Evolution Equations Governed by Elliptic Operators Wolfgang Arendt
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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. -
Arxiv:1901.07148V2 [Math.DS] 6 Mar 2020 Uvyo Ohasrc N Oceefaue Fteanalys the of Features Concrete Spect and Real Operators
COMPLEX SYMMETRIC EVOLUTION EQUATIONS PHAM VIET HAI AND MIHAI PUTINAR Abstract. We study certain dynamical systems which leave invari- ant an indefinite quadratic form via semigroups or evolution families of complex symmetric Hilbert space operators. In the setting of bounded operators we show that a C-selfadjoint operator generates a contraction C0-semigroup if and only if it is dissipative. In addition, we exam- ine the abstract Cauchy problem for nonautonomous linear differential equations possessing a complex symmetry. In the unbounded operator framework we isolate the class of complex symmetric, unbounded semi- groups and investigate Stone-type theorems adapted to them. On Fock space realization, we characterize all C-selfadjoint, unbounded weighted composition semigroups. As a byproduct we prove that the generator of a C-selfadjoint, unbounded semigroup is not necessarily C-selfadjoint. 1. Introduction 1.1. Complex symmetric operators. The study of abstract complex sym- metric operators is relatively new, originating in the articles [10, 11], al- though specific classes of these operators and their spectral behavior were investigated for several decades. Notable in this respect is the non-hermitian quantum mechanics formalism; its hamiltonians are complex symmetric, non-selfadjoint in the classical sense, but have real spectrum. See [9] for a survey of both abstract and concrete features of the analysis of complex symmetric operators. We start by recalling some basic terminology, illustrated by a couple of examples. arXiv:1901.07148v2 [math.DS] 6 Mar 2020 Definition 1.1. An unbounded, linear operator T is called C-symmetric on a separable, complex Hilbert space H if there exists a conjugation C (i.e. -
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. -
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. -
An Introduction to Evolution Pdes September 24, 2018
An introduction to evolution PDEs September 24, 2018 CHAPTER 3 - EVOLUTION EQUATION AND SEMIGROUP In this chapter we make the link between the existence theory for evolution PDEs we have presented in the two first chapters and the theory of continuous semigroup of linear and bounded operators. In that unified framework we may establish the Duhamel formula and the extension of the existence theory by perturbation argument. We also briefly present the Hille-Yosida-Lumer-Phillips existence theory for m-dissipative operators. Contents 1. From linear evolution equation to semigroup 1 1.1. Semigroup 1 1.2. From well-posedness to semigroup 2 2. Semigroup and generator 3 3. Duhamel formula and mild solution 6 4. Dual semigroup and weak solution 7 5. Coming back to the well-posedness issue for evolution equations 9 5.1. A perturbation trick 10 5.2. Semilinear evolution equation 11 5.3. Dissipativity and extension trick 13 6. Semigroup Hille-Yosida-Lumer-Phillips' existence theory 14 7. Complements 17 7.1. Continuity 17 7.2. Nonautonomous semigroup 18 7.3. Transport equation in measures and L1 frameworks 20 8. Discussion 21 8.1. Several way to build solutions 21 8.2. From Hille-Yosida theory to variational solutions. 21 8.3. Very weak solution 22 9. Bibliographic discussion 25 1. From linear evolution equation to semigroup 1.1. Semigroup. We state the definition of a continuous semigroup of linear and bounded oper- ators. Definition 1.1. We say that (St)t≥0 is a continuous semigroup of linear and bounded operators on a Banach space X, or we just say -
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. -
Fractional Powers of Non-Densely Defined Operators
ANNALI DELLA SCUOLA NORMALE SUPERIORE DI PISA Classe di Scienze CELSO MARTINEZ MIGUEL SANZ Fractional powers of non-densely defined operators Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4e série, tome 18, no 3 (1991), p. 443-454 <http://www.numdam.org/item?id=ASNSP_1991_4_18_3_443_0> © Scuola Normale Superiore, Pisa, 1991, tous droits réservés. L’accès aux archives de la revue « Annali della Scuola Normale Superiore di Pisa, Classe di Scienze » (http://www.sns.it/it/edizioni/riviste/annaliscienze/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Fractional Powers of Non-densely Defined Operators CELSO MARTINEZ - MIGUEL SANZ* 1. - Introduction and notation In [1] Balakrishnan extended the concept of fractional powers to closed linear operators A, defined on a Banach space X, such that ) - oo, 0[ is included in the resolvent set p(A) and the resolvent operator satisfies (Following Komatsu’s terminology in [10], we shall call these operators non- negative). Balakrishnan defined the power with base A and exponent a complex number a (Re a > 0) as the closure of a closable operator, JA, whose expression is: and and For ) and , For ) and , * Partially supported by D.G.C.Y.T., grant PS88-0115. Spain. Pervenuto alla Redazione il 25 Giugno 1990 e in forma definitiva il 13 Marzo 1991. -
Semigroups of Linear Operators
Semigroups of Linear Operators Sheree L. LeVarge December 4, 2003 Abstract This paper will serve as a basic introduction to semigroups of linear operators. It will define a semigroup in the context of a physical problem which will serve to motivate further (elementary) theoretical development of linear semigroups including the Hille- Yosida Theorem. Applications and examples will also be discussed. 1 Introduction Before defining what a semigroup is, one needs to recognize their global importance. Of course their importance cannot be fully realized until we have a clear definition and developed theory. However, in general, semigroups can be used to solve a large class of problems commonly known as evolution equations. These types of equations appear in many disciplines including physics, chemistry, biology, engineering, and economics. They are usually described by an initial value problem (IVP) for a differential equation which can be ordinary or partial. When we view the evolution of a system in the context of semigroups we break it down into transitional steps (i.e. the system evolves from state A to state B, and then from state B to state C). When we recognize that we have a semigroup, instead of studying the IVP directly, we can study it via the semigroup and its applicable theory. The theory of linear semigroups is very well developed [1]. For example, linear semigroup theory actually provides necessary and sufficient conditions to determine the well-posedness of a problem [3]. There is also theory for nonlinear semigroups which this paper will not address. This paper will focus on a special class of linear semigroups called C0 semigroups which are semigroups of strongly continuous bounded linear operators. -
SPECTRAL THEOREM for SYMMETRIC OPERATORS with COMPACT RESOLVENT 1. Compact Operators Let X, Y Be Banach Spaces. a Linear Operato
SPECTRAL THEOREM FOR SYMMETRIC OPERATORS WITH COMPACT RESOLVENT Abstract. These are the letcure notes prepared for the workshop on \Functional Analysis and Operator Algebras" to be held at NIT-Karnataka, during 2-7 June 2014. 1. Compact Operators Let X; Y be Banach spaces. A linear operator T from X into Y is said to be compact if for every bounded sequence fxng in X, fT xng has a convergent subsequence. Lemma 1.1. Compact operators form a subspace of B(X; Y ): Proof. Clearly, a scalar multiple of a compact operator is compact. Suppose S; T are com- pact operators and let fxng be a bounded sequence. Since S is compact, there exists a convergent subsequence fSxnk g of fSxng: Since fxnk g is bounded, by the compactness of T; we get a convergent subsequence fT xn g of fT xng: Thus we obtain a convergent kl subsequence f(S + T )xn g of f(S + T )xng; and hence S + T is compact. kl Remark 1.2 : If S is compact and T is bounded then ST; T S are compact. Thus compact operators actually form an ideal of B(X; Y ): Exercise 1.3 : Show that every finite-rank bounded linear map T : X ! Y is compact. Pk Hint. Note that there exist vectors y1; ··· ; yk 2 Y such that T x = i=1 λi(x)yi; where λ1; ··· ; λk are linear functionals on X. If fxng is bounded then so is each fλi(xn)g: Now apply Heine-Borel Theorem. The following proposition provides a way to generate examples of compact operators which are not necessarily of finite rank.