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ILBERT SPACE METHODS ....................... QUANTUM MECHANICS FuNDAMENTAL SciENCES ILBERT SPACE METHODS QUANTUM MECHANICS Werner 0. An1rein PFL Press A Swiss academic publisher distributed by CRC Press Taylor and Francis Group, LLC 6000 Broken Sound Parkway, NW, Suite 300, Boca Raton, FL 33487 Distribution and Customer Service [email protected] www.crcpress.com Library of Congress Cataloging-in-Publication Data A catalog record for this book is available fron1 the Library of Congress. This book is published under the editorial direction of Professor Philippe-Andre Martin (EPFL, Lausanne). is an in1print owned by Presses polytechniques et universitaires romandes, a Swiss acade1nic publishing company whose n1ain purpose is to publish the teaching and research works of the Ecole polytechnique federale de Lausanne. Presses polytechniques et universitaires romandes EPFL-Centre Midi Post office box 119 CH-1015 Lausanne, Switzerland E-Mail: [email protected] Phone: 021 I 693 21 30 Fax: 021/693 40 27 www.epflpress.org © 2009, First edition, EPFL Press ISBN 978-2-940222-35-3 (EPFL Press) ISBN 978-1-4200-6681-4 ( CRC Press) Printed in Spain All right reserved (including those of translation into other languages). No part of this book n1ay be reproduced in any fonn- by photoprint, microfilm, or any other 1neans - nor transn1itted or translated into a n1achine language without written pennission fro111 the publisher. Preface This text is based on lectures given at the University of Geneva during the period 1994- 2005. These courses were intended for advanced undergraduate students who had completed a first course in quantum mechanics and were thus expected to be fa miliar with the physical aspects and the basic 1nathernatical formalism of quantum theory. Partly due to lack of time, quantum mechanics is often taught with no or little exposition of the mathematical questions arising through the introduction of infinite dimensional Hilbert spaces. I hope that the present volume will prove useful, espe cially to somewhat theoretically minded students, for deepening their knowledge and understanding of the Hilbert space aspects of quantum mechanics, and prepare them for reading research papers. Mostly the lectures were organised as one-year courses (80 hours plus 25 hours of problem sessions) and covered essentially the contents of Chapters 1 -5 and parts of Chapters 6 or 7. To offer a few more applications, some 1naterial has been added to the original lecture notes (Sections 5.8, 6.6, 6.7, 7.2 and 7.5). Of course a strict selection of topics and applications to be treated had to be made from the outset. The emphasis is placed on a certain number of basic mathematical techniques, usually without striving for the most general results. For example there is no discussion of quadratic forms, and we have avoided the use of techniques from stochastic analysis. However we give essentially complete proofs for all results involving Hilbert space objects. Some of these proofs are collected in appendices to the various chapters. Son1e acquaintance with measure theory is required: the essential facts are explained without detailed proofs. Chapter 1 gives the basic properties of Hilbert space and a description of the neces sary material from measure theory. In Chapter 2 we present various classes of bounded linear operators and general notions on unbounded operators, including the invariance of self-adjointness under a class of perturbations. The problem of self-adjointness is further investigated in Chapter 3 which contains the theory of extensions of symmetric operators, with applications to Sturm-Liouville and Schrodinger operators. Chapter 4 deals with the spectral theory of self-adjoint operators, in particular with the spectral theorem and with the various spectral types. In Chapter 5 we prove Stone's Theo rem and then discuss the fundamental aspects of scattering theory: scattering states, asymptotic condition and wave operators, S-matrix, scattering cross sections. Chapter 6 is devoted to the Mourre method for controlling the resolvent of self-adjoint oper ators near the real axis and to implications for their spectrum. In the final Chapter 7 PREFACE we present stationary-state scattering theory and various applications of the results of Chapter 6: asymptotic completeness, properties of the S-matrix, time delay and the Flux-Across-Surfaces Theorem. Each chapter ends with some bibliographical notes and a selection of problems. The bibliography consists mostly of books. They are referred to for alternative or more advanced presentations of some material or for certain points not treated in the present text. A very small number of original and review papers are cited for those interested a deeper understanding of certain topics treated in the text. In combination with tnodern electronic means. these papers can also be useful as a basis for searching in the vast literature. The majority of the problems have been tested in class-room sessions. Many of then1 are meant to help students to become familiar with the concepts discussed in the main body; son1e require a more detailed study of technical aspects of the text. A few of the more difficult problems are provided with a hint for the solution. As regards notations, it should be pointed out that some symbols have more than one 1neaning in the text. In particular: the symbol II · II is used for various norms, the Greek letter for spectra and for scattering cross sections, the letter P for projections CJ and for mon1entum, and the letter R for resolvents and for S - I, where S is the scattering operator. For the convenience of the reader we have included a Notation Index (page 385). Constants are often denoted generically by c, but in some proofs different constants are numbered as c c etc. 1, 2, is a great pleasure to thank all those who helped me in one way or another during the preparation of the lectures or of this volume. The problems in the text are mostly due to Marius Mantoiu, Joachim Stubbe and Rafael Tiedra de Aldecoa; they assumed the responsibility for the problem sessions with much competence and devotion. The continual interest of my students and their constructive comments on earlier versions of the text have influenced a considerable number of details. I received precious sup port from Philippe Jacquet, Andreas Malaspinas, Peter Wittwer and Luis Zuleta for coming to grips with TEX -related difficulties. I thank Philippe Martin for proposing the publication of my lectures, the referee for pointing out some errors and for useful suggestions, and Fred Fenter from EPFL Pre,ss for advice and his very efficient man agement of the publishing process. am indebted to the Physics Department Finally~' of the University of Geneva for its kind hospitality after my retirement. Werner Amrein Geneva, Switzerland December 2008 Contents v 1 Hilbert Spaces 1 1.1 Definition and elementary properties 1 1.2 Vector-valued functions . . . . . . . . 6 1.3 Subsets and dual of a Hilbert space . . 8 1.4 Measures, integrals and LP spaces 14 Problems ............ . 25 2 Linear Operators 27 2.1 The algebra B(H) ..... . 27 2.2 Projections and isometries 37 2.3 Compact operators . . . . 41 2.4 Unbounded operators .... 47 2.5 Multiplication operators . . . . . . 56 2.6 Resolvent and spectrum of an operator .. 67 2. 7 Perturbations of self-adjoint operators 7 Appendix ... . 80 Problems ................ . 82 3 Symmetric Operators and their Extensions 87 3.1 The method of the Cay ley transform . . 87 8 .... 3.2 Differential operators with constant coefficients 96 3.3 Schrodinger operators . . . . . . . 111 Appendix 126 Problems ...... . 131 4 Spectral Theory of Self-Adjoint Operators 133 4.1 Stieltjes measures . . . . . . . . . . . . . 133 4.2 Spectral measures . . . . . . . . . . . . . 141 4.3 Spectral parts of a self-adjoint operator . 157 4.4 The spectral theorem. The resolvent near the spectrum . . . . 170 0 ••• Appendix: Proof of the Spectral Theorem .... 179 Problems ........................ . 190 CONTENTS Vlll 5 Evolution Groups and Scattering Theory 193 5.1 Evolution groups 193 5.2 Characterisation of the scattering states .. 204 5.3 Asymptotic condition. Wave operators . 213 5.4 Simple scattering systems. Scattering operator . . 218 5.5 Scattering operator and S-matrix . 226 5.6 Scattering cross sections 235 5.7 Bounds on scattering cross sections 243 5.8 Coulomb scattering .. 252 Problems .. . .. 260 6 The Conjugate Operator Method 263 6.1 A simple example . 264 6.2 The method of differential inequalities . 271 6.3 The Mourre inequality 283 6.4 Application to Schrodinger operators .. 286 6.5 Relatively smooth operators 292 6.6 Higher order resolvent estimates 300 6.7 Some comtnutators .. 306 Appendix: Interpolation of operators 310 Problems 315 7 Further Topics in Scattering Theory 317 7.1 Asymptotic completeness . 317 7.2 Flux and scattering into cones 324 7.3 Time-independent scattering theory ... 343 7.4 The scattering matrix 352 7.5 Time delay .. 364 Appendix 374 Problems 379 References I 381 Notation Index 385 Subject Index 389 CHAPTER! Hilbert Spaces Hilbert space sets the stage for standard quantum theory: the pure states of a physical system are identified with the unit rays of a Hilbert space 1{ and observables with self adjoint operators acting in H. In this initial chapter we present the essential concepts and prove the basic results concerning separable Hilbert spaces (Sections 1.1 - 1.3 ). In Section 1.4 we then introduce £2 spaces, which are of special importance for quantum mechanics. This requires some familiarity with measure theory, and we include a short description of the necessary concepts from this theory. 1.1 Definition and elementary properties Throughout this text a Hilbert space 1neans a co1nplex linear vector space, equipped with a Hermitian scalar product, which is complete and admits a countable basis. More precisely a (separable) Hilbert space His defined by the four postulates (HI)- (H4) stated below: (Hl) H is a linear vector space over the field CC o.f co1nplex nu1nbers: With each couple {f, g} of elements of H there is associated another element of H, denoted f + g, and with each couple {a, f}, a E CC, f E H, there is associated an ele ment af ofH, and these associations have the following properties (where f, hE 1{ and a, {3 E CC): f+g==g+f f + (g + h) == (f +g) + h (1.1) a(f+g)==af+ag (a+(3)f-af+(3f (1.2) a({3f) == (a{3)f If- f. (1.3) Furthermore there exists a unique eletnent 0 E H (called the zero vector) such that 1 O+f==f Of== 0 \If E H. (1.4) 1 Here 0 denotes the complex number a = 0.

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