Stability of Operators and C0-Semigroups
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1 Bounded and Unbounded Operators
1 1 Bounded and unbounded operators 1. Let X, Y be Banach spaces and D 2 X a linear space, not necessarily closed. 2. A linear operator is any linear map T : D ! Y . 3. D is the domain of T , sometimes written Dom (T ), or D (T ). 4. T (D) is the Range of T , Ran(T ). 5. The graph of T is Γ(T ) = f(x; T x)jx 2 D (T )g 6. The kernel of T is Ker(T ) = fx 2 D (T ): T x = 0g 1.1 Operations 1. aT1 + bT2 is defined on D (T1) \D (T2). 2. if T1 : D (T1) ⊂ X ! Y and T2 : D (T2) ⊂ Y ! Z then T2T1 : fx 2 D (T1): T1(x) 2 D (T2). In particular, inductively, D (T n) = fx 2 D (T n−1): T (x) 2 D (T )g. The domain may become trivial. 3. Inverse. The inverse is defined if Ker(T ) = f0g. This implies T is bijective. Then T −1 : Ran(T ) !D (T ) is defined as the usual function inverse, and is clearly linear. @ is not invertible on C1[0; 1]: Ker@ = C. 4. Closable operators. It is natural to extend functions by continuity, when possible. If xn ! x and T xn ! y we want to see whether we can define T x = y. Clearly, we must have xn ! 0 and T xn ! y ) y = 0; (1) since T (0) = 0 = y. Conversely, (1) implies the extension T x := y when- ever xn ! x and T xn ! y is consistent and defines a linear operator. -
A Topology for Operator Modules Over W*-Algebras Bojan Magajna
Journal of Functional AnalysisFU3203 journal of functional analysis 154, 1741 (1998) article no. FU973203 A Topology for Operator Modules over W*-Algebras Bojan Magajna Department of Mathematics, University of Ljubljana, Jadranska 19, Ljubljana 1000, Slovenia E-mail: Bojan.MagajnaÄuni-lj.si Received July 23, 1996; revised February 11, 1997; accepted August 18, 1997 dedicated to professor ivan vidav in honor of his eightieth birthday Given a von Neumann algebra R on a Hilbert space H, the so-called R-topology is introduced into B(H), which is weaker than the norm and stronger than the COREultrastrong operator topology. A right R-submodule X of B(H) is closed in the Metadata, citation and similar papers at core.ac.uk Provided byR Elsevier-topology - Publisher if and Connector only if for each b #B(H) the right ideal, consisting of all a # R such that ba # X, is weak* closed in R. Equivalently, X is closed in the R-topology if and only if for each b #B(H) and each orthogonal family of projections ei in R with the sum 1 the condition bei # X for all i implies that b # X. 1998 Academic Press 1. INTRODUCTION Given a C*-algebra R on a Hilbert space H, a concrete operator right R-module is a subspace X of B(H) (the algebra of all bounded linear operators on H) such that XRX. Such modules can be characterized abstractly as L -matricially normed spaces in the sense of Ruan [21], [11] which are equipped with a completely contractive R-module multi- plication (see [6] and [9]). -
7.3 Topological Vector Spaces, the Weak and Weak⇤ Topology on Banach Spaces
138 CHAPTER 7. ELEMENTS OF FUNCTIONAL ANALYSIS 7.3 Topological Vector spaces, the weak and weak⇤ topology on Banach spaces The following generalizes normed Vector space. Definition 7.3.1. Let X be a vector space over K, K = C, or K = R, and assume that is a topology on X. we say that X is a topological vector T space (with respect to ), if (X X and K X are endowed with the T ⇥ ⇥ respective product topology) +:X X X, (x, y) x + y is continuous ⇥ ! 7! : K X (λ, x) λ x is continuous. · ⇥ 7! · A topological vector space X is called locally convex,ifeveryx X has a 2 neighborhood basis consisting of convex sets, where a set A X is called ⇢ convex if for all x, y A, and 0 <t<1, it follows that tx +1 t)y A. 2 − 2 In order to define a topology on a vector space E which turns E into a topological vector space we (only) need to define an appropriate neighbor- hood basis of 0. Proposition 7.3.2. Assume that (E, ) is a topological vector space. And T let = U , 0 U . U0 { 2T 2 } Then a) For all x E, x + = x + U : U is a neighborhood basis of x, 2 U0 { 2U0} b) for all U there is a V so that V + V U, 2U0 2U0 ⇢ c) for all U and all R>0 there is a V ,sothat 2U0 2U0 λ K : λ <R V U, { 2 | | }· ⇢ d) for all U and x E there is an ">0,sothatλx U,forall 2U0 2 2 λ K with λ <", 2 | | e) if (E, ) is Hausdor↵, then for every x E, x =0, there is a U T 2 6 2U0 with x U, 62 f) if E is locally convex, then for all U there is a convex V , 2U0 2T with V U. -
On the Origin and Early History of Functional Analysis
U.U.D.M. Project Report 2008:1 On the origin and early history of functional analysis Jens Lindström Examensarbete i matematik, 30 hp Handledare och examinator: Sten Kaijser Januari 2008 Department of Mathematics Uppsala University Abstract In this report we will study the origins and history of functional analysis up until 1918. We begin by studying ordinary and partial differential equations in the 18th and 19th century to see why there was a need to develop the concepts of functions and limits. We will see how a general theory of infinite systems of equations and determinants by Helge von Koch were used in Ivar Fredholm’s 1900 paper on the integral equation b Z ϕ(s) = f(s) + λ K(s, t)f(t)dt (1) a which resulted in a vast study of integral equations. One of the most enthusiastic followers of Fredholm and integral equation theory was David Hilbert, and we will see how he further developed the theory of integral equations and spectral theory. The concept introduced by Fredholm to study sets of transformations, or operators, made Maurice Fr´echet realize that the focus should be shifted from particular objects to sets of objects and the algebraic properties of these sets. This led him to introduce abstract spaces and we will see how he introduced the axioms that defines them. Finally, we will investigate how the Lebesgue theory of integration were used by Frigyes Riesz who was able to connect all theory of Fredholm, Fr´echet and Lebesgue to form a general theory, and a new discipline of mathematics, now known as functional analysis. -
AND the DOUBLE COMMUTANT THEOREM Recall
Egbert Rijke Utrecht University [email protected] THE STRONG OPERATOR TOPOLOGY ON B(H) AND THE DOUBLE COMMUTANT THEOREM ABSTRACT. These are the notes for a presentation on the strong and weak operator topolo- gies on B(H) and on commutants of unital self-adjoint subalgebras of B(H) in the seminar on von Neumann algebras in Utrecht. The main goal for this talk was to prove the double commutant theorem of von Neumann. We will also give a proof of Vigiers theorem and we will work out several useful properties of the commutant. Recall that a seminorm on a vector space V is a map p : V ! [0;¥) with the properties that (i) p(lx) = jljp(x) for every vector x 2 V and every scalar l and (ii) p(x + y) ≤ p(x) + p(y) for every pair of vectors x;y 2 V. If P is a family of seminorms on V there is a topology generated by P of which the subbasis is defined by the sets fv 2 V : p(v − x) < eg; where e > 0, p 2 P and x 2 V. Hence a subset U of V is open if and only if for every x 2 U there exist p1;:::; pn 2 P, and e > 0 with the property that n \ fv 2 V : pi(v − x) < eg ⊂ U: i=1 A family P of seminorms on V is called separating if, for every non-zero vector x, there exists a seminorm p in P such that p(x) 6= 0. -
Dissipative Operators in a Banach Space
Pacific Journal of Mathematics DISSIPATIVE OPERATORS IN A BANACH SPACE GUNTER LUMER AND R. S. PHILLIPS Vol. 11, No. 2 December 1961 DISSIPATIVE OPERATORS IN A BANACH SPACE G. LUMER AND R. S. PHILLIPS 1. Introduction* The Hilbert space theory of dissipative operators1 was motivated by the Cauchy problem for systems of hyperbolic partial differential equations (see [5]), where a consideration of the energy of, say, an electromagnetic field leads to an L2 measure as the natural norm for the wave equation. However there are many interesting initial value problems in the theory of partial differential equations whose natural setting is not a Hilbert space, but rather a Banach space. Thus for the heat equation the natural measure is the supremum of the temperature whereas in the case of the diffusion equation the natural measure is the total mass given by an Lx norm. In the present paper a suitable extension of the theory of dissipative operators to arbitrary Banach spaces is initiated. An operator A with domain ®(A) contained in a Hilbert space H is called dissipative if (1.1) re(Ax, x) ^ 0 , x e ®(A) , and maximal dissipative if it is not the proper restriction of any other dissipative operator. As shown in [5] the maximal dissipative operators with dense domains precisely define the class of generators of strongly continuous semi-groups of contraction operators (i.e. bounded operators of norm =§ 1). In the case of the wave equation this furnishes us with a description of all solutions to the Cauchy problem for which the energy is nonincreasing in time. -
Resolvent and Polynomial Numerical Hull
Helsinki University of Technology Institute of Mathematics Research Reports Espoo 2008 A546 RESOLVENT AND POLYNOMIAL NUMERICAL HULL Olavi Nevanlinna AB TEKNILLINEN KORKEAKOULU TEKNISKA HÖGSKOLAN HELSINKI UNIVERSITY OF TECHNOLOGY TECHNISCHE UNIVERSITÄT HELSINKI UNIVERSITE DE TECHNOLOGIE D’HELSINKI Helsinki University of Technology Institute of Mathematics Research Reports Espoo 2008 A546 RESOLVENT AND POLYNOMIAL NUMERICAL HULL Olavi Nevanlinna Helsinki University of Technology Faculty of Information and Natural Sciences Department of Mathematics and Systems Analysis Olavi Nevanlinna: Resolvent and polynomial numerical hull; Helsinki University of Technology Institute of Mathematics Research Reports A546 (2008). Abstract: Given any bounded operator T in a Banach space X we dis- cuss simple approximations for the resolvent (λ − T )−1, rational in λ and polynomial in T . We link the convergence speed of the approximation to the Green’s function for the outside of the spectrum of T and give an application to computing Riesz projections. AMS subject classifications: 47A10, 47A12, 47A66 Keywords: resolvent operator, spectrum, polynomial numerical hull, numerical range, quasialgebraic operator, Riesz projection Correspondence Olavi Nevanlinna Helsinki University of Technology Institute of Mathematics P.O. Box 1100 FI-02015 TKK Finland olavi.nevanlinna@tkk.fi ISBN 978-951-22-9406-0 (print) ISBN 978-951-22-9407-7 (PDF) ISSN 0784-3143 (print) ISSN 1797-5867 (PDF) Helsinki University of Technology Faculty of Information and Natural Sciences Department of Mathematics and Systems Analysis P.O. Box 1100, FI-02015 TKK, Finland email: math@tkk.fi http://math.tkk.fi/ 1 Introduction Let T be a bounded operator in a complex Banach space X and denote by σ(T ) its spectrum. -
Limiting Absorption Principle for Some Long Range Perturbations of Dirac Systems at Threshold Energies
LIMITING ABSORPTION PRINCIPLE FOR SOME LONG RANGE PERTURBATIONS OF DIRAC SYSTEMS AT THRESHOLD ENERGIES NABILE BOUSSAID AND SYLVAIN GOLENIA´ Abstract. We establish a limiting absorption principle for some long range perturbations of the Dirac systems at threshold energies. We cover multi-center interactions with small coupling constants. The analysis is reduced to studying a family of non-self-adjoint operators. The technique is based on a positive commutator theory for non self-adjoint operators, which we develop in appendix. We also discuss some applications to the dispersive Helmholtz model in the quantum regime. Contents 1. Introduction 1 2. Reduction of the problem 5 2.1. The non self-adjoint operator 5 2.2. From one limiting absorption principle to another 7 3. Positive commutator estimates. 9 4. Main result 12 Appendix A. Commutator expansions. 14 Appendix B. A non-selfadjoint weak Mourre theory 16 Appendix C. Application to non-relativistic dispersive Hamiltonians 19 References 20 1. Introduction We study properties of relativistic massive charged particles with spin-1=2 (e.g., electron, positron, (anti-)muon, (anti-)tauon,:::). We follow the Dirac formalism, see [17]. Because of the spin, the configu- ration space of the particle is vector valued. To simplify, we consider finite dimensional and trivial fiber. Let ≥ 2 be an integer. The movement of the free particle is given by the Dirac equation, @' i = D '; in L2( 3; 2 ); ~ @t m R C where m > 0 is the mass, c the speed of light, ~ the reduced Planck constant, and 3 2 X 2 (1.1) Dm := c~ ⋅ P + mc = −ic~ k@k + mc : k=1 Here we set := ( 1; 2; 3) and := 4. -
Weak Operator Topology, Operator Ranges and Operator Equations Via Kolmogorov Widths
Weak operator topology, operator ranges and operator equations via Kolmogorov widths M. I. Ostrovskii and V. S. Shulman Abstract. Let K be an absolutely convex infinite-dimensional compact in a Banach space X . The set of all bounded linear operators T on X satisfying TK ⊃ K is denoted by G(K). Our starting point is the study of the closure WG(K) of G(K) in the weak operator topology. We prove that WG(K) contains the algebra of all operators leaving lin(K) invariant. More precise results are obtained in terms of the Kolmogorov n-widths of the compact K. The obtained results are used in the study of operator ranges and operator equations. Mathematics Subject Classification (2000). Primary 47A05; Secondary 41A46, 47A30, 47A62. Keywords. Banach space, bounded linear operator, Hilbert space, Kolmogorov width, operator equation, operator range, strong operator topology, weak op- erator topology. 1. Introduction Let K be a subset in a Banach space X . We say (with some abuse of the language) that an operator D 2 L(X ) covers K, if DK ⊃ K. The set of all operators covering K will be denoted by G(K). It is a semigroup with a unit since the identity operator is in G(K). It is easy to check that if K is compact then G(K) is closed in the norm topology and, moreover, sequentially closed in the weak operator topology (WOT). It is somewhat surprising that for each absolutely convex infinite- dimensional compact K the WOT-closure of G(K) is much larger than G(K) itself, and in many cases it coincides with the algebra L(X ) of all operators on X . -
Spectrum (Functional Analysis) - Wikipedia, the Free Encyclopedia
Spectrum (functional analysis) - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Spectrum_(functional_analysis) Spectrum (functional analysis) From Wikipedia, the free encyclopedia In functional analysis, the concept of the spectrum of a bounded operator is a generalisation of the concept of eigenvalues for matrices. Specifically, a complex number λ is said to be in the spectrum of a bounded linear operator T if λI − T is not invertible, where I is the identity operator. The study of spectra and related properties is known as spectral theory, which has numerous applications, most notably the mathematical formulation of quantum mechanics. The spectrum of an operator on a finite-dimensional vector space is precisely the set of eigenvalues. However an operator on an infinite-dimensional space may have additional elements in its spectrum, and may have no eigenvalues. For example, consider the right shift operator R on the Hilbert space ℓ2, This has no eigenvalues, since if Rx=λx then by expanding this expression we see that x1=0, x2=0, etc. On the other hand 0 is in the spectrum because the operator R − 0 (i.e. R itself) is not invertible: it is not surjective since any vector with non-zero first component is not in its range. In fact every bounded linear operator on a complex Banach space must have a non-empty spectrum. The notion of spectrum extends to densely-defined unbounded operators. In this case a complex number λ is said to be in the spectrum of such an operator T:D→X (where D is dense in X) if there is no bounded inverse (λI − T)−1:X→D. -
Hermitian Geometry on Resolvent Set
Hermitian geometry on resolvent set (I) Ronald G. Douglas and Rongwei Yang Abstract. For a tuple A = (A1, A2, ..., An) of elements in a unital Banach n algebra B, its projective joint spectrum P (A) is the collection of z ∈ C such that A(z)= z1A1 + z2A2 + · · · + znAn is not invertible. It is known that the −1 B-valued 1-form ωA(z) = A (z)dA(z) contains much topological informa- c tion about the joint resolvent set P (A). This paper studies geometric properties c of P (A) with respect to Hermitian metrics defined through the B-valued fun- ∗ damental form ΩA = −ωA ∧ ωA and its coupling with faithful states φ on B, i.e. φ(ΩA). The connection between the tuple A and the metric is the main subject of this paper. In particular, it shows that the K¨ahlerness of the metric is tied with the commutativity of the tuple, and its completeness is related to the Fuglede-Kadison determinant. Mathematics Subject Classification (2010). Primary 47A13; Secondary 53A35. Keywords. Maurer-Cartan form, projective joint spectrum, Hermitian metric, arXiv:1608.05990v4 [math.FA] 27 Feb 2020 Ricci tensor, Fuglede-Kadison determinant. 0. Introduction In [4], Cowen and the first-named author introduced geometric concepts such as holomorphic bundle and curvature into Operator Theory. This gave rise to complete and computable invariants for certain operators with rich spectral structure, i.e, the Cowen-Douglasoperators. The idea was extended to multivariable cases in the study of Hilbert modules in analytic function spaces, where curvature invariant is defined for some canonical tuples of commuting operators. -
Topological Results About the Set of Generalized Rhaly Matrices 1
Gen. Math. Notes, Vol. 17, No. 1, July 2013, pp. 1-7 ISSN 2219-7184; Copyright c ICSRS Publication, 2013 www.i-csrs.org Available free online at http://www.geman.in Topological Results About the Set of Generalized Rhaly Matrices Nuh Durna1 and Mustafa Yildirim2 1;2 Cumhuriyet University, Faculty of Sciences Department of Mathematics, 58140 Sivas, Turkey 1 E-mail: [email protected] 2 E-mail: [email protected]; [email protected] (Received: 1-2-12 / Accepted: 15-5-13) Abstract In this paper, we will investigate some topological properties of Rb set of all bounded generalized Rhally matrices given by b sequences in H2. We will show 2 that Rb is closed subspace of B (H ) and we will define an operator from T to Rb and show that this operator is injective and continuous in strong-operator topology. Keywords: Generalized Rhaly operators, weak-operator topology, strong- operator topology. 1 Introduction A Hilbert space has two useful topologies (weak and strong); the space of operators on a Hilbert space has several. The metric topology induced by the norm is one of them; to distinguish it from the others, it is usually called the norm topology or the uniform topology. The next two are natural outgrowths for operators of the strong and weak topologies for vectors. A subbase for the strong operator topology is the collection of all sets of the form fA : k(A − A0) fk < g ; correspondingly a base is the collection of all sets of the form fA : k(A − A0) fik < , i = 1; 2; : : : ; kg 2 Nuh Durna et al.