Comparison Between the Different Definitions of the Essential Spectrum
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Unbounded Jacobi Matrices with a Few Gaps in the Essential Spectrum: Constructive Examples
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Springer - Publisher Connector Integr. Equ. Oper. Theory 69 (2011), 151–170 DOI 10.1007/s00020-010-1856-x Published online January 11, 2011 c The Author(s) This article is published Integral Equations with open access at Springerlink.com 2010 and Operator Theory Unbounded Jacobi Matrices with a Few Gaps in the Essential Spectrum: Constructive Examples Anne Boutet de Monvel, Jan Janas and Serguei Naboko Abstract. We give explicit examples of unbounded Jacobi operators with a few gaps in their essential spectrum. More precisely a class of Jacobi matrices whose absolutely continuous spectrum fills any finite number of bounded intervals is considered. Their point spectrum accumulates to +∞ and −∞. The asymptotics of large eigenvalues is also found. Mathematics Subject Classification (2010). Primary 47B36; Secondary 47A10, 47B25. Keywords. Jacobi matrix, essential spectrum, gaps, asymptotics. 1. Introduction In this paper we look for examples of unbounded Jacobi matrices with sev- 2 2 eral gaps in the essential spectrum. Let 0 = 0(N) be the space of sequences ∞ {fk}1 with a finite number of nonzero coordinates. For given real sequences ∞ ∞ 2 {ak}1 and {bk}1 the Jacobi operator J 0 acts in 0 by the formula (J 0 f)k = ak−1fk−1 + bkfk + akfk+1 (1.1) where k =1, 2, ... and a0 = f0 =0.Theak’s and bk’s are called the weights and diagonal terms, respectively. ∞ In what follows we deal with positive sequences {ak}1 . By Carleman’s 2 2 criterion [1] one can extend J 0 to a self-adjoint operator J in = (N) provided that 1 =+∞. -
The Essential Spectrum of Schr¨Odinger, Jacobi, And
THE ESSENTIAL SPECTRUM OF SCHRODINGER,¨ JACOBI, AND CMV OPERATORS YORAM LAST1;3 AND BARRY SIMON2;3 Abstract. We provide a very general result that identifies the essential spectrum of broad classes of operators as exactly equal to the closure of the union of the spectra of suitable limits at infinity. Included is a new result on the essential spectra when potentials are asymptotic to isospectral tori. We also recover with a unified framework the HVZ theorem and Krein’s results on orthogonal polynomials with finite essential spectra. 1. Introduction One of the most simple but also most powerful ideas in spectral the- ory is Weyl’s theorem, of which a typical application is (in this intro- duction, in order to avoid technicalities, we take potentials bounded): Theorem 1.1. If V; W are bounded functions on Rº and limjxj!1[V (x) ¡ W (x)] = 0, then σess(¡∆ + V ) = σess(¡∆ + W ) (1.1) Our goal in this paper is to find a generalization of this result that allows “slippage” near infinity. Typical of our results are the following: Theorem 1.2. Let V be a bounded periodic function on (¡1; 1) d2 2 and HV the operator ¡ dx2 + V (x) on L (R). For x > 0, define p d2 2 W (x) = V (x + x) and let HW be ¡ dx2 + W (x) on L (0; 1) with some selfadjoint boundary conditions at zero. Then σess(HW ) = σ(HV ) (1.2) Date: March 7, 2005. 1 Institute of Mathematics, The Hebrew University, 91904 Jerusalem, Israel. E- mail: [email protected]. -
Complete Integrability of the Benjamin-Ono Equation on the Multi-Soliton Manifolds Ruoci Sun
Complete integrability of the Benjamin-Ono equation on the multi-soliton manifolds Ruoci Sun To cite this version: Ruoci Sun. Complete integrability of the Benjamin-Ono equation on the multi-soliton manifolds. 2020. hal-02548712 HAL Id: hal-02548712 https://hal.archives-ouvertes.fr/hal-02548712 Preprint submitted on 20 Apr 2020 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. Complete integrability of the Benjamin{Ono equation on the multi-soliton manifolds Ruoci Sun∗y April 20, 2020 Abstract This paper is dedicated to proving the complete integrability of the Benjamin{Ono (BO) equation on the line when restricted to every N-soliton manifold, denoted by UN . We construct gener- alized action{angle coordinates which establish a real analytic symplectomorphism from UN onto some open convex subset of R2N and allow to solve the equation by quadrature for any such initial datum. As a consequence, UN is the universal covering of the manifold of N-gap potentials for the BO equation on the torus as described by G´erard{Kappeler [19]. The global well-posedness of the BO equation in UN is given by a polynomial characterization and a spectral characterization of the manifold UN . -
Spectral Edge Properties of Periodic Elliptic Operators
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Texas A&M Repository SPECTRAL EDGE PROPERTIES OF PERIODIC ELLIPTIC OPERATORS A Dissertation by MINH TUAN KHA Submitted to the Office of Graduate and Professional Studies of Texas A&M University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Chair of Committee, Peter Kuchment Committee Members, Gregory Berkolaiko Kenneth Dykema Valery Pokrovsky Head of Department, Emil Straube August 2017 Major Subject: Mathematics Copyright 2017 Minh Tuan Kha ABSTRACT In this dissertation, we study some spectral problems for periodic elliptic operators arising in solid state physics, material sciences, and differential geometry. More precisely, we are interested in dealing with various effects near and at spectral edges of such opera- tors. We use the name “threshold effects” for the features that depend only on the infinites- imal structure (e.g., a finite number of Taylor coefficients) of the dispersion relation at a spectral edge. We begin with an example of a threshold effect by describing explicitly the asymp- totics of the Green’s function near a spectral edge of an internal gap of the spectrum of a periodic elliptic operator of second-order on Euclidean spaces, as long as the disper- sion relation of this operator has a non-degenerate parabolic extremum there. This result confirms the expectation that the asymptotics of such operators resemble the case of the Laplace operator. Then we generalize these results by establishing Green’s function asymptotics near and at gap edges of periodic elliptic operators on abelian coverings of compact Riemannian manifolds. -
Linear Operators and Their Essential Pseudospectra
Linear Operators and Their Essential Pseudospectra Linear Operators and Their Essential Pseudospectra Aref Jeribi, PhD Department of Mathematics, University of Sfax, Tunisia E-mail: [email protected] Apple Academic Press Inc. Apple Academic Press Inc. 3333 Mistwell Crescent 9 Spinnaker Way Oakville, ON L6L 0A2 Canada Waretown, NJ 08758 USA © 2018 by Apple Academic Press, Inc. Exclusive worldwide distribution by CRC Press, a member of Taylor & Francis Group No claim to original U.S. Government works Printed in the United States of America on acid-free paper International Standard Book Number-13: 978-1-77188-699-4 (Hardcover) International Standard Book Number-13: 978-1-351-04627-5 (eBook) All rights reserved. No part of this work may be reprinted or reproduced or utilized in any form or by any electric, mechanical or other means, now known or hereafter invented, including photocopying and re- cording, or in any information storage or retrieval system, without permission in writing from the publish- er or its distributor, except in the case of brief excerpts or quotations for use in reviews or critical articles. This book contains information obtained from authentic and highly regarded sources. Reprinted material is quoted with permission and sources are indicated. Copyright for individual articles remains with the authors as indicated. A wide variety of references are listed. Reasonable efforts have been made to publish reliable data and information, but the authors, editors, and the publisher cannot assume responsibility for the validity of all materials or the consequences of their use. The authors, editors, and the publisher have attempted to trace the copyright holders of all material reproduced in this publication and apologize to copyright holders if permission to publish in this form has not been obtained. -
Ultra-Weak Time Operators of Schrodinger Operators
Title Ultra-Weak Time Operators of Schrodinger Operators Author(s) Arai, Asao; Hiroshima, Fumio Annales Henri Poincaré, 18(9), 2995-3033 Citation https://doi.org/10.1007/s00023-017-0586-x Issue Date 2017-09 Doc URL http://hdl.handle.net/2115/71420 Rights The final publication is available at link.springer.com Type article (author version) File Information arai-hiroshima-rev.pdf Instructions for use Hokkaido University Collection of Scholarly and Academic Papers : HUSCAP Ultra-Weak Time Operators of SchrÄodinger Operators Asao Arai and Fumio Hiroshima Abstract. In an abstract framework, a new concept on time operator, ultra-weak time operator, is introduced, which is a concept weaker than that of weak time operator. Theorems on the existence of an ultra- weak time operator are established. As an application of the theorems, it is shown that SchrÄodingeroperators HV with potentials V obeying suitable conditions, including the Hamiltonian of the hydrogen atom, have ultra-weak time operators. Moreover, a class of Borel measurable functions f : R ! R such that f(HV ) has an ultra-weak time operator is found. Keywords. Time operators, Weyl relations, CCR, SchrÄodingeroperators. 1. Introduction The present paper concerns a time operator in quantum theory which is de- ¯ned, in a ¯rst stage of cognition, as a symmetric operator canonically con- jugate to a Hamiltonian if it exists. The uncertainty relation which is derived from the canonical commutation relation of a time operator and a Hamil- tonian may be interpreted as a mathematically rigorous form of time-energy uncertainty relation. Moreover time operators may play important roles in quantum phenomena [Miy01, Ara05, Ara08b, AM08b , MME08, MME09]. -
A Spectral Analysis of Linear Operator Pencils on Banach Spaces with Application to Quotient of Bounded Operators
International Journal of Analysis and Applications ISSN 2291-8639 Volume 7, Number 2 (2015), 104-128 http://www.etamaths.com A SPECTRAL ANALYSIS OF LINEAR OPERATOR PENCILS ON BANACH SPACES WITH APPLICATION TO QUOTIENT OF BOUNDED OPERATORS BEKKAI MESSIRDI1;∗, ABDELLAH GHERBI2 AND MOHAMED AMOUCH3 Abstract. Let X and Y two complex Banach spaces and (A; B) a pair of bounded linear operators acting on X with value on Y: This paper is con- cerned with spectral analysis of the pair (A; B): We establish some properties concerning the spectrum of the linear operator pencils A − λB when B is not necessarily invertible and λ 2 C: Also, we use the functional calculus for the pair (A; B) to prove the corresponding spectral mapping theorem for (A; B): In addition, we define the generalized Kato essential spectrum and the closed range spectra of the pair (A; B) and we give some relationships between this spectrums. As application, we describe a spectral analysis of quotient opera- tors. 1. Introduction Let L(X; Y ) be the Banach algebra of all bounded linear operators from one complex Banach space X to another Y: If X = Y; then L(X; X) = L(X): For A 2 L(X; Y ) we denote by R(A) its range, N(A) its null space and σ(A) its spectrum. If A 2 L(X); we denote by %(A) the resolvent set of A: Let IX (respectively IY ) denotes the identity operator in X (respectively in Y ). Recall that an operator A 2 L(X) is called nilpotent if Ap = 0 for some p 2 N∗ and A is said to be quasi- nilpotent if σ(A) = f0g : For a set M, let @M, M denote the boundary and the closure of M, respectively. -
Arxiv:1911.04811V3 [Math.FA] 20 Nov 2020 Hswr a Upre Ytentoa Cec Ete Pola Centre, Science National the by Supported Was Work This Pressure
SPECTRUM OF WEIGHTED ISOMETRIES: C∗-ALGEBRAS, TRANSFER OPERATORS AND TOPOLOGICAL PRESSURE KRZYSZTOF BARDADYN AND BARTOSZ KOSMA KWAŚNIEWSKI Abstract. We study the spectrum of operators aT (H) on a Hilbert space H ∈ B ∗ where T is an isometry and a belongs to a commutative C -subalgebra C(X) ∼= A (H) such that the formula L(a) = T ∗aT defines a faithful transfer operator on A⊆. BasedB on the analysis of the C∗-algebra C∗(A, T ) generated by the operators aT , a A, we give dynamical conditions implying that the spectrum σ(aT ) is invariant ∈ under rotation around zero, σ(aT ) coincides with the essential spectrum σess(aT ) or that σ(aT ) is the disc z C : z r(aT ) . We get the best results{ ∈ when| the|≤ underlying} mapping ϕ : X X is expanding and open. We prove for any such map and a continuous map c : X →[0, ) that the spec- → ∞ tral logarythm of a Ruelle-Perron-Frobenious operator cf(y)= −1 c(x)f(x) is L x∈ϕ (y) equal to the topological pressure P (ln c, ϕ). This extends Ruelle’s classical result and P implies the variational principle for the spectral radius: hϕ(µ) r(aT )= max exp ln( a √̺) dµ + , µ∈Erg(X,ϕ) | | 2 ZX where Erg(X, ϕ) is the set of ergodic Borel probability measures, hϕ(µ) is the Kolmo- gorov-Sinai entropy, and ̺ : X [0, 1] is the cocycle associated to L. In particular, we clarify the relationship between→ the Kolmogorov-Sinai entropy and t-entropy introduced by Antonevich, Bakhtin and Lebedev. -
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. -
Spectral Stability of the Critical Front in the Extended Fisher-KPP Equation
Spectral stability of the critical front in the extended Fisher-KPP equation Montie Avery∗ Louis Garénaux† September 4, 2020 Abstract We revisit the existence and stability of the critical front in the extended Fisher-KPP equation, refining earlier results of Rottschäfer and Wayne [28] which establish stability of fronts without identifying a precise decay rate. We verify that the front is marginally spectrally stable: while the essential spectrum touches the imaginary axis at the origin, there are no unstable eigenvalues and no eigenvalue (or resonance) embedded in the essential spectrum at the origin. Together with the recent work of Avery and Scheel [3], this implies nonlinear stability of the critical front with sharp t−3/2 decay rate, as previously obtained in the classical Fisher-KPP equation. The main challenges are to regularize the singular perturbation in the extended Fisher-KPP equation and to track eigenvalues near the essential spectrum, and we overcome these difficulties with functional analytic methods. 1 Introduction 1.1 Background and main results We consider the extended Fisher-KPP equation 2 ut = δ uxxxx + uxx + f(u), (1.1) − for small values of the parameter δ. Notice that the sign of δ R will play no role in what follows. Here we ∈ assume f is of Fisher-KPP type: f(0) = f(1) = 0, f 0(0) > 0, f 0(1) < 0, and f 00(u) < 0 for all u (0, 1); see ∈ Section 1.2 for comments on this last assumption. Equation (1.1) may be derived as an amplitude equation near certain co-dimension 2 bifurcations in reaction-diffusion systems [27], and for δ = 0, it reduces to the classical Fisher-KPP equation, which is a fundamental model for front propagation into unstable states. -
A Primary Introduction to Spectral Theory
A primary introduction to spectral theory Jianwei Yang∗ Assistant Professor at School of Mathematics and Statistics, Beijing Institute of Technology Chaire internationale au LAGA de l’Université Paris 13 En contriburant au projet scientifique du Labex MME-DII Novembre 2019 ∗http://math.bit.edu.cn/szdw/azcpl/tbfyjy/yjw/index.htm i Contents Introduction iii 1 Hilbert spaces and the spectrum of operators 1 1.1 Hilbert space and its subspaces . 1 1.1.1 Hilbert spaces . 1 1.1.2 Subspaces . 5 1.2 Operators on Hilbert spaces . 7 1.3 Spectrum . 11 2 Self-adjointness 13 2.1 Spectrum of self-adjoint operators . 13 2.2 Fundamental criteria for self-adjointness . 15 3 The essential spectrum and Compact operators 17 3.1 Weyl’s criterion on the essential spectrum . 17 3.2 Compact operators . 20 4 Stability of the essential spectrum: Weyl’s theorem 24 4.1 Relatively compact operators . 24 4.2 Weyl’s Theorem . 24 4.3 An application . 26 Bibliography 28 ii Introduction This course will be at very elementary level with prerequisite only on limited knowledge of integration theory and linear algebra. We will start with the theory of Hilbert space and operators on it, focusing our attention on self-adjoint operators and compact operators. After introducing the general notion of spectrum of an operator and its classification, we move on to certain properties of these operators in connection with their spectral behavior, including a simple version of the Fredholm alternative and Weyl’s theorem, which is about the invariance of the essential spectrum of an operator under relatively compact perturbation. -
On the Korteweg-De Vries Equation: Frequencies and Initial Value Problem
pacific journal of mathematics Vol. 181, No. 1, 1997 ON THE KORTEWEG-DE VRIES EQUATION: FREQUENCIES AND INITIAL VALUE PROBLEM D. Battig,¨ T. Kappeler and B. Mityagin The Korteweg-de Vries equation (KdV) 3 2 1 ∂tv(x, t)+∂xv(x, t) − 3∂xv(x, t) =0 (x∈S ,t∈R) is a completely integrable system with phase space L2(S1). R Although the Hamiltonian H(q):= 1 ∂q(x)2+q(x)3 dx S1 2 x is defined only on the dense subspace H1(S1), we prove that ∂H the frequencies ωj = can be defined on the whole space ∂Jj 2 1 L (S ), where (Jj)j≥1 denote the action variables which are globally defined on L2(S1). These frequencies are real ana- lytic functionals and can be used to analyze Bourgain’s weak solutions of KdV with initial data in L2(S1). The same method can be used for any equation in the KdV −hierarchy. 1. Introduction and summary of the results. It is well known that the Korteweg-de Vries equation (KdV ) on the circle 3 (1.1) ∂tv(x, t)=−∂xv(x, t)+6v(x, t)∂xv(x, t) can be viewed as a completely integrable Hamiltonian system of infinite dimension. We choose as its phase space L2(S1)=L2(S1;R) where S1 is the circle of length 1. The Poisson structure is the one proposed by Gardner, Z ∂F d ∂G (1.2) {F, G} = dx S1 ∂q(x) dx ∂q(x) where F, G are C1- functionals on L2(S1), and ∂F denotes the L2-gradient ∂q(x) of the functional F .