On the Distributional Divergence of Vector Fields Vanishing at Infinity

Total Page:16

File Type:pdf, Size:1020Kb

On the Distributional Divergence of Vector Fields Vanishing at Infinity Proceedings of the Royal Society of Edinburgh, 141A, 65–76, 2011 On the distributional divergence of vector fields vanishing at infinity Thierry De Pauw Institut de Recherches en Math´ematiques et Physique, Universit´e Catholique de Louvain, Chemin du Cyclotron 2, 1348 Louvain-la-Neuve, Belgium ([email protected]) Monica Torres Department of Mathematics, Purdue University, 150 N. University Street, West Lafayette, IN 47907-2067, USA ([email protected]) (MS received 31 August 2009; accepted 1 April 2010) The equation div v = F has a solution v in the space of continuous vector fields m vanishing at infinity if and only if F acts linearly on BVm/(m−1)(R ) (the space of functions in Lm/(m−1)(Rm) whose distributional gradient is a vector-valued measure) and satisfies the following continuity condition: F (uj ) converges to zero for each sequence {uj } such that the measure norms of ∇uj are uniformly bounded and m/(m−1) m uj 0 weakly in L (R ). 1. Introduction The equation ∆u = f ∈ Lm(Rm) need not have a solution u ∈ C1(Rm). In this paper we prove that, to each f ∈ Lm(Rm), there corresponds a continuous vector m m field, vanishing at infinity, v ∈ C0(R ; R ) such that div v = f weakly. In fact, we characterize those distributions F on Rm such that the equation div v = F admits m m a weak solution v ∈ C0(R ; R ). Related results have been obtained in [1–4, 6]. Our first proof, contained in §§ 3–6, follows the same pattern as [2]. A second proof, presented in § 7, is based on the more abstract methods developed in [3]. ∗ m In this paper m 2 and 1 := m/(m − 1). Let BV ∗ (R ) denote the subspace ∗ 1 of L1 (Rm) consisting of those functions u whose distributional gradient ∇u is a vector-valued measure (of finite total mass). We define a charge vanishing at infinity m to be a linear functional F :BV1∗ (R ) → R such that F (uj) → 0 whenever 1∗ m uj 0 weakly in L (R ) and sup ∇uM < ∞. (1.1) j m We denote by CH0(R ) the space of charges vanishing at infinity and we note (see m proposition 3.2) that it is a closed subspace of the dual of BV1∗ (R ) (where the latter is equipped with its norm ∇uM). Examples of charges vanishing at infinity include the functions f ∈ Lm(Rm) (see proposition 3.4) and the distributional c 2011 The Royal Society of Edinburgh 65 66 Th. De Pauw and M. Torres m m divergence div v of v ∈ C0(R ; R ) (see proposition 3.5). Our main result thus consists in proving that the operator m m m C0(R ; R ) → CH0(R ): v → div v (1.2) is onto. This is done by applying the closed range theorem. For this purpose we m ∗ m identify CH0(R ) with BV1∗ (R ) via the evaluation map (see proposition 5.1). m m m This in turn relies on the fact that L (R ) is dense in CH0(R ) (see corollary 4.3, which is obtained by smoothing). Therefore, the adjoint of (1.2) is m m m BV1∗ (R ) →M(R ; R ): u →−∇u. The observation that this operator has a closed range follows from compactness in m BV1∗ (R ) (see proposition 2.6). m Charges vanishing at infinity happen to be the linear functionals on BV1∗ (R ) which are continuous with respect to a certain locally convex linear (sequential, non- m metrizable, non-barrelled) topology TC on BV1∗ (R ). In other words, there exists a m locally convex topology TC on BV1∗ (R ) such that a sequence uj → 0 in the sense of TC if and only if the sequence {uj} verifies the conditions of (1.1). Topologies of this type have been studied in [3, § 3]. Referring to the general theory yields a quicker, though very much abstract proof in § 7. In order to appreciate this alternative route, the reader is expected to be familiar with the methods of [3, § 3]. From m ∗ ∼ m this perspective the key identification CH0(R ) = BV1∗ (R ) is simply saying m that BV1∗ (R )[TC] is semireflexive; a property which follows from the compactness proposition 2.6. 2. Preliminaries A continuous vector field v : Rm → Rm is said to vanish at infinity if, for every ε>0, there exists a compact set K ⊂ Rm such that |v(x)| ε whenever x ∈ Rm \ K. m m These form a linear space denoted by C0(R ; R ), which is complete under the m m m norm v∞ := sup{|v(x)|: x ∈ R }. The linear subspace Cc(R ; R ) (respectively, D(Rm; Rm)) consisting of those vector fields having compact support (respectively, m m smooth vector fields having compact support) is dense in C0(R ; R ). Thus, each m m ∗ element of the dual, T ∈ C0(R ; R ) , is uniquely associated with some vector- valued measure µ ∈M(Rm; Rm) as follows: T (v)= v, dµ , Rm according to the Riesz–Markov representation theorem. Furthermore, m m µM = sup v, dµ : v ∈D(R ; R ) and v∞ 1 . Rm A vector-valued distribution T ∈D(Rm; Rm)∗ with the property that m m sup{T (v): v ∈D(R ; R ) and v∞ 1} < ∞ m m extends uniquely to an element of C0(R ; R ) and is therefore associated with a vector-valued measure as above. Distributional divergence 67 We recall some properties of convolution. Let 1 p<∞, u ∈ Lp(Rm) and ϕ ∈D(Rm). For each x ∈ Rm, we define (u ∗ ϕ)(x)= u(y)ϕ(x − y)dy. Rm It follows from Young’s inequality that u ∗ ϕ ∈ Lp(Rm) and u ∗ ϕLp uLp ϕL1 . (2.1) Furthermore, u ∗ ϕ ∈ C∞(Rm) and ∇(u ∗ ϕ)=u ∗∇ϕ. In the case when ϕ is even and f ∈ Lq(Rm) with p−1 + q−1 =1,wehave f(u ∗ ϕ)= u(f ∗ ϕ). Rm Rm m We fix an approximate identity on R , {ϕk} [5, (6.31)], and we infer that lim u − u ∗ ϕkLp =0. (2.2) k Henceforth we assume that m 2. We let the Sobolev conjugate exponent of 1 be m 1∗ := . m − 1 ∗ Note that L1 (Rm) is isometrically isomorphic to Lm(Rm)∗. We will recall the Gagliardo–Nirenberg–Sobolev inequality ∗ ∇ ϕ L1 κm ϕ L1 whenever ϕ ∈D(Rm). m 1∗ m Definition 2.1. We let BV1∗ (R ) denote the linear subspace of L (R ) con- sisting of those functions u whose distributional gradient ∇u is a vector-valued measure, i.e. m m ∇uM = sup u div v : v ∈D(R ; R ) and v∞ 1 < ∞. Rm | | ∗ ∇ ∗ Rm Readily u := u L1 + u M defines a norm on BV1 ( ), which makes it a Banach space. In view of proposition 2.5, we will use the equivalent norm ∗ ∇ u BV1 := u M. m Definition 2.2. Given a sequence {uj} in BV1∗ (R ), we write uj 0 whenever ∇ ∞ (i) supj uj M < , 1∗ m (ii) uj 0 weakly in L (R ). m 1∗ m Proposition 2.3. Let {uj} be a sequence in BV1∗ (R ), u ∈ L (R ), and assume 1∗ m that uj uweakly in L (R ). It follows that ∇uM lim inf ∇ujM. (2.3) j 68 Th. De Pauw and M. Torres m m m m Proof. Let v ∈D(R ; R ) with v∞ 1. Since div v ∈ L (R ) and u u ∗ j weakly in L1 (Rm) we have, from definition 2.1, u div v = lim uj div v lim inf ∇ujM Rm j Rm j and, taking the supremum over all such v, we conclude that ∇uM lim inf ∇ujM. j The following density result is basic. m Proposition 2.4. Let u ∈ BV1∗ (R ). The following hold: m m (i) for every ϕ ∈D(R ), u ∗ ϕ ∈ BV1∗ (R ) and ∇(u ∗ ϕ)L1 ∇uMϕL1 ; (ii) if {ϕk} is an approximate identity, then u − u ∗ ϕk 0 and lim ∇(u ∗ ϕk)L1 = ∇uM; k m (iii) there exists a sequence {uj} in D(R ) such that u − uj 0 as well as lim ∇ujL1 = ∇uM. j ∗ Proof. We note that (2.1) yields u ∗ ϕ ∈ L1 .Wehave |∇(u ∗ ϕ)|(x)dx = |ϕ ∗∇u|(x)dx Rm Rm = ϕ(x − y)d∇u(y) dx Rm Rm |ϕ(x − y)| d∇u(y)dx Rm Rm = |ϕ(x − y)| dx d∇u(y) Rm Rm = ∇uMϕL1 , (2.4) which shows proposition 2.4(i). Let {ϕk} be an approximate identity. From proposition 2.4(i), we obtain ∇(u ∗ ϕk)M = |∇(u ∗ ϕk)|(x)dx ∇uMϕkL1 = ∇uM. (2.5) Rm 1∗ m 1∗ m Since u ∗ ϕk → u in L (R ), then, in particular, u ∗ ϕk uweakly in L (R ); i.e. m m f[(u ∗ ϕk) − u] → 0 for every f ∈ L (R ). (2.6) Rm Distributional divergence 69 From (2.5) and (2.6) we obtain that u − u ∗ ϕk 0. Moreover, from (2.5) and the lower semicontinuity (2.3) we conclude that limk ∇(u ∗ ϕk)L1 = ∇uM, which shows that proposition 2.4(ii) holds. m In order to establish (iii), we choose a sequence {ψi} in D(R ) such that 1B(0,i) ψi 1B(0,2i) and sup ∇ψiLm < ∞. (2.7) i As usual, let {ϕk} be an approximate identity. Referring to proposition 2.4(ii) we inductively define a strictly increasing sequence of integers {kj} such that |∇ ∗ | ∇ 1 (u ϕkj ) u M + . Rm j For each j and i, we observe that |∇ ∗ | | ∇ ∗ | | ∗ ∇ | [(u ϕkj )ψi] ψi (u ϕkj ) + (u ϕkj ) ψi . | ∗ |1∗ ∈ 1 Rm For fixed j we infer from (2.7) and the relation u ϕkj L ( ) that | ∗ ∇ | | ∗ ∇ | lim sup (u ϕkj ) ψi = lim sup (u ϕkj ) ψi i Rm i B(0,i)c ∗ 1/1 1∗ | ∗ | ∇ m lim sup u ϕkj ψi L i B(0,i)c =0.
Recommended publications
  • Constructive Closed Range and Open Mapping Theorems in This Paper
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Indag. Mathem., N.S., 11 (4), 509-516 December l&2000 Constructive Closed Range and Open Mapping Theorems by Douglas Bridges and Hajime lshihara Department of Mathematics and Statistics, University of Canterbury, Private Bag 4800, Christchurch, New Zealand email: d. [email protected] School of Information Science, Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan email: [email protected] Communicated by Prof. AS. Troelstra at the meeting of November 27,200O ABSTRACT We prove a version of the closed range theorem within Bishop’s constructive mathematics. This is applied to show that ifan operator Ton a Hilbert space has an adjoint and a complete range, then both T and T’ are sequentially open. 1. INTRODUCTION In this paper we continue our constructive exploration of the theory of opera- tors, in particular operators on a Hilbert space ([5], [6], [7]). We work entirely within Bishop’s constructive mathematics, which we regard as mathematics with intuitionistic logic. For discussions of the merits of this approach to mathematics - in particular, the multiplicity of its models - see [3] and [ll]. The technical background needed in our paper is found in [I] and [IO]. Our main aim is to prove the following result, the constructive Closed Range Theorem for operators on a Hilbert space (cf. [18], pages 99-103): Theorem 1. Let H be a Hilbert space, and T a linear operator on H such that T* exists and ran(T) is closed.
    [Show full text]
  • Operator Algebras Generated by Left Invertibles Derek Desantis [email protected]
    University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers Mathematics, Department of in Mathematics 3-2019 Operator algebras generated by left invertibles Derek DeSantis [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/mathstudent Part of the Analysis Commons, Harmonic Analysis and Representation Commons, and the Other Mathematics Commons DeSantis, Derek, "Operator algebras generated by left invertibles" (2019). Dissertations, Theses, and Student Research Papers in Mathematics. 93. https://digitalcommons.unl.edu/mathstudent/93 This Article is brought to you for free and open access by the Mathematics, Department of at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Dissertations, Theses, and Student Research Papers in Mathematics by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. OPERATOR ALGEBRAS GENERATED BY LEFT INVERTIBLES by Derek DeSantis A DISSERTATION Presented to the Faculty of The Graduate College at the University of Nebraska In Partial Fulfilment of Requirements For the Degree of Doctor of Philosophy Major: Mathematics Under the Supervision of Professor David Pitts Lincoln, Nebraska March, 2019 OPERATOR ALGEBRAS GENERATED BY LEFT INVERTIBLES Derek DeSantis, Ph.D. University of Nebraska, 2019 Adviser: David Pitts Operator algebras generated by partial isometries and their adjoints form the basis for some of the most well studied classes of C*-algebras. Representations of such algebras encode the dynamics of orthonormal sets in a Hilbert space. We instigate a research program on concrete operator algebras that model the dynamics of Hilbert space frames. The primary object of this thesis is the norm-closed operator algebra generated by a left y invertible T together with its Moore-Penrose inverse T .
    [Show full text]
  • U. Green's Functions
    Theoretical Physics Prof. Ruiz, UNC Asheville, doctorphys on YouTube Chapter U Notes. Green's Functions U1. Impulse Response. We return to our low-pass filter with R 1 , C 1 , and ft( ) 1 for 1 second from t 0 to t 1 . The initial charge on the capacitor is q(0) 0 . We have already solved this problem. The charge on the capacitor is given by the following integral. t q()()() t f u g t u du 0 This solution is the convolution of our input voltage function ft() t and the capacitor-decay response function g() t e . The input function is for us to choose, but the capacitor response function is intrinsic to our low-pass filter. q dq f() t V IR I q q Our differential equation is C dt . The Laplace transform gives F()()() s sQ s Q s 1 Q()()()() s F s F s G s s 1 We know from before that a product in Laplace-transform s-space means a convolution of the respective functions in our t-space. The s-space shows clearly the separation of our input function and the response function. All of the secrets of the system are in Gs(). What is the formal way to solve for this without the Fs() getting in the way? Well, if you set ft( ) 0 , that kills things because the Laplace transform of zero is 1 Q() s (0) (0)() G s 0 zero and you would get . s 1 Michael J. Ruiz, Creative Commons Attribution-NonCommercial-ShareAlike 3.0 Unported License So we really want Q() s F ()() s G s (1)() G s G () s in order to get to know the system for itself.
    [Show full text]
  • An Introduction to Basic Functional Analysis
    AN INTRODUCTION TO BASIC FUNCTIONAL ANALYSIS T. S. S. R. K. RAO . 1. Introduction This is a write-up of the lectures given at the Advanced Instructional School (AIS) on ` Functional Analysis and Harmonic Analysis ' during the ¯rst week of July 2006. All of the material is standard and can be found in many basic text books on Functional Analysis. As the prerequisites, I take the liberty of assuming 1) Basic Metric space theory, including completeness and the Baire category theorem. 2) Basic Lebesgue measure theory and some abstract (σ-¯nite) measure theory in- cluding the Radon-Nikodym theorem and the completeness of Lp-spaces. I thank Professor A. Mangasuli for carefully proof reading these notes. 2. Banach spaces and Examples. Let X be a vector space over the real or complex scalar ¯eld. Let k:k : X ! R+ be a function such that (1) kxk = 0 , x = 0 (2) k®xk = j®jkxk (3) kx + yk · kxk + kyk for all x; y 2 X and scalars ®. Such a function is called a norm on X and (X; k:k) is called a normed linear space. Most often we will be working with only one speci¯c k:k on any given vector space X thus we omit writing k:k and simply say that X is a normed linear space. It is an easy exercise to show that d(x; y) = kx ¡ yk de¯nes a metric on X and thus there is an associated notion of topology and convergence. If X is a normed linear space and Y ½ X is a subspace then by restricting the norm to Y , we can consider Y as a normed linear space.
    [Show full text]
  • Normed and Banach Spaces 9 1
    Funtional Analysis Lecture notes for 18.102 Richard Melrose Department of Mathematics, MIT E-mail address: [email protected] Version 0.8D; Revised: 4-5-2010; Run: February 4, 2014 . Contents Preface 5 Introduction 6 Chapter 1. Normed and Banach spaces 9 1. Vector spaces 9 2. Normed spaces 11 3. Banach spaces 13 4. Operators and functionals 16 5. Subspaces and quotients 19 6. Completion 20 7. More examples 24 8. Baire's theorem 26 9. Uniform boundedness 27 10. Open mapping theorem 28 11. Closed graph theorem 30 12. Hahn-Banach theorem 30 13. Double dual 34 14. Axioms of a vector space 34 Chapter 2. The Lebesgue integral 35 1. Integrable functions 35 2. Linearity of L1 39 3. The integral on L1 41 4. Summable series in L1(R) 45 5. The space L1(R) 47 6. The three integration theorems 48 7. Notions of convergence 51 8. Measurable functions 51 9. The spaces Lp(R) 52 10. The space L2(R) 53 11. The spaces Lp(R) 55 12. Lebesgue measure 58 13. Density of step functions 59 14. Measures on the line 61 15. Higher dimensions 62 Removed material 64 Chapter 3. Hilbert spaces 67 1. pre-Hilbert spaces 67 2. Hilbert spaces 68 3 4 CONTENTS 3. Orthonormal sets 69 4. Gram-Schmidt procedure 69 5. Complete orthonormal bases 70 6. Isomorphism to l2 71 7. Parallelogram law 72 8. Convex sets and length minimizer 72 9. Orthocomplements and projections 73 10. Riesz' theorem 74 11. Adjoints of bounded operators 75 12.
    [Show full text]
  • An Introduction to Some Aspects of Functional Analysis
    An introduction to some aspects of functional analysis Stephen Semmes Rice University Abstract These informal notes deal with some very basic objects in functional analysis, including norms and seminorms on vector spaces, bounded linear operators, and dual spaces of bounded linear functionals in particular. Contents 1 Norms on vector spaces 3 2 Convexity 4 3 Inner product spaces 5 4 A few simple estimates 7 5 Summable functions 8 6 p-Summable functions 9 7 p =2 10 8 Bounded continuous functions 11 9 Integral norms 12 10 Completeness 13 11 Bounded linear mappings 14 12 Continuous extensions 15 13 Bounded linear mappings, 2 15 14 Bounded linear functionals 16 1 15 ℓ1(E)∗ 18 ∗ 16 c0(E) 18 17 H¨older’s inequality 20 18 ℓp(E)∗ 20 19 Separability 22 20 An extension lemma 22 21 The Hahn–Banach theorem 23 22 Complex vector spaces 24 23 The weak∗ topology 24 24 Seminorms 25 25 The weak∗ topology, 2 26 26 The Banach–Alaoglu theorem 27 27 The weak topology 28 28 Seminorms, 2 28 29 Convergent sequences 30 30 Uniform boundedness 31 31 Examples 32 32 An embedding 33 33 Induced mappings 33 34 Continuity of norms 34 35 Infinite series 35 36 Some examples 36 37 Quotient spaces 37 38 Quotients and duality 38 39 Dual mappings 39 2 40 Second duals 39 41 Continuous functions 41 42 Bounded sets 42 43 Hahn–Banach, revisited 43 References 44 1 Norms on vector spaces Let V be a vector space over the real numbers R or the complex numbers C.
    [Show full text]
  • Frames and Representing Systems in Fréchet Spaces and Their Duals
    Frames and representing systems in Fr´echet spaces and their duals J. Bonet, C. Fern´andez,A. Galbis, J.M. Ribera Abstract Frames and Bessel sequences in Fr´echet spaces and their duals are defined and studied. Their relation with Schauder frames and representing systems is analyzed. The abstract results presented here, when applied to concrete spaces of analytic functions, give many examples and consequences about sampling sets and Dirichlet series expansions. 1 Introduction and preliminaries The purpose of this paper is twofold. On the one hand we study Λ-Bessel sequences 0 (gi)i ⊂ E , Λ-frames and frames with respect to Λ in the dual of a Hausdorff locally convex space E, in particular for Fr´echet spaces and complete (LB)-spaces E, with Λ a sequence space. We investigate the relation of these concepts with representing systems in the sense of Kadets and Korobeinik [12] and with the Schauder frames, that were investigated by the authors in [7]. On the other hand our article emphasizes the deep connection of frames for Fr´echet and (LB)-spaces with the sufficient and weakly sufficient sets for weighted Fr´echet and (LB)-spaces of holomorphic functions. These concepts correspond to sampling sets in the case of Banach spaces of holomorphic functions. Our general results in Sections 2 and 3 permit us to obtain as a consequence many examples and results in the literature in a unified way in Section 4. Section 2 of our article is inspired by the work of Casazza, Christensen and Stoeva [9] in the context of Banach spaces.
    [Show full text]
  • Methods of Applied Mathematics
    Methods of Applied Mathematics Todd Arbogast and Jerry L. Bona Department of Mathematics, and Institute for Computational Engineering and Sciences The University of Texas at Austin Copyright 1999{2001, 2004{2005, 2007{2008 (corrected version) by T. Arbogast and J. Bona. Contents Chapter 1. Preliminaries 5 1.1. Elementary Topology 5 1.2. Lebesgue Measure and Integration 13 1.3. Exercises 23 Chapter 2. Normed Linear Spaces and Banach Spaces 27 2.1. Basic Concepts and Definitions. 27 2.2. Some Important Examples 34 2.3. Hahn-Banach Theorems 43 2.4. Applications of Hahn-Banach 48 2.5. The Embedding of X into its Double Dual X∗∗ 52 2.6. The Open Mapping Theorem 53 2.7. Uniform Boundedness Principle 57 2.8. Compactness and Weak Convergence in a NLS 58 2.9. The Dual of an Operator 63 2.10. Exercises 66 Chapter 3. Hilbert Spaces 73 3.1. Basic Properties of Inner-Products 73 3.2. Best Approximation and Orthogonal Projections 75 3.3. The Dual Space 78 3.4. Orthonormal Subsets 79 3.5. Weak Convergence in a Hilbert Space 86 3.6. Exercises 87 Chapter 4. Spectral Theory and Compact Operators 89 4.1. Definitions of the Resolvent and Spectrum 90 4.2. Basic Spectral Theory in Banach Spaces 91 4.3. Compact Operators on a Banach Space 93 4.4. Bounded Self-Adjoint Linear Operators on a Hilbert Space 99 4.5. Compact Self-Adjoint Operators on a Hilbert Space 104 4.6. The Ascoli-Arzel`aTheorem 107 4.7. Sturm Liouville Theory 109 4.8.
    [Show full text]
  • On Linear Operators with Closed Range 1 Introduction
    Journal of Applied Mathematics & Bioinformatics, vol.1, no.2, 2011, 175-182 ISSN: 1792-6602 (print), 1792-6939 (online) International Scientific Press, 2011 On Linear Operators with Closed Range P. Sam Johnson1 and S. Balaji2 Abstract Linear operators between Fr´echet spaces such that the closedness of range of an operator implies the closedness of range of another operator are discussed when the operators are topologically dominated by each other. Mathematics Subject Classification (2010): 47A05, 47A30. Keywords: Fr´echet spaces, closed range operators 1 Introduction Let X and Y be normed spaces, B(X,Y ) will denote the normed space of all continuous linear operators from X to Y . R(T ) and N(T ) will denote the range and null spaces of a linear operator T respectively. The Banach’s closed range theorem [5] reads as follows : If X and Y are Banach spaces and if T ∈B(X,Y ), then R(T ) is closed in Y if and only if R(T ∗) is closed in X∗. Given a differential operator T defined on some subspace of Lp(Ω), one may be interested in determining the family of functions y ∈ Lp(Ω) for which Tf = y has a solution. It is well known that if T ∈ B(X,Y ) has closed range, then the space of such y is the orthogonal complement of the solutions to the homogeneous equation T ∗g = 0. There are many important 1 National Institute of Technology Karnataka, Mangalore, India, e-mail: [email protected] 2 National Institute of Technology Karnataka, Mangalore, India, e-mail: [email protected] Article Info: Revised : August 24, 2011.
    [Show full text]
  • Unbounded Linear Operators Jan Derezinski
    Unbounded linear operators Jan Derezi´nski Department of Mathematical Methods in Physics Faculty of Physics University of Warsaw Ho_za74, 00-682, Warszawa, Poland Lecture notes, version of June 2013 Contents 3 1 Unbounded operators on Banach spaces 13 1.1 Relations . 13 1.2 Linear partial operators . 17 1.3 Closed operators . 18 1.4 Bounded operators . 20 1.5 Closable operators . 21 1.6 Essential domains . 23 1.7 Perturbations of closed operators . 24 1.8 Invertible unbounded operators . 28 1.9 Spectrum of unbounded operators . 32 1.10 Functional calculus . 36 1.11 Spectral idempotents . 41 1.12 Examples of unbounded operators . 43 1.13 Pseudoresolvents . 45 2 One-parameter semigroups on Banach spaces 47 2.1 (M; β)-type semigroups . 47 2.2 Generator of a semigroup . 49 2.3 One-parameter groups . 54 2.4 Norm continuous semigroups . 55 2.5 Essential domains of generators . 56 2.6 Operators of (M; β)-type ............................ 58 2.7 The Hille-Philips-Yosida theorem . 60 2.8 Semigroups of contractions and their generators . 65 3 Unbounded operators on Hilbert spaces 67 3.1 Graph scalar product . 67 3.2 The adjoint of an operator . 68 3.3 Inverse of the adjoint operator . 72 3.4 Numerical range and maximal operators . 74 3.5 Dissipative operators . 78 3.6 Hermitian operators . 80 3.7 Self-adjoint operators . 82 3.8 Spectral theorem . 85 3.9 Essentially self-adjoint operators . 89 3.10 Rigged Hilbert space . 90 3.11 Polar decomposition . 94 3.12 Scale of Hilbert spaces I . 98 3.13 Scale of Hilbert spaces II .
    [Show full text]
  • An Overview of Some Recent Developments on the Invariant Subspace Problem
    Concrete Operators Review Article • DOI: 10.2478/conop-2012-0001 • CO • 2013 • 1-10 An overview of some recent developments on the Invariant Subspace Problem Abstract This paper presents an account of some recent approaches to Isabelle Chalendar1∗, Jonathan R. Partington2† the Invariant Subspace Problem. It contains a brief historical account of the problem, and some more detailed discussions 1 Université de Lyon; CNRS; Université Lyon 1; INSA de Lyon; Ecole of specific topics, namely, universal operators, the Bishop op- Centrale de Lyon, CNRS, UMR 5208, Institut Camille Jordan 43 bld. du 11 novembre 1918, F-69622 Villeurbanne Cedex, France erators, and Read’s Banach space counter-example involving a finitely strictly singular operator. 2 School of Mathematics, University of Leeds, Leeds LS2 9JT, U.K. Keywords Received 24 July 2012 Invariant subspace • Universal operator • Weighted shift • Composition operator • Bishop operator • Strictly singular • Accepted 31 August 2012 Finitely strictly singular MSC: 47A15, 47B37, 47B33, 47B07 © Versita sp. z o.o. 1. History of the problem There is an important problem in operator theory called the invariant subspace problem. This problem is open for more than half a century, and there are many significant contributions with a huge variety of techniques, making this challenging problem so interesting; however the solution seems to be nowhere in sight. In this paper we first review the history of the problem, and then present an account of some recent developments with which we have been involved. Other recent approaches are discussed in [21]. The invariant subspace problem is the following: let X be a complex Banach space of dimension at least 2 and let T ∈ L(X), i.e., T : X → X, linear and bounded.
    [Show full text]
  • Functional Analysis
    Principles of Functional Analysis SECOND EDITION Martin Schechter Graduate Studies in Mathematics Volume 36 American Mathematical Society http://dx.doi.org/10.1090/gsm/036 Selected Titles in This Series 36 Martin Schechter, Principles of functional analysis, second edition, 2002 35 JamesF.DavisandPaulKirk, Lecture notes in algebraic topology, 2001 34 Sigurdur Helgason, Differential geometry, Lie groups, and symmetric spaces, 2001 33 Dmitri Burago, Yuri Burago, and Sergei Ivanov, A course in metric geometry, 2001 32 Robert G. Bartle, A modern theory of integration, 2001 31 Ralf Korn and Elke Korn, Option pricing and portfolio optimization: Modern methods of financial mathematics, 2001 30 J. C. McConnell and J. C. Robson, Noncommutative Noetherian rings, 2001 29 Javier Duoandikoetxea, Fourier analysis, 2001 28 Liviu I. Nicolaescu, Notes on Seiberg-Witten theory, 2000 27 Thierry Aubin, A course in differential geometry, 2001 26 Rolf Berndt, An introduction to symplectic geometry, 2001 25 Thomas Friedrich, Dirac operators in Riemannian geometry, 2000 24 Helmut Koch, Number theory: Algebraic numbers and functions, 2000 23 Alberto Candel and Lawrence Conlon, Foliations I, 2000 22 G¨unter R. Krause and Thomas H. Lenagan, Growth of algebras and Gelfand-Kirillov dimension, 2000 21 John B. Conway, A course in operator theory, 2000 20 Robert E. Gompf and Andr´as I. Stipsicz, 4-manifolds and Kirby calculus, 1999 19 Lawrence C. Evans, Partial differential equations, 1998 18 Winfried Just and Martin Weese, Discovering modern set theory. II: Set-theoretic tools for every mathematician, 1997 17 Henryk Iwaniec, Topics in classical automorphic forms, 1997 16 Richard V. Kadison and John R. Ringrose, Fundamentals of the theory of operator algebras.
    [Show full text]