Throughout the book, material has also been added on recent developments, including stability theory, the frame radius, and applications to signal analysis and the control of partial differential equations.
An Introduction to Non-Harmonic Fourier Series, Revised Edition is an update of a widely known and highly respected classic textbook.Throughout the book, material has also been added on recent developments, including stability theory, the frame radius, and applications to signal analysis and the control of partial differential equations.
Cover 1
Contents 8
Preface to the Revised First Edition 12
Preface to the First Edition 14
Chapter 1. Bases in Banach Spaces 16
1 Schauder Bases 16
2 Schauder’s Basis for C[a, b] 18
3 Orthonormal Bases in Hilbert Space 20
4 The Reproducing Kernel 28
5 Complete Sequences 31
6 The Coefficient Functionals 34
7 Duality 37
8 Riesz Bases 40
9 The Stability of Bases in Banach Spaces 46
10 The Stability of Orthonormal Bases in Hilbert Space 50
Chapter 2. Entire Functions of Exponential Type 60
Part one. The Classical Factorization Theorems 61
1 Weierstrass’s Factorization Theorem 61
2 Jensen’s Formula 65
3 Functions of Finite Order 68
4 Estimates for Canonical Products 74
5 Hadamard’s Factorization Theorem 78
Part two. Restrictions along a Line 83
1 The Phragmén.Lindel¨öfŽ Method 83
2 Carleman’s Formula 89
3 Integrability on a Line 94
4 The Paley–Wiener Theorem 100
5 The Paley–Wiener Space 105
Chapter 3. The Completeness of Sets of Complex Exponentials 108
1 The Trigonometric System 109
2 Exponentials Close to the Trigonometric System 114
3 A Counterexample 117
4 Some Intrinsic Properties of Sets of Complex Exponentials 121
5 Stability 125
6 Density and the Completeness Radius 130
Chapter 4. Interpolation and Bases in Hilbert Space 136
1 Moment Sequences in Hilbert Space 137
2 Bessel Sequences and Riesz–Fischer Sequences 143
3 Applications to Systems of Complex Exponentials 150
4 The Moment Space and Its Relation to Equivalent Sequences 154
5 Interpolation in the Paley–Wiener Space: Functions of Sine Type 157
6 Interpolation in the Paley–Wiener Space: Stability 164
7 The Theory of Frames 169
8 The Stability of Nonharmonic Fourier Series 175
9 Pointwise Convergence 180
Notes and Comments 186
References 214
List of Special Symbols 236
Author Index 238
Subject Index 244
Bases in Banach Spaces
1 SCHAUDER BASES
Let X be an infinite-dimensional Banach space over the field of real or complex numbers. When viewed as a vector space, X is known to possess a Hamel basis — a linearly independent subset of X that spans the entire space. Unfortunately, such bases cannot in general be constructed, their very existence depending on the axiom of choice, and their usefulness is therefore severely limited. Of far greater importance and applicability in analysis is the notion of a basis first introduced by Schauder [1927].
Definition. A sequence of vectors {x1, x2, x3, …} in an infinite-dimensional Banach space X is said to be a Schauder basis for X if to each vector x in the space there corresponds a unique sequence of scalars {c1, c2, c3, …} such that
=∑n=1∞cnxn.
The convergence of the series is understood to be with respect to the strong (norm) topology of X; in other words,
−∑i=1ncixi→0asn→∞
Henceforth, the term basis for an infinite-dimensional Banach space will always mean a Schauder basis.
Example. The Banach space lp (1 p < ∞) consists, by definition, of all infinite sequences of scalars c = {c1, c2, c3, …} such that p=∑n=1∞|cn|p1/p<∞. The vector operations are coordinatewise. In each of these spaces, the “natural basis” {e1, e2, e3, …}, where
n=00....010…,
and the 1 appears in the nth position, is easily seen to be a Schauder basis. If c = {cn} is in lp, then the obvious expansion =∑n=1∞cnen is valid.
It is clear that a Banach space with a basis must be separable. Reason: If {xn} is a basis for X, then the set of all finite linear combinations cnxn, where the cn are rational scalars, is countable and dense in X. It follows, for example, that since l∞ is not separable, it cannot possess a basis.
The “basis problem”— whether or not every separable Banach space has a basis — was raised by Banach [1932] and remained until recently one of the outstanding unsolved problems of functional analysis. The question was finally settled by Per Enflo [1973], who constructed an example of a separable Banach space having no basis. The negative answer to the basis problem is perhaps surprising in light of the fact that bases are now known for almost all the familiar examples of infinite-dimensional separable Banach spaces.
PROBLEMS
1. Prove that every vector space has a Hamel basis.
2. Prove that every Hamel basis for a given vector space has the same number of elements. This number is called the (linear) dimension of the space.
3. Show that a Hamel basis for an infinite-dimensional Banach space is uncountable.
4. Show that the dimension of l∞ is equal to c. (Hint: Show that the set {(1, r, r2, …): 0 < r < 1} is linearly independent.)
5. Let X be an infinite-dimensional Banach space.
a. Prove that dim X c. (Hint: Show that there is a vector space isomorphism between l∞ and a subspace of X.)
b. Prove that if X is separable, then dim X = c.
6. The Banach space c0 consists of all infinite sequences of scalars which converge to zero (with the l∞ norm). Show that the natural basis is a Schauder basis for c0.
7. Exhibit a Schauder basis for the Banach space c consisting of all convergent sequences of scalars (with the l∞ norm).
8. Aninfinite series ∑ xn in a Banach space X is said to be unconditionally convergent if every arrangement of its terms converges to the same element. It is said to be absolutely convergent if the series ‖xn‖ is convergent. Show that every absolutely convergent series in X is unconditionally convergent. What about the converse?
9. A basis {xn} for a Banach space X is said to be unconditional (absolute) if every convergent series of the form cnxn is unconditionally (absolutely) convergent.
(a) Show that the natural basis is unconditional for the spaces lp, 1 p < ∞, and c0. Show also that it is absolute for lp only when p = 1. Is it absolute for c0?
(b) Show that the sequence of vectors
,0,0,0…,1100…,1110…,…
forms a basis for c0 which is not unconditional.
2 SCHAUDER’S BASIS FOR C[a, b]
One of the most important and widely studied classical Banach spaces is C[a, b], the space of all continuous functions on the closed finite interval [a, b], together with the norm
f‖=max|fx|.
The celebrated Weierstrass approximation theorem asserts that the polynomials are dense in C[a, b]: if f is continuous on [a, b], then for every positive number ε there is a polynomial P such that the inequality
fx−Px|<ε
holds throughout the interval [a, b].
For a given continuous function, a sequence of approximating polynomials can even be given explicitly. The most elegant representation is due to Bernstein. Let us suppose, for simplicity, that f is continuous on the interval [0, 1]. Then the nth Bernstein polynomial for f is
nx=∑k=0nnkfknxk1−xn−k,n=1,2,3,....
As is well known,
x=limn→∞Bnx
uniformly on [0, 1] (see Akhiezer [1956, p. 30]).
Since every polynomial can be uniformly approximated on a closed interval by a polynomial with rational coefficients, the preceding remarks show that the space C[a, b] is separable; in fact, it has a basis.
Theorem 1
(Schauder). The space C[a, b] possesses a basis.
Proof. We are going to construct a basis for C[a, b] consisting of piecewise-linear functions fn (n = 0, 1, 2, …). This means that to each function f in the space there will correspond a unique sequence of scalars {cn} such that
x=∑n=0∞cnfnx
uniformly on [a, b].
Let {x0, x1, x2, …} be a countable dense subset of [a, b] with x0 = a and x1 = b. Set
0x=1andf1x=x−ab−a.
When n 2, the set of points {x0, x1, …, xn–1} partitions [a, b] into disjoint open intervals, one of which contains xn; call it I. Define
nx=0ifx∉I1ifx=xnlinearelsewhere
for n = 2, 3, 4, … The sequence {f0, f1, f2, …} will be the required basis.
For each function f in C[a, b] and each positive integer n, we denote by Ln f the polygonal function that agrees with f at each of the points x0, x1,…, xn; we denote by L0 f the function whose constant value is f(x0). Since f is uniformly continuous on [a, b], a simple continuity argument shows that
nf→funiformlyonab.
Therefore, we can write
=L0f+∑n=1∞Lnf−Ln−1f.
We are going to show that there are scalars c1, c2, c3, … such that
nf−Ln−1f=cnfnn=1,2,3,….
For this purpose, we shall define a sequence of functions {g0,...
Erscheint lt. Verlag | 23.5.2001 |
---|---|
Sprache | englisch |
Themenwelt | Mathematik / Informatik ► Mathematik ► Analysis |
Naturwissenschaften ► Physik / Astronomie ► Mechanik | |
Technik | |
ISBN-10 | 0-08-049574-5 / 0080495745 |
ISBN-13 | 978-0-08-049574-3 / 9780080495743 |
Haben Sie eine Frage zum Produkt? |
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