Commutativity of the Exponential Spectrum

Total Page:16

File Type:pdf, Size:1020Kb

Commutativity of the Exponential Spectrum Commutativity of the Exponential Spectrum Aram Gevorgyan Maîtrise en mathématiques Québec, Canada © Aram Gevorgyan, 2015 Résumé Pour l’algèbre de Banach complexe A ayant l’élément unité, on dénote par G(A) l’ensemble des éléments inversibles de A, et par G1(A) on dénote la composante qui contient l’unité. Le spectre de a 2 A est l’ensemble de tous les nombres complexes λ tels que λ1 − a2 = G(A), et le spectre exponentiel de a est l’ensemble de tous les nombres complexes tels que λ1−a2 = G1(A). Évidemment, pour chaque élément de l’algèbre, son spectre exponentiel contient le spectre habituel. Il est bien connu que le spectre habituel a une propriété que l’on nommera «propriété de commutativité». Cela signifie que, pour chaque choix des deux éléments a; b 2 A, nous avons Sp(ab) n f0g = Sp(ba) n f0g, où Sp est le spectre. Avons-nous la même propriété pour les spectres exponentiels? Cette question n’est toujours pas résolue. L’objectif de ce mémoire est d’étudier le spectre exponentiel, et plus particulièrement sa propriété de commutativité. Dans le premier chapitre, nous donnerons les définitions d’algèbre de Banach complexe, spectre et spectre exponentiel de ses éléments, et leurs propriétés de base. Aussi nous établirons des relations topologiques entre les spectres exponentiel et habituel. Dans le deuxième chapitre, nous définirons les fonctions holomorphes sur une algèbre de Banach, et discuterons du problème de la propriété de commutativité de spectre exponentiel, en établissant des résultats positifs connus. Dans le troisième et dernier chapitre, nous examinerons quelques exemples d’algèbres de Ba- nach, décrivant les ensembles G(A) et G1(A), et discuterons de la propriété de commutativité pour ces algèbres. iii Abstract For a complex Banach algebra A with unit element, we denote by G(A) the set of invertible elements of A, and by G1(A) we denote the component of G(A) which contains the unit. The spectrum of a 2 A is the set of all complex numbers λ such that λ1−a2 = G(A), and the exponential spectrum of a is the set of all complex numbers λ such that λ1−a2 = G1(A). Of course for each element of the algebra its exponential spectrum contains the usual spectrum. It is well known that the usual spectrum has the so-called commutativity property. This means that, for any two elements a and b of A, we have Sp(ab) n f0g = Sp(ba) n f0g, where Sp denotes the spectrum. Does this property hold for exponential spectra? This is still an open question. The purpose of this memoir is to study the exponential spectrum, and particularly its commutativity property. In chapter one, we will give definitions of a complex Banach algebra, the spectrum and expo- nential spectrum of its elements, and their basic properties. Also we will establish topological relations between exponential and usual spectra. In chapter two, we will define holomorphic functions on a Banach algebra, and also discuss the commutativity property problem for the exponential spectrum, establishing some known positive results. In the last chapter, we will consider some examples of Banach algebras, describing the sets G(A) and G1(A), and discuss the commutativity property for these algebras. v Contents Résumé iii Abstract v Contents vii Acknowledgments xiii 1 Banach Algebras, Spectrum and Exponential Spectrum1 1.1 Banach Algebras, Definitions and Examples.................... 1 1.2 Invertible Elements and Spectrum ......................... 4 1.3 Holomorphic Functional Calculus.......................... 9 1.4 Exponential Spectrum................................ 13 2 Commutativity of Exponential Spectrum: Positive Results 17 2.1 Special Case, When at Least One of the Two Elements is a Limit of Invertible Elements ....................................... 17 2.2 Other Special Cases ................................. 19 3 Examples of Exponential Spectra 23 3.1 The Wiener Algebra ................................. 23 3.2 The Algebra of Bounded Linear Operators on Infinite-Dimensional Hilbert Space 27 3.3 The Calkin Algebra.................................. 29 3.4 Banach Algebra, With a Disconnected Group of Invertible Elements . 33 Conclusion 37 Bibliography 39 vii To my family ix God used beautiful mathematics in creating the world. Paul Dirac (1902-1984) xi Acknowledgments Several people have been supporting me during my studies and my integration into the social life of Quebec City, since the very first day of my arrival in this town. They were always there to help me with any advice and services I asked for. Without them, my education in Laval university simply couldn’t have progressed to the final stage. First of all I would like to thank my supervisor Professor Thomas Joseph Ransford. Professor Ransford helped me with the very first steps, personally introducing me the Laval University and its personnel who I needed to know during my education. The next and the most valuable help of him was the professional support, scientific discussions, advice he provided through per- sonal meetings. I’m deeply grateful to Professor Ransford, his valuable support was essential at every stage of my education. I also would like to thank all the staff and professors of the Department of Mathematics and Statistics with whom I collaborated or asked for help. They were always kind and ready to help me with any service I needed. Specially I would like to mention Sylvie Drolet and Robert Guénette, whose help and support were very significant for me. I am grateful to my friends in Quebec City, for their advice and support in daily life that was especially valuable at the starting period of my stay in Quebec. Specially I want to thank my friend Anush Stepanyan who advised me to start my education in Laval University and helped me very much with everything I needed. Finally, and most of all, I’m deeply grateful to my family and my friends (in Armenia) who encouraged me and provided all the necessary help to make the decision to move to Canada and to start my education in Laval University. Aram Gevorgyan xiii Chapter 1 Banach Algebras, Spectrum and Exponential Spectrum 1.1 Banach Algebras, Definitions and Examples The material of this chapter is mainly from the book of B. Aupetit Aupetit[1991]. Definition 1.1.1. An algebra is a vector space A over the field C, with a multiplication satisfying the following properties: x(yz) = (xy)z; (x + y)z = xz + yz; x(y + z) = xy + xz; λ(xy) = (λx)y = x(λy) for all x; y; z 2 A, and λ 2 C. If moreover A is a Banach space for a norm k · k and satisfies the norm inequality kxyk ≤ kxkkyk; for all x; y 2 A, we say that A is a complex Banach algebra. In the definition, C could be replaced by any field K, in particular by R, but in this memoir we will deal mainly with complex Banach algebras. A Banach algebra A is called commutative, if for all a; b 2 A we have ab = ba, and with unit, if there is an element 1 2 A with k1k = 1, such that for all a 2 A we have 1a = a1 = a. Obviously if the algebra has a unit, then the unit is unique. Indeed, if there were another e 2 A, such that ea = ae = a for all a 2 A, then e = e1 = 1e = 1. Let us give some examples of Banach algebras. 1 Remark 1.1.2. If A is a Banach algebra without unit, it is always possible to embed it isomet- rically in the Banach algebra with unit A+ = A × C, where the operations and the norm are defined by (x; α) + (y; β) = (x + y; α + β); λ(x; α) = (λx, λα); : (x; α)(y; β) = (xy + βx + αy; αβ); k(x; α)k = kxk + jαj Here e = (0; 1) will be the unit element of A+, and the function x 7! (x; 0) is an isomorphism from A into A+. Example 1.1.3. Let K be a compact set. Then C(K), the space of all complex continuous functions on K, with the supremum norm, is a Banach algebra with unit. If K has only n n elements then C(K) = C with coordinatewise multiplication, and of course C is the simplest commutative Banach algebra. If K is a locally compact space, then the Banach space of all complex continuous functions on K which go to zero at infinity, that is, continuous functions f such that fx : x 2 K; jf(x)j ≥ g is compact for all > 0, with the supremum norm, is a Banach algebra, which has no unit if K is not compact. Example 1.1.4. If K is compact, every closed subalgebra of C(K) is a Banach algebra. For instance if K is a compact subset of C, the following examples of Banach algebras are interesting: The algebra P (K), of continuous functions on K which are uniform limits of polynomials on K; the algebra R(K), of continuous functions on K which are uniform limits of rational functions with poles outside of K; and the algebra A(K), of continuous functions on K which are holomorphic on the interior of K. We have the inclusions P (K) ⊂ R(K) ⊂ A(K) ⊂ C(K), and there are examples of K for which all these inclusions are strict. Example 1.1.5. Let G be a locally compact commutative group and let µ be its Haar measure. Then L1(G) is a Banach algebra if we define multiplication by convolution Z (f ∗ g)(x) = f(xy−1)g(y)dµ(y) G 1 R and the norm by the L -norm kfk1 = G jf(x)jdµ(x).
Recommended publications
  • Fundamental Theorems in Mathematics
    SOME FUNDAMENTAL THEOREMS IN MATHEMATICS OLIVER KNILL Abstract. An expository hitchhikers guide to some theorems in mathematics. Criteria for the current list of 243 theorems are whether the result can be formulated elegantly, whether it is beautiful or useful and whether it could serve as a guide [6] without leading to panic. The order is not a ranking but ordered along a time-line when things were writ- ten down. Since [556] stated “a mathematical theorem only becomes beautiful if presented as a crown jewel within a context" we try sometimes to give some context. Of course, any such list of theorems is a matter of personal preferences, taste and limitations. The num- ber of theorems is arbitrary, the initial obvious goal was 42 but that number got eventually surpassed as it is hard to stop, once started. As a compensation, there are 42 “tweetable" theorems with included proofs. More comments on the choice of the theorems is included in an epilogue. For literature on general mathematics, see [193, 189, 29, 235, 254, 619, 412, 138], for history [217, 625, 376, 73, 46, 208, 379, 365, 690, 113, 618, 79, 259, 341], for popular, beautiful or elegant things [12, 529, 201, 182, 17, 672, 673, 44, 204, 190, 245, 446, 616, 303, 201, 2, 127, 146, 128, 502, 261, 172]. For comprehensive overviews in large parts of math- ematics, [74, 165, 166, 51, 593] or predictions on developments [47]. For reflections about mathematics in general [145, 455, 45, 306, 439, 99, 561]. Encyclopedic source examples are [188, 705, 670, 102, 192, 152, 221, 191, 111, 635].
    [Show full text]
  • Variable-Coefficient Toeplitz Matrices with Symbols Beyond the Wiener
    Operator Theory: Advances and Applications, Vol. 199, 191–202 c 2009 Birkh¨auser Verlag Basel/Switzerland Variable-coefficient Toeplitz Matrices with Symbols beyond the Wiener Algebra Albrecht B¨ottcher and Sergei Grudsky In Memory of Georg Heinig Abstract. Sequences of so-called variable-coefficient Toeplitz matrices arise in many problems, including the discretization of ordinary differential equations with variable coefficients. Such sequences are known to be bounded if the generating function satisfies a condition of the Wiener type, which is far away from the minimal requirement in the case of constant coefficients. The purpose of this paper is to uncover some phenomena beyond the Wiener condition. We provide counterexamples on the one hand and prove easy-to-check sufficient conditions for boundedness on the other. Mathematics Subject Classification (2000). Primary 47B35; Secondary 15A60, 65F35. Keywords. Toeplitz matrix, variable coefficients, matrix norm. 1. Introduction Let a be a complex-valued continuous function on [0, 1] × [0, 1] × T,whereT is the complex unit circle, a :[0, 1] × [0, 1] × T → C, (x, y, t) → a(x, y, t). For n ∈ Z,we −n puta ˆn(x, y)= T a(x, y, t) t |dt|/(2π) and so have the Fourier series ∞ n a(x, y, t)= aˆn(x, y)t , (1) n=−∞ 2 where equality holds at least in the L sense. Let AN (a)bethematrix N j k AN (a)= aˆj−k , . (2) N N j,k=0 Occasionally we allow us to write a(x, y, t)andAN (a(x, y, t)) for a and AN (a). This work was partially supported by CONACYT project U46936-F, Mexico.
    [Show full text]
  • Harmonic Analysis and Centers of Group Algebras
    TRANSACTIONSOF THE AMERICANMATHEMATICAL SOCIETY Volume 195, 1974 HARMONICANALYSIS AND CENTERS OF GROUPALGEBRAS BY J. LIUKKONENi1) AND R. MOSAK(2) ABSTRACT. The purpose of this paper is to present some results of harmonic analysis on the center of the group algebra Z (L (G)) where G is a locally com- pact group. We prove that Z (L (G)) is a regular, Tauberian, symmetric Banach *-algebra and contains a bounded approximate identity. Wiener's generalized Tauberian theorem is therefore applicable to Z (L (G)). These results complement those of I. E. Segal relating to the group algebra of locally compact abelian and compact groups. We also prove that if G contains a compact normal subgroup K such that G/K is abelian, then Z (L (G)) satisfies the condition of Wiener-Ditkin, so that any closed set in its maximal ideal space whose boundary contains no per- fect subset is a set of spectral synthesis. We give an example of a general locally compact group for which Z {L (G)) does not satisfy the condition of Wiener-Ditkin. Introduction. The purpose of this paper is to present some results of harmonic analysis on the center of the group algebra Z(L (G)) where G is a locally com- pact group. We prove that Z (L (G)) is a regular, Tauberian, symmetric Banach *-algebra containing a bounded approximate identity. Wiener's generalized Tau- berian theorem is therefore applicable to Z(L (G)): If M is a closed proper ideal in Z(L (G)), then M is contained in a regular maximal ideal. These results com- plement those of Segal [17] relating to the group algebra of locally compact abe- lian and compact groups.
    [Show full text]
  • Symmetry and Nonsymmetry for Locally Compact Groups
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF FUNCTIONAL ANALYSIS 33, 119-134 (1979) Symmetry and Nonsymmetry for Locally Compact Groups HORS-C LEPTIN AND DETLEV POGUNTKE Universitiit Bielefeld, Universitiitstrasse, 4800 Bielefeld I, Federal Republic of Germany Communicated by the Editors Received June 22, 1977; revised April 3, 1978 The class [S] of locally compact groups G is considered, for which the algebra L’(G) is symmetric (=Hermitian). It is shown that [S] is stable under semidirect compact extensions, i.e., HE [S] and K compact implies K x 8 HE [S]. For connected solvable Lie groups inductive conditions for symmetry are given. A construction for nonsymmetric Banach algebras is given which shows that there exists exactly one connected and simply connected solvable Lie group of dimension 94 which is not in [S]. This example shows that G/Z E [S], Z the center of G, in general does not imply G E [S]. It is shown that nevertheless for discrete groups and a (possibly) stronger form of symmetry this implication holds, implying a new and shorter proof of the fact that [S] contains all discrete nilpotent groups. Recall that a Banach algebra LZ~with isometric involution a -+ a* is called symmetric, if the spectrum Sp a*a for every element a E & is always contained in IW+ = [0, co[. The theorem of Ford and Shirali [2] tells us that this is equiva- Ient to .d being Hermitian, i.e., that Sp b C [w for each b E :d with b = h*.
    [Show full text]
  • Some Algebraic Properties of the Wiener–Laplace Algebra
    Journal of Applied Analysis 16 (2010), 16 pages DOI 10.1515/JAA.2010.006 © de Gruyter 2010 Some algebraic properties of the Wiener–Laplace algebra Raymond Mortini and Amol Sasane Abstract. We denote by W C.C / the set of all complex-valued functions defined in the Note 1 closed right half plane C sC C Re.s/ 0 that differ from the Laplace transform Please 1 C WD ¹ 2 j º check the of functions from L .0; / by a constant. Equipped with pointwise operations, W C.C / 1 C MSC forms a ring. It is known that W C.C / is a pre-Bézout ring. The following properties are numbers C shown for W C.C /: for 2010 C (see W C.C / is not a GCD domain, that is, there exist functions F1;F2 in W C.C / that C C www.ams. do not possess a greatest common divisor in W C.C /. C org/msc). W C.C / is not coherent, and in fact, we give an example of two principal ideals whose intersectionC is not finitely generated. We will also observe that W C.C / is a Hermite ring, by showing that the maximal C ideal space of W C.C /, equipped with the Gelfand topology, is contractible. C Keywords. GCD domain, Wiener–Laplace algebra, control theory. 2010 Mathematics Subject Classification. Primary 46J15; Secondary 13G05, 93D15. 1 Introduction The aim of this paper is to study some algebraic properties of the ring W C.C / (defined below). C We first recall the notion of a GCD domain, a coherent ring and a Hermite ring below.
    [Show full text]
  • Frank - Olme Speck
    DEMONSTRATIO MATHEMATICA Vol. XVIII No 3 1985 Frank - Olme Speck ON GENERAL WIENER-HOPF OPERATOR THEORY AND RECENT APPLICATIONS Dedicated to Professor Donald Cecil Pack on the occasion of his 65th birthday 1. Introduction We oonaider 3 &aneraljffiecar~Hopf operator (WHO) defined by (1.1) W t* PAjpi where X le assumed to be a Banach space, P,AeL(X) linear p bounded operators on X, P = P a projector,, and A invertible, I.e. A"1 e l(X). This notion introduced by M. Shinbrot [14..2] comprehends several Glasses of singular operators in the sen- se of S. ProBSdorf [13], of. section 2„ A crucial point in WHO theory consists in the equivalence of the "regularity" of W (invertible, IPredholm, ...) to a par- ticular factorization of A « A.,A,,... with certain "factor pro- perties" of A< {e.g. having invariant subspaces PX,...), which «J _ -i Ay yieldmeanins g a to"pseudoinverse present the "complet of W e(i nsolutio termsn otf o Pth, e WHA ^equatio ) In nth e The results of this paper were presented during the 3rd Symposium on Integral Equations and Their Applications held at the Teohnioal University of Warsaw, December 3-6, 1984. - 725 2 F.-0. Speck (1.2) WU = V 6 PX. Various applications admit the same operator theoretic facto- rization type due to similar operator algebra structures (sym- bol calculus), cf. the monographs [5, 13» 7, 11]. We always shall assume a cross factorization of A (with respect to X and P) to be given, i.e. (1.3) A = A_CA+ holds with invertible factors and A+PX ® PX, A_QX = QX, P + Q = I (1.4) 1 1 p1 C" PCP P? = PP.,.
    [Show full text]
  • Wiener Algebra for the Quaternions Daniel Alpay Chapman University, [email protected]
    Chapman University Chapman University Digital Commons Mathematics, Physics, and Computer Science Science and Technology Faculty Articles and Faculty Articles and Research Research 2016 Wiener Algebra for the Quaternions Daniel Alpay Chapman University, [email protected] Fabrizio Colombo Politecnico di Milano David P. Kimsey Ben Gurion University of the Negev Irene Sabadini Politecnico di Milano Follow this and additional works at: http://digitalcommons.chapman.edu/scs_articles Part of the Algebra Commons, Discrete Mathematics and Combinatorics Commons, and the Other Mathematics Commons Recommended Citation D. Alpay, F. Colombo,D. Kimsey and I. Sabadini. Wiener algebra for the quaternions. Mediterrean Journal of Mathematics, vol. 13 (2016), no 2, 2463-2482. This Article is brought to you for free and open access by the Science and Technology Faculty Articles and Research at Chapman University Digital Commons. It has been accepted for inclusion in Mathematics, Physics, and Computer Science Faculty Articles and Research by an authorized administrator of Chapman University Digital Commons. For more information, please contact [email protected]. Wiener Algebra for the Quaternions Comments This is a pre-copy-editing, author-produced PDF of an article accepted for publication in Mediterrean Journal of Mathematics, volume 13, issue 2, in 2016 following peer review. The final publication is available at Springer via DOI: 10.1007/s00009-015-0634-z Copyright Springer This article is available at Chapman University Digital Commons: http://digitalcommons.chapman.edu/scs_articles/440 WIENER ALGEBRA FOR THE QUATERNIONS DANIEL ALPAY, FABRIZIO COLOMBO, DAVID P. KIMSEY, AND IRENE SABADINI Abstract. We define and study the counterpart of the Wiener algebra in the quaternionic setting, both for the discrete and continuous case.
    [Show full text]
  • Pairs of Selfadjoint Operators and Their Invariants
    Algebra i analiz St. Petersburg Math. J. Tom. 16 (2004), vyp. 1 Vol. 16 (2005), No. 1, Pages 59–104 S 1061-0022(04)00844-1 Article electronically published on December 14, 2004 PAIRS OF SELFADJOINT OPERATORS AND THEIR INVARIANTS D. ALPAY AND I. GOHBERG Dedicated to Mikhail Birman on the occasion of his 75th birthday, with admiration Abstract. A trace formula is proved for pairs of selfadjoint operators that are close to each other in a certain sense. An important role is played by a function analytic in the open upper half-plane and with positive imaginary part there. This function, called the characteristic function of the pair,coincideswithKre˘ın’s Q-function in the case where the selfadjoint operators are canonical extensions of a common simple and closed Hermitian operator. Special emphasis is given to the finite-dimensional case. Relationships with Kre˘ın’s spectral shift function are also considered. Finally, the case of canonical differential expressions is discussed briefly. In this case, the function N may be chosen to be the Weyl function of the canonical differential expression. §1. Introduction This paper is the second in a series where we study models and trace formulas for pairs of selfadjoint operators. In [8] we considered the case of the so-called canonical differential expressions (see §6 and equation (6.1) for the definitions). Here our starting point is a pair (H+,H−) of selfadjoint operators defined on a separable Hilbert space H and possessing the following properties: 1) for all ω ∈ C \ R, −1 −1 rank (H+ − ωI) − (H− − ωI) = n<∞; 2) we have −1 −1 ker (H+ − ωI) − (H− − ωI) = {0}.
    [Show full text]
  • BANACH FRAMES and BANACH GELFAND TRIPLES (Promoting a New Category)
    Numerical Harmonic Analysis Group BANACH FRAMES and BANACH GELFAND TRIPLES (Promoting a New Category) Hans G. Feichtinger [email protected] www.nuhag.eu Feb. 24th, 2011 London Analysis and Probability Seminar Hans G. Feichtinger [email protected] www.nuhag.euBANACH FRAMES and BANACH GELFAND TRIPLES (Promoting a New Category) Goals of this lecture show that the usual generalizations of linear algebra concepts to the Hilbert space case (namely linear independence and totality) are inappropriate in many cases; that frames and Riesz bases (for subspaces) are the right generalization to Hilbert spaces; that Hilbert spaces are themselves a too narrow concept and should be replaced Banach Gelfand Triples, ideally isomorphic to the canonical ones (`1; `2; `1); Describing the situation of frames or Riesz bases via commutative diagrams allows to extend this notation to Banach Gelfand Triples (:BGTs); Demonstrate by examples (Fourier transform, kernel theorem) that this viewpoint brings us very close to the finite-dimensional setting! Hans G. Feichtinger BANACH FRAMES and BANACH GELFAND TRIPLES (Promoting a New Category) OVERVIEW over this lecture 60- MINUTES This is a talk about the frames viewing frames as RETRACTS, i.e. a construction which can be done in any category; about the ubiquity of Banach Gelfand Triples; provides a setting very similar to the finite dimensional setting; showing how easy they are to use; showing some applications in Fourier Analysis; indicating its relevance for numerical applications; and for teaching purposes; that it is a good vehicle to transfer algebraic facts (over finite Abelian group to the setting of LCA groups); perhaps change your view on Fourier Analysis.
    [Show full text]
  • Linear Functional Analysis (Chapters 8 and 9) Joan Cerd`A
    Linear Functional Analysis (Chapters 8 and 9) Joan Cerd`a Universitat de Barcelona E-mail address: [email protected] 2000 Mathematics Subject Classification. 46-01 Chapter 8 Banach algebras Some important Banach spaces are equipped in a natural way with a con- tinuous product that determines a Banach algebra structure.1 Two basic examples are C(K) with the pointwise multiplication and L(E) with the product of operators if E is a Banach space. It can be useful for the reader to retain C(K) as a simple reference model. The first work devoted to concrete Banach algebras is contained in some papers by J. von Neumann and beginning in 1930. The advantage of con- sidering algebras of operators was clear in his contributions, but it was the abstract setting of Banach algebras which proved to be convenient and which allowed the application of similar ideas in many directions. 2 The main operator on these algebras is the Gelfand transform G : a 7! ba, which maps a unitary commutative Banach algebra A on C to the space C(∆) of all complex continuous functions on the spectrum ∆ of A, which is the set of all nonzero elements χ 2 A0 that are multiplicative. Here ∆ is endowed with the restriction of the w∗-topology and it is compact. As seen in Example 8.14, ∆ is the set of all the evaluations δt (t 2 K) if A = C(K), and fb(δt) = δt(f) = f(t), so that in this case one can consider fb = f. But we will be concerned with the spectral theory of operators in a complex Hilbert space H.
    [Show full text]
  • On a (No Longer) New Segal Algebra
    On a (no longer) new Segal algebra — a review of the Feichtinger algebra Mads Sielemann Jakobsen∗ July 27, 2017 Abstract: Since its invention in 1979, the Feichtinger algebra has become a very useful Banach space of functions with applications in time-frequency analysis, the theory of pseudo-differential operators and several other top- ics. It is easily defined on locally compact abelian groups and, in compar- ison with the Schwartz(-Bruhat) space, the Feichtinger algebra allows for more general results with easier proofs. This review paper gives a linear and comprehensive deduction of the theory of the Feichtinger algebra and its favourable properties. The material gives an entry point into the sub- ject, but it will also give new insight to the expert. A main goal of this paper is to show the equivalence of the many different characterizations of the Feichtinger algebra known in the literature. This task naturally guides the paper through basic properties of functions that belong to the space, over operators on it and to aspects of its dual space. Further results in- clude a seemingly forgotten theorem by Reiter on operators which yield Banach space isomorphisms of the Feichtinger algebra; a new identification of the Feichtinger algebra as the unique Banach space in L1 with certain properties; and the kernel theorem for the Feichtinger algebra. A historical description of the development of the theory, its applications and related function space constructions is included. 1 Introduction arXiv:1608.04566v2 [math.FA] 25 Jul 2017 In 1979 at the “International Workshop on Topological Groups and Group Algebras” at the University of Vienna, H.
    [Show full text]
  • MTH 510/615: Operator Theory and Operator Algebras Semester 2, 2018-19
    MTH 510/615: Operator Theory and Operator Algebras Semester 2, 2018-19 Dr. Prahlad Vaidyanathan Contents 1 Banach Algebras3 1.1 Definition and Examples...........................3 1.2 Invertible Elements..............................7 1.3 Spectrum of an Element........................... 10 1.4 Unital Commutative Banach Algebras................... 15 1.5 Examples of the Gelfand Spectrum..................... 19 1.6 Spectral Permanence Theorem........................ 21 1.7 Exercises.................................... 23 2 C*-Algebras 27 2.1 Operators on Hilbert Spaces......................... 27 2.2 Spectrum of an Element........................... 36 2.3 Unital Commutative C∗ algebras...................... 39 2.4 Spectrum of a Normal Operator....................... 44 2.5 Positive Operators and Polar Decomposition................ 49 2.6 Exercises.................................... 52 3 The Spectral Theorem 53 3.1 The Finite Dimensional Case........................ 53 3.2 Multiplication Operators........................... 56 3.3 The Spectral Theorem............................ 61 3.4 Exercises.................................... 65 3.5 Complex Measures.............................. 66 3.6 Borel Functional Calculus.......................... 71 3.7 Spectral Measures............................... 82 3.8 Compact Normal Operators......................... 84 3.9 Exercises.................................... 89 4 Additional Topics 91 4.1 Quotients of C∗ algebras........................... 91 4.2 Positive Linear Functionals.......................... 94 4.3 The Gelfand-Naimark-Segal Construction.................. 101 5 Instructor Notes 107 2 1 Banach Algebras 1.1 Definition and Examples All vector spaces in this course will be over C. Definition 1.1.1. 1. An algebra is a vector space A over C together with a bilinear multiplication under which A is a ring. In other words, for all α; β 2 C; a; b; c 2 A, we have (αa + βb)c = α(ac) + β(bc) and a(αb + βc) = α(ab) + β(ac) 2.
    [Show full text]