Spectral Theory of Self-Adjoint Ordinary Differential Operators

Total Page:16

File Type:pdf, Size:1020Kb

Spectral Theory of Self-Adjoint Ordinary Differential Operators University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 12-1958 Spectral Theory of Self-Adjoint Ordinary Differential Operators Charles C. Oehring University of Tennessee - Knoxville Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Mathematics Commons Recommended Citation Oehring, Charles C., "Spectral Theory of Self-Adjoint Ordinary Differential Operators. " PhD diss., University of Tennessee, 1958. https://trace.tennessee.edu/utk_graddiss/2951 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Charles C. Oehring entitled "Spectral Theory of Self-Adjoint Ordinary Differential Operators." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Mathematics. F. A. Ficken, Major Professor We have read this dissertation and recommend its acceptance: Leo Simons, Walter Snyder, O. M. Harrod, D. D. Lillian Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) November 24, 1958 To the Graduat e Council: I am submitting herewith a thesis written by Charles c. Oehring entitled "Spectral Theory of Self-Adjoint Ordinar,y Differential Operators ." I recommend that it be accepted in partial fulfillment of the requirements for the degree of Doctor of Philosophy, with a major in Ma thematics. Major Professor We have read this thesis and recommend its acceptance: L��� � (f). 11. I�.). 'Q.IJ_Lf?s- ._. Accepted for the Council:· 4UJ Dean of the!'4:rL� uate SFOOJ. - SPECTRAL 'mEORY OF SELF-ADJOINT ORDINARY DIFFERENTIAL OPERATORS A 'IHESIS Submitted to The Graduate Council of �Ihe University of Tennessee in Partial Fulfillment o! the Requirements for the degree of Doctor of Philosophy' Charles Co Oehring December 1958 ACKNOWLEDGMENT 'lbe author wishes to express his thanks to Professor F. A. Ficken for his assistance in the preparation of this paper. 457.724 TABLE OP CONTEN'IS CHAPTER PAGE IN 'ffiODUCTION . • • • • • • • • • iv I. PRELIMINARIES • • . • 0 • • • • • • 1 Linear operators; spectral representation of self-adj oint operators • • • • • • • • o • • • • • • • • • • • 1 Generalized direct sums of Hilbert spaces • • • • • • • • 3 Differential Operators • • • • • • • • • • • • • • • • • 6 .n. THE �XPANSION 'IHEOREM AND PARS EVAL EQUALITr •••••••• 10 Lenuna • • . • • • • 25 Theorem • • • • • • • • • • 32 Corollary to �eorem 2.64 •• . 40 rn. BOUNDARY CONDITIONS • • • • • • • . • • • 42 EXTENSIOOS SYMME'IRIC IV. SPEC'IRA OF SELF-ADJOINT OF A OP ERA'IUR 49 Von Neumann's theory of symmetric extensions • • • • • • 49 �e �pee� of __a �el�-adjoint operator ••• • • • • • • 51 _ Spectra of self-adjoint extensions • • • • • • • • • • • 51 BIBLIOCB..APHY • • .. • • • • • • • • • • • • • • • • • . 56 IN 'lRODUCTION Many of the properties of the ordinary Fourier seri es expansion of a given function are shared by the orthogonal expansions in terms of eigenfunctions of a second order ordinary differential operator. Let p • p(x) and q • q(x) be real-valued functions such that p , p' , and q are continuous, and p(x) 0 on a .f'inite interval ? , a � x � b • Le� � be a C<?JUplex p�ameter. The classical Sturm­ 1 Liouville theory [9, section 27; 4, Chapter 7; 211 Chapter 1] is con- cerned with solutions or the differential equation � y , -(py•)' + Cf7 • which satisfy certain real boundary conditions whose form need not be given here. These solutions, the so-called eigenfunctions, exist only tor certain values of , the corresponding eigenvalues. The St .A urm- Liouville theory states that the eigenvalues constitute a countable set of rea1 numbers which cluster only at • The corresponding + oo eigenfUnctions constitute an orthogonal system on [a,b] whieh is com- . 2': plete in L (a,b) • . 'lhus the Parseval relation is also valid. now the possibilities a � and b • are allowed• It • - + oc or if the restriction p(x) 0 is required merely for a b , > <: x <: the complexity of the situation increases. In these cases the problem is called singular, in contrast to the regular case considered above. lwumbere in brackets refer to the bibliography at the end of this paper. To obtain satisfactory analogues of the completeness and Parseval theorems, i� now becomes necessar.y to replace the series expansion of an arbitrar.y 2 function in L (a,b) by an expansion in terms of a Stieltjes integral. 'lhe singtil_ar·case has been treated exhaustively by Weyl [23J24], by Stone [20] who uses the general theory of unb ounded symmetric operators, by . Tltchmarsh [21] who uses function theoretic methods, by Kodaira [10] who combines and simplifies the ideas of Weyl and Stone, by Yosida_ [2$], and [13Jlh] as limi.ting b7- Levineon. who obtains results cases of theorems valid for compact subintervals of (a,b) • '!he basic facts in the regular ease extend verbatim to a formally se�f��djoint �iff�rent�al operator L (see Chapter I) of arbitrar.y order n , with complex coefficients defined on a compact interval, provided the th coefficient of the n order derivative does not vanish on that interval [�J.. Chapter 7]. Proofs in this case require no�ing more than the �ilbert­ ' Schmidt theory of integral equations . When the problem is singular, general results have been obtained nly rece tly Glazman [.5] has general­ _ o n . ized several important_r�sults of Weyl and Stone conce�ning the nature or the boundary conditions when the coefficients are real. Kodaira [11] has also discussed boundar,y conditions in the case of real coefficients and an of and proved the alogues the completeness. Parseval relations. Coddington [2] and Lev.i.nson [15] have considered these questions when the co�f.fieients are complex and haTe obtained the expansion and Parseval theorems in two important cases. In these cases they also prove the in- verse transform theorem which is the analogue of the Riesz..;Fiseher theo­ rem in the !heory of ordinary Fourier series. One of the mai.n results or the present paper is a proof, in Chap- vi ter II, of the expansion, Parseval, and inverse transform theorems, by use of the �eor.y of generalized direct sums of Hilbert spaces, which theory - .�· � is due to von Ne These theorems are most elegantly sta e in a umann [22]. t d - . .. ro:m g1v n them by Kodaira Let be Hermiti n non­ � [10]. (fjk) an a , decreasing n by n matrix whose elements are Lebesgue-Btieltjes measures -· - - on the real A axis, (see Chapter • Let and be n-vactor ./'). II) "X w . --- valued i th co fUnctions or A vi th mponent �i (A) and t.Ui (A) res­ pect1Tel7. If we introduce the inner product n - (w,'X.) • { I... Wj(A.)I (}I.)d/' (�), j,k•1 \ jk it is easy to see that the set -"1- of those uJ for which (w,w) <:. oo becomes Hilbert space in this inner product. The expansion, Parsev l a a 9 and inverse transform theorems may then be stated as the following theorem, which will be proved in ·- Chapter. IIo If L is a formally self-adjoint differential operator of order n , and if H is self- j int extension of L in the Hilbert space a ad o - . L 2 (a, b) , then corresponding to each system of linearly independent sol u- ti?�• ( x, i\) j • 11 o o. or Ly·• Ay on (a, b) , ·there exists sj 9 n, a spectral matri x (/'jk) , with the properties described aboveg· su�h . that the as s ci ted Hilbert space is unitarily equivalent L 2 (a,b) o o a -rL to Thus if u L2'(a,b) and is its image in 1 the Parseval £ w JL equality vii 2 is valid. 1he fact that to each w in JL.. corresponds a u E, t (a,b) is the content of the inverse transform theorem. Finally the expansion theorem, the analogue of the completeness theorem in the regular case, states that u and W are related by the specific formulas and n u(x) • f.._ Bj(·x,A) uJk{l,)d i'A) 1 j,Lk-1 ft where the fi rst integral converges in the norm of _n_ and the second in the norm of L2(a,b) • Chapter I contains definitions and facts pertinent to later chap- ters. In Chapter III a generali zation, with a different proof, is given of a theorem of Coddington [-2, 'lheorem 3] which characterizes the self- adjoint extensions of L , when such extensions exist, in terms of cer- tain boundary conditions. !t is shown in Chapter that a theorem of Hartman an ·- . IV d Wintner [7] .concerning the eigenvalues of L in one of the eases considered by Weyl is aetua1ly valid in a much more general setting . viii the o the the a Since printing f text of this paper uthor has noted the appearance in the Canadian Journal of Mathematics, Vol. I, No. 3 (1958), of by F. Brauer which the gen n ppo -���-�6, a paper in ei functio expansion problem is treated using the method of generalized direct sums of Hilbert spaces. Brauer's approach to the problem is very similar to the one used e present paperJ in th -- and in .faet he proves the analogues of the main re- sul of Theorem 2.64 tor the eigeDTalue problem Lu • where . ts -- - 7\ Mu 1 L and M o i s�lf-adjoint differential operators and is semi- - are.
Recommended publications
  • The Notion of Observable and the Moment Problem for ∗-Algebras and Their GNS Representations
    The notion of observable and the moment problem for ∗-algebras and their GNS representations Nicol`oDragoa, Valter Morettib Department of Mathematics, University of Trento, and INFN-TIFPA via Sommarive 14, I-38123 Povo (Trento), Italy. [email protected], [email protected] February, 17, 2020 Abstract We address some usually overlooked issues concerning the use of ∗-algebras in quantum theory and their physical interpretation. If A is a ∗-algebra describing a quantum system and ! : A ! C a state, we focus in particular on the interpretation of !(a) as expectation value for an algebraic observable a = a∗ 2 A, studying the problem of finding a probability n measure reproducing the moments f!(a )gn2N. This problem enjoys a close relation with the selfadjointness of the (in general only symmetric) operator π!(a) in the GNS representation of ! and thus it has important consequences for the interpretation of a as an observable. We n provide physical examples (also from QFT) where the moment problem for f!(a )gn2N does not admit a unique solution. To reduce this ambiguity, we consider the moment problem n ∗ (a) for the sequences f!b(a )gn2N, being b 2 A and !b(·) := !(b · b). Letting µ!b be a n solution of the moment problem for the sequence f!b(a )gn2N, we introduce a consistency (a) relation on the family fµ!b gb2A. We prove a 1-1 correspondence between consistent families (a) fµ!b gb2A and positive operator-valued measures (POVM) associated with the symmetric (a) operator π!(a). In particular there exists a unique consistent family of fµ!b gb2A if and only if π!(a) is maximally symmetric.
    [Show full text]
  • Asymptotic Spectral Measures: Between Quantum Theory and E
    Asymptotic Spectral Measures: Between Quantum Theory and E-theory Jody Trout Department of Mathematics Dartmouth College Hanover, NH 03755 Email: [email protected] Abstract— We review the relationship between positive of classical observables to the C∗-algebra of quantum operator-valued measures (POVMs) in quantum measurement observables. See the papers [12]–[14] and theB books [15], C∗ E theory and asymptotic morphisms in the -algebra -theory of [16] for more on the connections between operator algebra Connes and Higson. The theory of asymptotic spectral measures, as introduced by Martinez and Trout [1], is integrally related K-theory, E-theory, and quantization. to positive asymptotic morphisms on locally compact spaces In [1], Martinez and Trout showed that there is a fundamen- via an asymptotic Riesz Representation Theorem. Examples tal quantum-E-theory relationship by introducing the concept and applications to quantum physics, including quantum noise of an asymptotic spectral measure (ASM or asymptotic PVM) models, semiclassical limits, pure spin one-half systems and quantum information processing will also be discussed. A~ ~ :Σ ( ) { } ∈(0,1] →B H I. INTRODUCTION associated to a measurable space (X, Σ). (See Definition 4.1.) In the von Neumann Hilbert space model [2] of quantum Roughly, this is a continuous family of POV-measures which mechanics, quantum observables are modeled as self-adjoint are “asymptotically” projective (or quasiprojective) as ~ 0: → operators on the Hilbert space of states of the quantum system. ′ ′ A~(∆ ∆ ) A~(∆)A~(∆ ) 0 as ~ 0 The Spectral Theorem relates this theoretical view of a quan- ∩ − → → tum observable to the more operational one of a projection- for certain measurable sets ∆, ∆′ Σ.
    [Show full text]
  • ASYMPTOTICALLY ISOSPECTRAL QUANTUM GRAPHS and TRIGONOMETRIC POLYNOMIALS. Pavel Kurasov, Rune Suhr
    ISSN: 1401-5617 ASYMPTOTICALLY ISOSPECTRAL QUANTUM GRAPHS AND TRIGONOMETRIC POLYNOMIALS. Pavel Kurasov, Rune Suhr Research Reports in Mathematics Number 2, 2018 Department of Mathematics Stockholm University Electronic version of this document is available at http://www.math.su.se/reports/2018/2 Date of publication: Maj 16, 2018. 2010 Mathematics Subject Classification: Primary 34L25, 81U40; Secondary 35P25, 81V99. Keywords: Quantum graphs, almost periodic functions. Postal address: Department of Mathematics Stockholm University S-106 91 Stockholm Sweden Electronic addresses: http://www.math.su.se/ [email protected] Asymptotically isospectral quantum graphs and generalised trigonometric polynomials Pavel Kurasov and Rune Suhr Dept. of Mathematics, Stockholm Univ., 106 91 Stockholm, SWEDEN [email protected], [email protected] Abstract The theory of almost periodic functions is used to investigate spectral prop- erties of Schr¨odinger operators on metric graphs, also known as quantum graphs. In particular we prove that two Schr¨odingeroperators may have asymptotically close spectra if and only if the corresponding reference Lapla- cians are isospectral. Our result implies that a Schr¨odingeroperator is isospectral to the standard Laplacian on a may be different metric graph only if the potential is identically equal to zero. Keywords: Quantum graphs, almost periodic functions 2000 MSC: 34L15, 35R30, 81Q10 Introduction. The current paper is devoted to the spectral theory of quantum graphs, more precisely to the direct and inverse spectral theory of Schr¨odingerop- erators on metric graphs [3, 20, 24]. Such operators are defined by three parameters: a finite compact metric graph Γ; • a real integrable potential q L (Γ); • ∈ 1 vertex conditions, which can be parametrised by unitary matrices S.
    [Show full text]
  • Lecture Notes on Spectra and Pseudospectra of Matrices and Operators
    Lecture Notes on Spectra and Pseudospectra of Matrices and Operators Arne Jensen Department of Mathematical Sciences Aalborg University c 2009 Abstract We give a short introduction to the pseudospectra of matrices and operators. We also review a number of results concerning matrices and bounded linear operators on a Hilbert space, and in particular results related to spectra. A few applications of the results are discussed. Contents 1 Introduction 2 2 Results from linear algebra 2 3 Some matrix results. Similarity transforms 7 4 Results from operator theory 10 5 Pseudospectra 16 6 Examples I 20 7 Perturbation Theory 27 8 Applications of pseudospectra I 34 9 Applications of pseudospectra II 41 10 Examples II 43 1 11 Some infinite dimensional examples 54 1 Introduction We give an introduction to the pseudospectra of matrices and operators, and give a few applications. Since these notes are intended for a wide audience, some elementary concepts are reviewed. We also note that one can understand the main points concerning pseudospectra already in the finite dimensional case. So the reader not familiar with operators on a separable Hilbert space can assume that the space is finite dimensional. Let us briefly outline the contents of these lecture notes. In Section 2 we recall some results from linear algebra, mainly to fix notation, and to recall some results that may not be included in standard courses on linear algebra. In Section 4 we state some results from the theory of bounded operators on a Hilbert space. We have decided to limit the exposition to the case of bounded operators.
    [Show full text]
  • 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.
    [Show full text]
  • Functional Analysis—Spectral Theory in Hilbert Space
    Functional analysis—spectral theory in Hilbert space J. B. Cooper Johannes Kepler Universit¨at Linz Contents 1 Spectral theory in Hilbert space—the classical approach 2 2 Banach algebras 10 3 The spectral theorem—abstract approach 29 4 The spectral theory – unbounded operators 36 1 1 Spectral theory in Hilbert space—the clas- sical approach Introduction In these notes we consider one of the most attractive and im- portant results from the theory of functional analysis – the spectral theorem for self-adjoint operators on Hilbert space. This is an infinite dimensional analogue of the classical result on the diagonalisation of hermitian matrices which, in turn, has its origin one of the climaxes of Greek mathematics – the study of conic sections. In the process of his work on integral equations, Hilbert showed that for operators on L2 which are defined by summetric ker- nels, an exact analogue of the finite dimensional results can be obtained – more precisely the space is spanned by an orthonormal basis consisting of eigenvectors of the operator and in fact he classical function systems which played such a central role in the mathematics of the nineteenth century arise in this way. Later, partly motivated by the needs of quantum theory (where non bounded self-adjoint operators appear as observables), the theory was generalised to operators on Hilbert space, which are not necessarily bounded. For such operators, the spectrum need no longer be compact and eigenvec- tors need no longer exist so that the final form of the theorem is necessarily more abstract and complex. We begin with a direct proof of the spectral theorem for bounded opera- tors in Section 1.
    [Show full text]
  • Spectral Theory
    Spectral Theory Kim Klinger-Logan November 25, 2016 Abstract: The following is a collection of notes (one of many) that compiled in prepa- ration for my Oral Exam which related to spectral theory for automorphic forms. None of the information is new and it is rephrased from Rudin's Functional Analysis, Evans' Theory of PDE, Paul Garrett's online notes and various other sources. Background on Spectra To begin, here is some basic terminology related to spectral theory. For a continuous linear operator T 2 EndX, the λ-eigenspace of T is Xλ := fx 2 X j T x = λxg: −1 If Xλ 6= 0 then λ is an eigenvalue. The resolvent of an operator T is (T − λ) . The resolvent set ρ(T ) := fλ 2 C j λ is a regular value of T g: The value λ is said to be a regular value if (T − λ)−1 exists, is a bounded linear operator and is defined on a dense subset of the range of T . The spectrum of is the collection of λ such that there is no continuous linear resolvent (inverse). In oter works σ(T ) = C − ρ(T ). spectrum σ(T ) := fλ j T − λ does not have a continuous linear inverseg discrete spectrum σdisc(T ) := fλ j T − λ is not injective i.e. not invertibleg continuous spectrum σcont(T ) := fλ j T −λ is not surjective but does have a dense imageg residual spectrum σres(T ) := fλ 2 σ(T ) − (σdisc(T ) [ σcont(T ))g Bounded Operators Usually we want to talk about bounded operators on Hilbert spaces.
    [Show full text]
  • Spectral Geometry Bruno Iochum
    Spectral Geometry Bruno Iochum To cite this version: Bruno Iochum. Spectral Geometry. A. Cardonna, C. Neira-Jemenez, H. Ocampo, S. Paycha and A. Reyes-Lega. Spectral Geometry, Aug 2011, Villa de Leyva, Colombia. World Scientific, 2014, Geometric, Algebraic and Topological Methods for Quantum Field Theory, 978-981-4460-04-0. hal- 00947123 HAL Id: hal-00947123 https://hal.archives-ouvertes.fr/hal-00947123 Submitted on 14 Feb 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Spectral Geometry Bruno Iochum Aix-Marseille Université, CNRS UMR 7332, CPT, 13288 Marseille France Abstract The goal of these lectures is to present some fundamentals of noncommutative geometry looking around its spectral approach. Strongly motivated by physics, in particular by relativity and quantum mechanics, Chamseddine and Connes have defined an action based on spectral considerations, the so-called spectral action. The idea here is to review the necessary tools which are behind this spectral action to be able to compute it first in the case of Riemannian manifolds (Einstein–Hilbert action). Then, all primary objects defined for manifolds will be generalized to reach the level of noncommutative geometry via spectral triples, with the concrete analysis of the noncommutative torus which is a deformation of the ordinary one.
    [Show full text]
  • Rigged Hilbert Spaces
    Chapter 4 Rigged Hilbert Spaces A considerable part of functional analysis, including the theory of linear operators, particularly the spectral theory, cannot be presented successively without the no- tion of a rigged Hilbert space. The use of the method of rigged spaces allows one to beyond the setting with two starting objects, a single Hilbert space H and an operator A on H. To provide a complete picture of the spectral properties for A in the general case, it is necessary to equip the space H with an additional couple of Hilbert (or topological) spaces in a specific way. So, in a natural way there appear ∗ the triples of embedding spaces of a view H− ⊃H⊃H+, (or Φ ⊃H⊃Φ). In this book we will restrict our attention to the Hilbert equipping which form the so-called rigged Hilbert spaces. In the most advanced approach (see [42] and references therein) it is assumed that Dom A is a part of some positive Hilbert space H+, which is continuously embedded into H. Then the generalized eigen-functions of the operator A belong to the negative space H− which extends H. This approach proved its success in a wide class of various problems of mathematical physics, the theory of differential operators, and, especially, in the infinite-dimensional analysis (see, e.g., [45]). In this chapter we describe the standard construction of the rigged Hilbert space following to the detail presentation in Berezansky’s books [42, 44] (see also [48]). In addition, we will briefly analyze the properties of the A-scale of Hilbert spaces which will be used in that follows.
    [Show full text]
  • Spectral Theory
    Spectral Theory Michael E. Taylor Contents 0. Introduction 1. The spectral theorem 2. Self-adjoint differential operators 3. Heat asymptotics and eigenvalue asymptotics 4. The Laplace operator on Sn 5. The Laplace operator on hyperbolic space 6. The harmonic oscillator 7. The quantum Coulomb problem 8. The Laplace operator on cones Introduction This chapter is devoted to the spectral theory of self-adjoint, differential operators. We cover a number of different topics, beginning in x1 with a proof of the spectral theorem. It was an arbitrary choice to put that material here, rather than in Appendix A, on functional analysis. The main motivation for putting it here is to begin a line of reasoning that will be continued in subsequent sections, using the great power of studying unitary groups as a tool in spectral theory. After we show how easily this study leads to a proof of the spectral theorem in x1, in later sections we use it in various ways: as a tool to establish self-adjointness, as a tool for obtaining specific formulas, including basic identities among special functions, and in other capacities. Sections 2 and 3 deal with some general questions in spectral theory, such as when does a differential operator define a self-adjoint operator, when does it have a compact resolvent, and what asymptotic properties does its spectrum have? We tackle the latter question, for the Laplace operator ∆, by examining the asymptotic behavior of the trace of the solution operator et∆ for the heat equation, showing that (0.1) Tr et∆ = (4πt)−n=2 vol Ω + o(t−n=2); t & 0; when Ω is either a compact Riemannian manifold or a bounded domain in Rn (and has the Dirichlet boundary condition).
    [Show full text]
  • Chapter 6: Spectral Theory Overview
    Spectral Theory: Overview 6-1 Chapter 6: Spectral Theory Overview Intuitive approach to stability: two viewpoints for study of stability, linearization • and Lagrangian reduction; [ book: Sec. 6.1 ] Force operator formalism: equation of motion, Hilbert space, self-adjointness of • the force operator; [ book: Sec. 6.2 ] Quadratic forms and variational principles: expressions for the potential energy, • different variational principles, the energy principle; [ book: Sec. 6.4 ] Further spectral issues: returning to the two viewpoints; [ book: Sec. 6.5 ] • Extension to interface plasmas: boundary conditions, extended variational princi- • ples, Rayleigh–Taylor instability. [ book: Sec. 6.6 ] Spectral Theory: Intuitive approach to stability (1) 6-2 Two viewpoints How does one know whether a dynamical system is stable or not? • W0 a b W1 Energy W1 W0 ξ ξ Force F F stable unstable Method: split the non-linear problem in static equilibrium (no flow) and small (linear) • time-dependent perturbations. Two approaches: exploiting variational principles involving quadratic forms (energy), • or solving the partial differential equations themselves (forces). Spectral Theory: Intuitive approach to stability (2) 6-3 Aside: nonlinear stability Distinct from linear stability, involves finite amplitude displacements: • (a) system can be linearly stable, nonlinearly unstable; (b) system can be linearly unstable, nonlinearly stable (e.g. evolving towards the equilibrium states 1 or 2). a b 1 2 Quite relevant for topic of magnetic confinement, but too complicated at this stage. • Spectral Theory: Intuitive approach to stability (3) 6-4 Linearization Start from ideal MHD equations: • ∂v ρ( + v v) = p + j B ρ Φ , j = B , (1) ∂t · ∇ −∇ × − ∇ ∇× ∂p = v p γp v , (2) ∂t − · ∇ − ∇· ∂B = (v B) , B =0 , (3) ∂t ∇× × ∇· ∂ρ = (ρv) .
    [Show full text]
  • And Singular Values)
    Finite-dimensional spectral theory part II: understanding the spectrum (and singular values) Ed Bueler MATH 617 Functional Analysis Spring 2020 Ed Bueler (MATH 617) Finite-dimensional spectral theory II Spring 2020 1 / 41 Outline 1 introduction 2 functional calculus 3 resolvents 4 orthogonal projectors 5 singular value decomposition 6 conclusion Ed Bueler (MATH 617) Finite-dimensional spectral theory II Spring 2020 2 / 41 what happened in part I see part I first: bueler.github.io/M617S20/slides1.pdf definition. for a square matrix A 2 Cn×n, the spectrum is the set σ(A) = λ 2 C Av = λv for some v 6= 0 we proved: ∗ n×n A = QTQ Schur decomposition for any A 2 C A = QΛQ∗ spectral theorem for normal (AA∗ = A∗A) matrices where Q is unitary, T is upper-triangular, and Λ is diagonal ◦ both decompositions “reveal” the spectrum: σ(A) = fdiagonal entries of T or Λg ◦ spectral theorem for hermitian matrices is sometimes called the principal axis decomposition for quadratic forms Ed Bueler (MATH 617) Finite-dimensional spectral theory II Spring 2020 3 / 41 goal for MATH 617 goal extend the spectral theorem to 1-dimensions only possible for linear operators on Hilbert spaces H ◦ inner product needed for adjoints and unitaries ◦ unitary maps needed because they preserve vector space and metric and adjoint structures textbook (Muscat) extends to compact normal operators on H ◦ the spectrum is eigenvalues (almost exclusively) recommended text (B. Hall, Quantum Theory for Mathematicians) extends further to bounded (continuous) normal operators on H ◦ spectrum is not only eigenvalues ◦ statement of theorem uses projector-valued measures Hall also extends to unbounded normal operators on H ◦ but we won’t get there .
    [Show full text]