n 8 CHAPTER 2 Lebesgue Measure on R n Our goal is to construct a notion of the volume, or Lebesgue measure, of rather general subsets of R n that reduces to the usual volume of elementary geometrical sets

More information

9 More on differentiation

9 More on differentiation Tel Aviv University, 2013 Measure and category 75 9 More on differentiation 9a Finite Taylor expansion............... 75 9b Continuous and nowhere differentiable..... 78 9c Differentiable and nowhere monotone......

More information

Cartesian Products and Relations

Cartesian Products and Relations Cartesian Products and Relations Definition (Cartesian product) If A and B are sets, the Cartesian product of A and B is the set A B = {(a, b) :(a A) and (b B)}. The following points are worth special

More information

n k=1 k=0 1/k! = e. Example 6.4. The series 1/k 2 converges in R. Indeed, if s n = n then k=1 1/k, then s 2n s n = 1 n + 1 +...

n k=1 k=0 1/k! = e. Example 6.4. The series 1/k 2 converges in R. Indeed, if s n = n then k=1 1/k, then s 2n s n = 1 n + 1 +... 6 Series We call a normed space (X, ) a Banach space provided that every Cauchy sequence (x n ) in X converges. For example, R with the norm = is an example of Banach space. Now let (x n ) be a sequence

More information

Lecture 18 - Clifford Algebras and Spin groups

Lecture 18 - Clifford Algebras and Spin groups Lecture 18 - Clifford Algebras and Spin groups April 5, 2013 Reference: Lawson and Michelsohn, Spin Geometry. 1 Universal Property If V is a vector space over R or C, let q be any quadratic form, meaning

More information

RANDOM INTERVAL HOMEOMORPHISMS. MICHA L MISIUREWICZ Indiana University Purdue University Indianapolis

RANDOM INTERVAL HOMEOMORPHISMS. MICHA L MISIUREWICZ Indiana University Purdue University Indianapolis RANDOM INTERVAL HOMEOMORPHISMS MICHA L MISIUREWICZ Indiana University Purdue University Indianapolis This is a joint work with Lluís Alsedà Motivation: A talk by Yulij Ilyashenko. Two interval maps, applied

More information

THE KADISON-SINGER PROBLEM IN MATHEMATICS AND ENGINEERING: A DETAILED ACCOUNT

THE KADISON-SINGER PROBLEM IN MATHEMATICS AND ENGINEERING: A DETAILED ACCOUNT THE ADISON-SINGER PROBLEM IN MATHEMATICS AND ENGINEERING: A DETAILED ACCOUNT PETER G. CASAZZA, MATTHEW FICUS, JANET C. TREMAIN, ERIC WEBER Abstract. We will show that the famous, intractible 1959 adison-singer

More information

The sample space for a pair of die rolls is the set. The sample space for a random number between 0 and 1 is the interval [0, 1].

The sample space for a pair of die rolls is the set. The sample space for a random number between 0 and 1 is the interval [0, 1]. Probability Theory Probability Spaces and Events Consider a random experiment with several possible outcomes. For example, we might roll a pair of dice, flip a coin three times, or choose a random real

More information

Practice with Proofs

Practice with Proofs Practice with Proofs October 6, 2014 Recall the following Definition 0.1. A function f is increasing if for every x, y in the domain of f, x < y = f(x) < f(y) 1. Prove that h(x) = x 3 is increasing, using

More information

Differential Operators and their Adjoint Operators

Differential Operators and their Adjoint Operators Differential Operators and their Adjoint Operators Differential Operators inear functions from E n to E m may be described, once bases have been selected in both spaces ordinarily one uses the standard

More information

4.5 Linear Dependence and Linear Independence

4.5 Linear Dependence and Linear Independence 4.5 Linear Dependence and Linear Independence 267 32. {v 1, v 2 }, where v 1, v 2 are collinear vectors in R 3. 33. Prove that if S and S are subsets of a vector space V such that S is a subset of S, then

More information

4. Expanding dynamical systems

4. Expanding dynamical systems 4.1. Metric definition. 4. Expanding dynamical systems Definition 4.1. Let X be a compact metric space. A map f : X X is said to be expanding if there exist ɛ > 0 and L > 1 such that d(f(x), f(y)) Ld(x,

More information

Solving Linear Systems, Continued and The Inverse of a Matrix

Solving Linear Systems, Continued and The Inverse of a Matrix , Continued and The of a Matrix Calculus III Summer 2013, Session II Monday, July 15, 2013 Agenda 1. The rank of a matrix 2. The inverse of a square matrix Gaussian Gaussian solves a linear system by reducing

More information

THE BANACH CONTRACTION PRINCIPLE. Contents

THE BANACH CONTRACTION PRINCIPLE. Contents THE BANACH CONTRACTION PRINCIPLE ALEX PONIECKI Abstract. This paper will study contractions of metric spaces. To do this, we will mainly use tools from topology. We will give some examples of contractions,

More information

Notes on Orthogonal and Symmetric Matrices MENU, Winter 2013

Notes on Orthogonal and Symmetric Matrices MENU, Winter 2013 Notes on Orthogonal and Symmetric Matrices MENU, Winter 201 These notes summarize the main properties and uses of orthogonal and symmetric matrices. We covered quite a bit of material regarding these topics,

More information

1 Inner Products and Norms on Real Vector Spaces

1 Inner Products and Norms on Real Vector Spaces Math 373: Principles Techniques of Applied Mathematics Spring 29 The 2 Inner Product 1 Inner Products Norms on Real Vector Spaces Recall that an inner product on a real vector space V is a function from

More information

The Ideal Class Group

The Ideal Class Group Chapter 5 The Ideal Class Group We will use Minkowski theory, which belongs to the general area of geometry of numbers, to gain insight into the ideal class group of a number field. We have already mentioned

More information

Math 550 Notes. Chapter 7. Jesse Crawford. Department of Mathematics Tarleton State University. Fall 2010

Math 550 Notes. Chapter 7. Jesse Crawford. Department of Mathematics Tarleton State University. Fall 2010 Math 550 Notes Chapter 7 Jesse Crawford Department of Mathematics Tarleton State University Fall 2010 (Tarleton State University) Math 550 Chapter 7 Fall 2010 1 / 34 Outline 1 Self-Adjoint and Normal Operators

More information

CITY UNIVERSITY LONDON. BEng Degree in Computer Systems Engineering Part II BSc Degree in Computer Systems Engineering Part III PART 2 EXAMINATION

CITY UNIVERSITY LONDON. BEng Degree in Computer Systems Engineering Part II BSc Degree in Computer Systems Engineering Part III PART 2 EXAMINATION No: CITY UNIVERSITY LONDON BEng Degree in Computer Systems Engineering Part II BSc Degree in Computer Systems Engineering Part III PART 2 EXAMINATION ENGINEERING MATHEMATICS 2 (resit) EX2005 Date: August

More information

CHAPTER II THE LIMIT OF A SEQUENCE OF NUMBERS DEFINITION OF THE NUMBER e.

CHAPTER II THE LIMIT OF A SEQUENCE OF NUMBERS DEFINITION OF THE NUMBER e. CHAPTER II THE LIMIT OF A SEQUENCE OF NUMBERS DEFINITION OF THE NUMBER e. This chapter contains the beginnings of the most important, and probably the most subtle, notion in mathematical analysis, i.e.,

More information

v w is orthogonal to both v and w. the three vectors v, w and v w form a right-handed set of vectors.

v w is orthogonal to both v and w. the three vectors v, w and v w form a right-handed set of vectors. 3. Cross product Definition 3.1. Let v and w be two vectors in R 3. The cross product of v and w, denoted v w, is the vector defined as follows: the length of v w is the area of the parallelogram with

More information