Absolutely Minimum Attaining Closed Operators
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Adjoint of Unbounded Operators on Banach Spaces
November 5, 2013 ADJOINT OF UNBOUNDED OPERATORS ON BANACH SPACES M.T. NAIR Banach spaces considered below are over the field K which is either R or C. Let X be a Banach space. following Kato [2], X∗ denotes the linear space of all continuous conjugate linear functionals on X. We shall denote hf; xi := f(x); x 2 X; f 2 X∗: On X∗, f 7! kfk := sup jhf; xij kxk=1 defines a norm on X∗. Definition 1. The space X∗ is called the adjoint space of X. Note that if K = R, then X∗ coincides with the dual space X0. It can be shown, analogues to the case of X0, that X∗ is a Banach space. Let X and Y be Banach spaces, and A : D(A) ⊆ X ! Y be a densely defined linear operator. Now, we st out to define adjoint of A as in Kato [2]. Theorem 2. There exists a linear operator A∗ : D(A∗) ⊆ Y ∗ ! X∗ such that hf; Axi = hA∗f; xi 8 x 2 D(A); f 2 D(A∗) and for any other linear operator B : D(B) ⊆ Y ∗ ! X∗ satisfying hf; Axi = hBf; xi 8 x 2 D(A); f 2 D(B); D(B) ⊆ D(A∗) and B is a restriction of A∗. Proof. Suppose D(A) is dense in X. Let S := ff 2 Y ∗ : x 7! hf; Axi continuous on D(A)g: For f 2 S, define gf : D(A) ! K by (gf )(x) = hf; Axi 8 x 2 D(A): Since D(A) is dense in X, gf has a unique continuous conjugate linear extension to all ∗ of X, preserving the norm. -
Proved for Real Hilbert Spaces. Time Derivatives of Observables and Applications
AN ABSTRACT OF THE THESIS OF BERNARD W. BANKSfor the degree DOCTOR OF PHILOSOPHY (Name) (Degree) in MATHEMATICS presented on (Major Department) (Date) Title: TIME DERIVATIVES OF OBSERVABLES AND APPLICATIONS Redacted for Privacy Abstract approved: Stuart Newberger LetA andH be self -adjoint operators on a Hilbert space. Conditions for the differentiability with respect totof -itH -itH <Ae cp e 9>are given, and under these conditionsit is shown that the derivative is<i[HA-AH]e-itHcp,e-itHyo>. These resultsare then used to prove Ehrenfest's theorem and to provide results on the behavior of the mean of position as a function of time. Finally, Stone's theorem on unitary groups is formulated and proved for real Hilbert spaces. Time Derivatives of Observables and Applications by Bernard W. Banks A THESIS submitted to Oregon State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy June 1975 APPROVED: Redacted for Privacy Associate Professor of Mathematics in charge of major Redacted for Privacy Chai an of Department of Mathematics Redacted for Privacy Dean of Graduate School Date thesis is presented March 4, 1975 Typed by Clover Redfern for Bernard W. Banks ACKNOWLEDGMENTS I would like to take this opportunity to thank those people who have, in one way or another, contributed to these pages. My special thanks go to Dr. Stuart Newberger who, as my advisor, provided me with an inexhaustible supply of wise counsel. I am most greatful for the manner he brought to our many conversa- tions making them into a mutual exchange between two enthusiasta I must also thank my parents for their support during the earlier years of my education.Their contributions to these pages are not easily descerned, but they are there never the less. -
On Relaxation of Normality in the Fuglede-Putnam Theorem
proceedings of the american mathematical society Volume 77, Number 3, December 1979 ON RELAXATION OF NORMALITY IN THE FUGLEDE-PUTNAM THEOREM TAKAYUKIFURUTA1 Abstract. An operator means a bounded linear operator on a complex Hubert space. The familiar Fuglede-Putnam theorem asserts that if A and B are normal operators and if X is an operator such that AX = XB, then A*X = XB*. We shall relax the normality in the hypotheses on A and B. Theorem 1. If A and B* are subnormal and if X is an operator such that AX = XB, then A*X = XB*. Theorem 2. Suppose A, B, X are operators in the Hubert space H such that AX = XB. Assume also that X is an operator of Hilbert-Schmidt class. Then A*X = XB* under any one of the following hypotheses: (i) A is k-quasihyponormal and B* is invertible hyponormal, (ii) A is quasihyponormal and B* is invertible hyponormal, (iii) A is nilpotent and B* is invertible hyponormal. 1. In this paper an operator means a bounded linear operator on a complex Hilbert space. An operator T is called quasinormal if F commutes with T* T, subnormal if T has a normal extension and hyponormal if [ F*, T] > 0 where [S, T] = ST - TS. The inclusion relation of the classes of nonnormal opera- tors listed above is as follows: Normal § Quasinormal § Subnormal ^ Hyponormal; the above inclusions are all proper [3, Problem 160, p. 101]. The familiar Fuglede-Putnam theorem is as follows ([3, Problem 152], [4]). Theorem A. If A and B are normal operators and if X is an operator such that AX = XB, then A*X = XB*. -
Hilbert Space Quantum Mechanics
qmd113 Hilbert Space Quantum Mechanics Robert B. Griffiths Version of 27 August 2012 Contents 1 Vectors (Kets) 1 1.1 Diracnotation ................................... ......... 1 1.2 Qubitorspinhalf ................................. ......... 2 1.3 Intuitivepicture ................................ ........... 2 1.4 General d ............................................... 3 1.5 Ketsasphysicalproperties . ............. 4 2 Operators 5 2.1 Definition ....................................... ........ 5 2.2 Dyadsandcompleteness . ........... 5 2.3 Matrices........................................ ........ 6 2.4 Daggeroradjoint................................. .......... 7 2.5 Hermitianoperators .............................. ........... 7 2.6 Projectors...................................... ......... 8 2.7 Positiveoperators............................... ............ 9 2.8 Unitaryoperators................................ ........... 9 2.9 Normaloperators................................. .......... 10 2.10 Decompositionoftheidentity . ............... 10 References: CQT = Consistent Quantum Theory by Griffiths (Cambridge, 2002). See in particular Ch. 2; Ch. 3; Ch. 4 except for Sec. 4.3. 1 Vectors (Kets) 1.1 Dirac notation ⋆ In quantum mechanics the state of a physical system is represented by a vector in a Hilbert space: a complex vector space with an inner product. The term “Hilbert space” is often reserved for an infinite-dimensional inner product space having the property◦ that it is complete or closed. However, the term is often used nowadays, as in these notes, in a way that includes finite-dimensional spaces, which automatically satisfy the condition of completeness. ⋆ We will use Dirac notation in which the vectors in the space are denoted by v , called a ket, where v is some symbol which identifies the vector. | One could equally well use something like v or v. A multiple of a vector by a complex number c is written as c v —think of it as analogous to cv of cv. | ⋆ In Dirac notation the inner product of the vectors v with w is written v w . -
Multiple Operator Integrals: Development and Applications
Multiple Operator Integrals: Development and Applications by Anna Tomskova A thesis submitted for the degree of Doctor of Philosophy at the University of New South Wales. School of Mathematics and Statistics Faculty of Science May 2017 PLEASE TYPE THE UNIVERSITY OF NEW SOUTH WALES Thesis/Dissertation Sheet Surname or Family name: Tomskova First name: Anna Other name/s: Abbreviation for degree as given in the University calendar: PhD School: School of Mathematics and Statistics Faculty: Faculty of Science Title: Multiple Operator Integrals: Development and Applications Abstract 350 words maximum: (PLEASE TYPE) Double operator integrals, originally introduced by Y.L. Daletskii and S.G. Krein in 1956, have become an indispensable tool in perturbation and scattering theory. Such an operator integral is a special mapping defined on the space of all bounded linear operators on a Hilbert space or, when it makes sense, on some operator ideal. Throughout the last 60 years the double and multiple operator integration theory has been greatly expanded in different directions and several definitions of operator integrals have been introduced reflecting the nature of a particular problem under investigation. The present thesis develops multiple operator integration theory and demonstrates how this theory applies to solving of several deep problems in Noncommutative Analysis. The first part of the thesis considers double operator integrals. Here we present the key definitions and prove several important properties of this mapping. In addition, we give a solution of the Arazy conjecture, which was made by J. Arazy in 1982. In this part we also discuss the theory in the setting of Banach spaces and, as an application, we study the operator Lipschitz estimate problem in the space of all bounded linear operators on classical Lp-spaces of scalar sequences. -
Class Notes, Functional Analysis 7212
Class notes, Functional Analysis 7212 Ovidiu Costin Contents 1 Banach Algebras 2 1.1 The exponential map.....................................5 1.2 The index group of B = C(X) ...............................6 1.2.1 p1(X) .........................................7 1.3 Multiplicative functionals..................................7 1.3.1 Multiplicative functionals on C(X) .........................8 1.4 Spectrum of an element relative to a Banach algebra.................. 10 1.5 Examples............................................ 19 1.5.1 Trigonometric polynomials............................. 19 1.6 The Shilov boundary theorem................................ 21 1.7 Further examples....................................... 21 1.7.1 The convolution algebra `1(Z) ........................... 21 1.7.2 The return of Real Analysis: the case of L¥ ................... 23 2 Bounded operators on Hilbert spaces 24 2.1 Adjoints............................................ 24 2.2 Example: a space of “diagonal” operators......................... 30 2.3 The shift operator on `2(Z) ................................. 32 2.3.1 Example: the shift operators on H = `2(N) ................... 38 3 W∗-algebras and measurable functional calculus 41 3.1 The strong and weak topologies of operators....................... 42 4 Spectral theorems 46 4.1 Integration of normal operators............................... 51 4.2 Spectral projections...................................... 51 5 Bounded and unbounded operators 54 5.1 Operations.......................................... -
Some Elements of Functional Analysis
Some elements of functional analysis J´erˆome Le Rousseau January 8, 2019 Contents 1 Linear operators in Banach spaces 1 2 Continuous and bounded operators 2 3 Spectrum of a linear operator in a Banach space 3 4 Adjoint operator 4 5 Fredholm operators 4 5.1 Characterization of bounded Fredholm operators ............ 5 6 Linear operators in Hilbert spaces 10 Here, X and Y will denote Banach spaces with their norms denoted by k.kX , k.kY , or simply k.k when there is no ambiguity. 1 Linear operators in Banach spaces An operator A from X to Y is a linear map on its domain, a linear subspace of X, to Y . One denotes by D(A) the domain of this operator. An operator from X to Y is thus characterized by its domain and how it acts on this domain. Operators defined this way are usually referred to as unbounded operators. One writes (A, D(A)) to denote the operator along with its domain. The set of linear operators from X to Y is denoted by L (X,Y ). If D(A) is dense in X the operator is said to be densely defined. If D(A) = X one says that the operator A is on X to Y . The range of the operator is denoted by Ran(A), that is, Ran(A)= {Ax; x ∈ D(A)} ⊂ Y, 1 and its kernel, ker(A), is the set of all x ∈ D(A) such that Ax = 0. The graph of A, G(A), is given by G(A)= {(x, Ax); x ∈ D(A)} ⊂ X × Y. -
On Lifting of Operators to Hilbert Spaces Induced by Positive Selfadjoint Operators
View metadata, citation and similar papers at core.ac.uk brought to you by CORE J. Math. Anal. Appl. 304 (2005) 584–598 provided by Elsevier - Publisher Connector www.elsevier.com/locate/jmaa On lifting of operators to Hilbert spaces induced by positive selfadjoint operators Petru Cojuhari a, Aurelian Gheondea b,c,∗ a Department of Applied Mathematics, AGH University of Science and Technology, Al. Mickievicza 30, 30-059 Cracow, Poland b Department of Mathematics, Bilkent University, 06800 Bilkent, Ankara, Turkey c Institutul de Matematic˘a al Academiei Române, C.P. 1-764, 70700 Bucure¸sti, Romania Received 10 May 2004 Available online 29 January 2005 Submitted by F. Gesztesy Abstract We introduce the notion of induced Hilbert spaces for positive unbounded operators and show that the energy spaces associated to several classical boundary value problems for partial differential operators are relevant examples of this type. The main result is a generalization of the Krein–Reid lifting theorem to this unbounded case and we indicate how it provides estimates of the spectra of operators with respect to energy spaces. 2004 Elsevier Inc. All rights reserved. Keywords: Energy space; Induced Hilbert space; Lifting of operators; Boundary value problems; Spectrum 1. Introduction One of the central problem in spectral theory refers to the estimation of the spectra of linear operators associated to different partial differential equations. Depending on the specific problem that is considered, we have to choose a certain space of functions, among * Corresponding author. E-mail addresses: [email protected] (P. Cojuhari), [email protected], [email protected] (A. -
Common Cyclic Vectors for Normal Operators 11
COMMON CYCLIC VECTORS FOR NORMAL OPERATORS WILLIAM T. ROSS AND WARREN R. WOGEN Abstract. If µ is a finite compactly supported measure on C, then the set Sµ 2 2 ∞ of multiplication operators Mφ : L (µ) → L (µ),Mφf = φf, where φ ∈ L (µ) is injective on a set of full µ measure, is the complete set of cyclic multiplication operators on L2(µ). In this paper, we explore the question as to whether or not Sµ has a common cyclic vector. 1. Introduction A bounded linear operator S on a separable Hilbert space H is cyclic with cyclic vector f if the closed linear span of {Snf : n = 0, 1, 2, ···} is equal to H. For many cyclic operators S, especially when S acts on a Hilbert space of functions, the description of the cyclic vectors is well known. Some examples: When S is the multiplication operator f → xf on L2[0, 1], the cyclic vectors f are the L2 functions which are non-zero almost everywhere. When S is the forward shift f → zf on the classical Hardy space H2, the cyclic vectors are the outer functions [10, p. 114] (Beurling’s theorem). When S is the backward shift f → (f − f(0))/z on H2, the cyclic vectors are the non-pseudocontinuable functions [9, 16]. For a collection S of operators on H, we say that S has a common cyclic vector f, if f is a cyclic vector for every S ∈ S. Earlier work of the second author [19] showed that the set of co-analytic Toeplitz operators Tφ, with non-constant symbol φ, on H2 has a common cyclic vector. -
Mathematical Work of Franciszek Hugon Szafraniec and Its Impacts
Tusi Advances in Operator Theory (2020) 5:1297–1313 Mathematical Research https://doi.org/10.1007/s43036-020-00089-z(0123456789().,-volV)(0123456789().,-volV) Group ORIGINAL PAPER Mathematical work of Franciszek Hugon Szafraniec and its impacts 1 2 3 Rau´ l E. Curto • Jean-Pierre Gazeau • Andrzej Horzela • 4 5,6 7 Mohammad Sal Moslehian • Mihai Putinar • Konrad Schmu¨ dgen • 8 9 Henk de Snoo • Jan Stochel Received: 15 May 2020 / Accepted: 19 May 2020 / Published online: 8 June 2020 Ó The Author(s) 2020 Abstract In this essay, we present an overview of some important mathematical works of Professor Franciszek Hugon Szafraniec and a survey of his achievements and influence. Keywords Szafraniec Á Mathematical work Á Biography Mathematics Subject Classification 01A60 Á 01A61 Á 46-03 Á 47-03 1 Biography Professor Franciszek Hugon Szafraniec’s mathematical career began in 1957 when he left his homeland Upper Silesia for Krako´w to enter the Jagiellonian University. At that time he was 17 years old and, surprisingly, mathematics was his last-minute choice. However random this decision may have been, it was a fortunate one: he succeeded in achieving all the academic degrees up to the scientific title of professor in 1980. It turned out his choice to join the university shaped the Krako´w mathematical community. Communicated by Qingxiang Xu. & Jan Stochel [email protected] Extended author information available on the last page of the article 1298 R. E. Curto et al. Professor Franciszek H. Szafraniec Krako´w beyond Warsaw and Lwo´w belonged to the famous Polish School of Mathematics in the prewar period. -
Positive Forms on Banach Spaces
POSITIVE FORMS ON BANACH SPACES B´alint Farkas, M´at´eMatolcsi 25th June 2001 Abstract The first representation theorem establishes a correspondence between positive, self-adjoint operators and closed, positive forms on Hilbert spaces. The aim of this paper is to show that some of the results remain true if the underlying space is a reflexive Banach space. In particular, the construc- tion of the Friedrichs extension and the form sum of positive operators can be carried over to this case. 1 Introduction Let X denote a reflexive complex Banach space, and X∗ its conjugate dual space (i.e. the space of all continuous, conjugate linear functionals over X). We will use the notation (v, x) := v(x) for v X∗ , x X, and (x, v) := v(x). Let A be a densely defined linear operator from∈ X to ∈X∗. Notice that in this context it makes sense to speak about positivity and self-adjointness of A. Indeed, A defines a sesquilinear form on Dom A Dom A via t (x, y) = (Ax)(y) = (Ax, y) × A and A is called positive if tA is positive, i.e. if (Ax, x) 0 for all x Dom A. Also, the adjoint A∗ of A is defined (because A is densely≥ defined)∈ and is a mapping from X∗∗ to X∗, i.e. from X to X∗. Thus, A is called self-adjoint ∗ if A = A . Similarly, the operator A is called symmetric if the form tA is symmetric. In Section 2 we deal with closed, positive forms and associated operators, and arXiv:math/0612015v1 [math.FA] 1 Dec 2006 we establish a generalized version of the first representation theorem. -
A Note on the Definition of an Unbounded Normal Operator
A NOTE ON THE DEFINITION OF AN UNBOUNDED NORMAL OPERATOR MATTHEW ZIEMKE 1. Introduction Let H be a complex Hilbert space and let T : D(T )(⊆ H) !H be a generally unbounded linear operator. In order to begin the discussion about whether or not the operator T is normal, we need to require that T have a dense domain. This ensures that the adjoint operator T ∗ is defined. In the literature, one sees two definitions for what it means for a densely defined operator T to be normal. The first requires that T be closed and that T ∗T = TT ∗ while the second requires that D(T ) = D(T ∗) and kT xk = kT ∗xk for all x 2 D(T ) = D(T ∗). There is no harm in having these competing definitions as they are, in fact, equivalent. While the equivalence of these statements seems to be widely known, the proof is not obvious, and my efforts to find a detailed and self-contained proof of this fact have left me empty-handed. I attempt to give such a proof here. I also want to note that while we say a bounded linear operator T is normal if and only if T ∗T = TT ∗, the lone requirement of T ∗T = TT ∗ for an unbounded densely defined operator does not, in general, imply T is normal. I used [1] and [2] to write this note. 2. Proof of the equivalence We begin with a definition. Definition 2.1. Let T : D(T )(⊆ H) !H be a densely defined operator. We define the T -inner product on D(T ) × D(T ), denoted as h·; ·iT , by the equation hx; yiT = hx; yi + hT x; T yi; for all x; y 2 D(T ): It is easy to see that the T -inner product is, in fact, an inner product on D(T ).