Self-Adjoint Semigroups with Nilpotent Commutators ∗ Matjaž Omladiˇc A, ,1, Heydar Radjavi B,2
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Appendix A. Measure and Integration
Appendix A. Measure and integration We suppose the reader is familiar with the basic facts concerning set theory and integration as they are presented in the introductory course of analysis. In this appendix, we review them briefly, and add some more which we shall need in the text. Basic references for proofs and a detailed exposition are, e.g., [[ H a l 1 ]] , [[ J a r 1 , 2 ]] , [[ K F 1 , 2 ]] , [[ L i L ]] , [[ R u 1 ]] , or any other textbook on analysis you might prefer. A.1 Sets, mappings, relations A set is a collection of objects called elements. The symbol card X denotes the cardi- nality of the set X. The subset M consisting of the elements of X which satisfy the conditions P1(x),...,Pn(x) is usually written as M = { x ∈ X : P1(x),...,Pn(x) }.A set whose elements are certain sets is called a system or family of these sets; the family of all subsystems of a given X is denoted as 2X . The operations of union, intersection, and set difference are introduced in the standard way; the first two of these are commutative, associative, and mutually distributive. In a { } system Mα of any cardinality, the de Morgan relations , X \ Mα = (X \ Mα)and X \ Mα = (X \ Mα), α α α α are valid. Another elementary property is the following: for any family {Mn} ,whichis { } at most countable, there is a disjoint family Nn of the same cardinality such that ⊂ \ ∪ \ Nn Mn and n Nn = n Mn.Theset(M N) (N M) is called the symmetric difference of the sets M,N and denoted as M #N. -
The Index of Normal Fredholm Elements of C* -Algebras
proceedings of the american mathematical society Volume 113, Number 1, September 1991 THE INDEX OF NORMAL FREDHOLM ELEMENTS OF C*-ALGEBRAS J. A. MINGO AND J. S. SPIELBERG (Communicated by Palle E. T. Jorgensen) Abstract. Examples are given of normal elements of C*-algebras that are invertible modulo an ideal and have nonzero index, in contrast to the case of Fredholm operators on Hubert space. It is shown that this phenomenon occurs only along the lines of these examples. Let T be a bounded operator on a Hubert space. If the range of T is closed and both T and T* have a finite dimensional kernel then T is Fredholm, and the index of T is dim(kerT) - dim(kerT*). If T is normal then kerT = ker T*, so a normal Fredholm operator has index 0. Let us consider a generalization of the notion of Fredholm operator intro- duced by Atiyah. Let X be a compact Hausdorff space and consider continuous functions T: X —>B(H), where B(H) is the set of bounded linear operators on a separable infinite dimensional Hubert space with the norm topology. The set of such functions forms a C*- algebra C(X) <g>B(H). A function T is Fredholm if T(x) is Fredholm for each x . Atiyah [1, Appendix] showed how such an element has an index which is an element of K°(X). Suppose that T is Fredholm and T(x) is normal for each x. Is the index of T necessarily 0? There is a generalization of this question that we would like to consider. -
C*-Algebraic Spectral Sets, Twisted Groupoids and Operators
C∗-Algebraic Spectral Sets, Twisted Groupoids and Operators Marius M˘antoiu ∗ July 7, 2020 Abstract We treat spectral problems by twisted groupoid methods. To Hausdorff locally compact groupoids endowed with a continuous 2-cocycle one associates the reduced twisted groupoid C∗-algebra. Elements (or multipliers) of this algebra admit natural Hilbert space representations. We show the relevance of the orbit closure structure of the unit space of the groupoid in dealing with spectra, norms, numerical ranges and ǫ-pseudospectra of the resulting operators. As an ex- ample, we treat a class of pseudo-differential operators introduced recently, associated to group actions. We also prove a Decomposition Principle for bounded operators connected to groupoids, showing that several relevant spectral quantities of these operators coincide with those of certain non-invariant restrictions. This is applied to Toeplitz-like operators with variable coefficients and to band dominated operators on discrete metric spaces. Introduction Many applications of C∗-algebras to spectral analysis rely on a very simple principle: a morphism between two C∗-algebras is contractive and reduces the spectrum of elements. In addition, if it is injective, it is isometric and preserves spectra. While working on this project, we became aware of the fact that such a principle works ef- fectively for much more than spectra (and essential spectra). We call C∗-algebraic spectral set a function Σ sending, for any unital C∗-algebra E , the elements E of this one to closed (usually com- pact) subsets Σ(E |E ) of C , having the above mentioned behavior under C∗-morphisms. Definition 1.1 states this formally. -
Arxiv:1909.02676V3 [Math.DG] 25 Jul 2021 Elsetu Jcb Arcshv Ipera Pcrm.Mor a of Spectrum)
AN ATLAS ADAPTED TO THE TODA FLOW DAVID MART´INEZ TORRES AND CARLOS TOMEI Abstract. We describe an atlas adapted to the Toda flow on the mani- fold of full flags of any non-compact real semisimple Lie algebra, and on its Hessenberg-type submanifolds. We show that in these local coordinates the Toda flow becomes linear. The local coordinates are used to show that the Toda flow on the manifold of full flags is Morse-Smale, which generalizes the re- sult for traceless matrices in [27] to arbitrary non-compact real semisimple Lie algebras. As a byproduct we describe new features of classical constructions in matrix theory. 1. Introduction The non-periodic Toda lattice is a Hamiltonian model for a wave propagation along n particles in a line proposed by Toda [30]. A change of variables introduced by Flaschka [14] transforms the original O.D.E. into the matrix differential equation X′ = [X, πkX]= T (X), (1) where X runs over Jacobi matrices and πk is the first projection associated to the decomposition of a matrix into its antisymmetric and upper triangular summands. From a mathematical viewpoint (1) is a vector field everywhere defined on the Lie algebra of real traceless matrices. Since it is in Lax form it is tangent to every adjoint orbit and, in particular, to the orbit made of traceless matrices of any fixed simple real spectrum (Jacobi matrices have simple real spectrum). Moreover, formula (1) implies that the Toda vector field T is tangent to any vector subspace which is stable upon taking Lie bracket with antisymmetric matrices. -
Chapter 2 C -Algebras
Chapter 2 C∗-algebras This chapter is mainly based on the first chapters of the book [Mur90]. Material bor- rowed from other references will be specified. 2.1 Banach algebras Definition 2.1.1. A Banach algebra C is a complex vector space endowed with an associative multiplication and with a norm k · k which satisfy for any A; B; C 2 C and α 2 C (i) (αA)B = α(AB) = A(αB), (ii) A(B + C) = AB + AC and (A + B)C = AC + BC, (iii) kABk ≤ kAkkBk (submultiplicativity) (iv) C is complete with the norm k · k. One says that C is abelian or commutative if AB = BA for all A; B 2 C . One also says that C is unital if 1 2 C , i.e. if there exists an element 1 2 C with k1k = 1 such that 1B = B = B1 for all B 2 C . A subalgebra J of C is a vector subspace which is stable for the multiplication. If J is norm closed, it is a Banach algebra in itself. Examples 2.1.2. (i) C, Mn(C), B(H), K (H) are Banach algebras, where Mn(C) denotes the set of n × n-matrices over C. All except K (H) are unital, and K (H) is unital if H is finite dimensional. (ii) If Ω is a locally compact topological space, C0(Ω) and Cb(Ω) are abelian Banach algebras, where Cb(Ω) denotes the set of all bounded and continuous complex func- tions from Ω to C, and C0(Ω) denotes the subset of Cb(Ω) of functions f which vanish at infinity, i.e. -
Dilations on Locally Hilbert Spaces
The article was published in “Topics in Mathematics, Computer Science and Philosophy, A Festschrift for Wolfgang W. Breckner”, Presa Universitar˘aClujean˘a, 2008, pp. 107 – 122. The present version contains some spelling and typing corrections and is differently formatted. For references please use the information above. DILATIONS ON LOCALLY HILBERT SPACES DUMITRU GAS¸PAR, PASTOREL˘ GAS¸PAR, AND NICOLAE LUPA Dedicated to Wolfgang W. Breckner for his 65th birthday Abstract. The principal theorem of Sz.-Nagy on dilation of a positive definite Hilbert space operator valued function has played a central role in the development of the non-self-adjoint operator theory. In this paper we introduce the positive definiteness for locally Hilbert space operator valued kernels, we prove an analogue of the Sz.-Nagy dilation theorem and, as application, we obtain dilation results for locally contractions and locally ρ - contractions as well as for locally semi-spectral measures. 1. Introduction It is well known that the class B(H) of all bounded linear operators on a Hilbert space H can be organized as a C∗ - algebra, and any C∗ - alge- bra embeds isometrically in such an operator algebra. At the same time, because the above algebra B(H) is the dual of the trace-class C1(H), it follows that it is a W ∗ - algebra and conversely, any W ∗ - algebra can be identified up to an algebraic-topological isomorphism with a weak operator closed ∗ - subalgebra in B(H). Hence, the spectral theory of bounded lin- ear operators on a Hilbert space is developed in close connection with the arXiv:1504.07756v1 [math.FA] 29 Apr 2015 theory of C∗ - algebras. -
Class Notes, Functional Analysis 7212
Class notes, Functional Analysis 7212 Ovidiu Costin Contents 1 Banach Algebras 2 1.1 The exponential map.....................................5 1.2 The index group of B = C(X) ...............................6 1.2.1 p1(X) .........................................7 1.3 Multiplicative functionals..................................7 1.3.1 Multiplicative functionals on C(X) .........................8 1.4 Spectrum of an element relative to a Banach algebra.................. 10 1.5 Examples............................................ 19 1.5.1 Trigonometric polynomials............................. 19 1.6 The Shilov boundary theorem................................ 21 1.7 Further examples....................................... 21 1.7.1 The convolution algebra `1(Z) ........................... 21 1.7.2 The return of Real Analysis: the case of L¥ ................... 23 2 Bounded operators on Hilbert spaces 24 2.1 Adjoints............................................ 24 2.2 Example: a space of “diagonal” operators......................... 30 2.3 The shift operator on `2(Z) ................................. 32 2.3.1 Example: the shift operators on H = `2(N) ................... 38 3 W∗-algebras and measurable functional calculus 41 3.1 The strong and weak topologies of operators....................... 42 4 Spectral theorems 46 4.1 Integration of normal operators............................... 51 4.2 Spectral projections...................................... 51 5 Bounded and unbounded operators 54 5.1 Operations.......................................... -
Toroidal Matrix Links: Local Matrix Homotopies and Soft Tori
University of New Mexico UNM Digital Repository Mathematics & Statistics ETDs Electronic Theses and Dissertations 8-25-2016 Toroidal Matrix Links: Local Matrix Homotopies and Soft orT i Fredy Antonio Vides Romero Follow this and additional works at: https://digitalrepository.unm.edu/math_etds Recommended Citation Vides Romero, Fredy Antonio. "Toroidal Matrix Links: Local Matrix Homotopies and Soft orT i." (2016). https://digitalrepository.unm.edu/math_etds/51 This Dissertation is brought to you for free and open access by the Electronic Theses and Dissertations at UNM Digital Repository. It has been accepted for inclusion in Mathematics & Statistics ETDs by an authorized administrator of UNM Digital Repository. For more information, please contact [email protected]. Fredy Antonio Vides Romero Candidate Mathematics and Statistics Department This dissertation is approved, and it is acceptable in quality and form for publication: Approved by the Dissertation Committee: Terry A. Loring Prof. Terry A. Loring, Chair Alexandru Buium Prof. Alexandru Buium, Member Charles Boyer Prof. Charles Boyer, Member Judith Packer Prof. Judith Packer, Member Toroidal Matrix Links: Local Matrix Homotopies and Soft Tori by Fredy Antonio Vides Romero B.Sc., Mathematics, National Autonomous University of Honduras, 2010 M.Sc., Mathematics, University of New Mexico, 2013 THESIS Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy Mathematics The University of New Mexico Albuquerque, New Mexico July, 2016 c 2016, Fredy Antonio Vides Romero iii Dedication To my mom Fidelia and my wife Mirna, for their love, support and their unbreakable faith in me. \Mathematics is the alphabet with which God has written the universe." { Galileo Galilei iv Acknowledgments I thank God, the divine mathematician, for the adventure of life. -
Approximation with Normal Operators with Finite Spectrum, and an Elementary Proof of a Brown–Douglas–Fillmore Theorem
Pacific Journal of Mathematics APPROXIMATION WITH NORMAL OPERATORS WITH FINITE SPECTRUM, AND AN ELEMENTARY PROOF OF A BROWN–DOUGLAS–FILLMORE THEOREM Peter Friis and Mikael Rørdam Volume 199 No. 2 June 2001 PACIFIC JOURNAL OF MATHEMATICS Vol. 199, No. 2, 2001 APPROXIMATION WITH NORMAL OPERATORS WITH FINITE SPECTRUM, AND AN ELEMENTARY PROOF OF A BROWN–DOUGLAS–FILLMORE THEOREM Peter Friis and Mikael Rørdam We give a short proof of the theorem of Brown, Douglas and Fillmore that an essentially normal operator on a Hilbert space is of the form “normal plus compact” if and only if it has trivial index function. The proof is basically a modification of our short proof of Lin’s theorem on almost commuting self- adjoint matrices that takes into account the index. Using similar methods we obtain new results, generalizing results of Lin, on approximating normal operators by ones with finite spectrum. 1. Introduction. Let H be an infinite-dimensional separable Hilbert space, let K denote the compact operators on H, and consider the short-exact sequence 0 −−−→ K −−−→ B(H) −−−→π Q(H) −−−→ 0 where Q(H) is the Calkin algebra B(H)/K. An operator T ∈ B(H) is essentially normal if T ∗T − TT ∗ ∈ K, or equivalently, if π(T ) is normal. An operator T ∈ B(H) is Fredholm if π(T ) is invertible in Q(H), and it’s Fredholm index is denoted by index(T ). The essential spectrum spess(T ) is the spectrum of π(T ). The index function of T is the map C \ spess(T ) → Z; λ 7→ index(T − λ·1). -
Arxiv:1605.06590V2 [Math.OA] 22 Jun 2016
LOCAL MATRIX HOMOTOPIES AND SOFT TORI TERRY A. LORING AND FREDY VIDES Abstract. We present solutions to local connectivity problems in matrix rep- N 2 resentations of the form C([−1; 1] ) ! An;" C"(T ) for any " 2 [0; 2] 2 and any integer n ≥ 1, where An;" ⊆ Mn and where C"(T ) denotes the Soft Torus. We solve the connectivity problems by introducing the so called toroidal matrix links, which can be interpreted as normal contractive matrix analogies of free homotopies in differential algebraic topology. In order to deal with the locality constraints, we have combined some tech- niques introduced in this document with some techniques from matrix geom- etry, combinatorial optimization, classification and representation theory of C∗-algebras. 1. Introduction In this document we study the solvability of some local connectivity problems via constrained normal matrix homotopies in C∗-representations of the form N (1.1) C(T ) −! Mn; for a fixed but arbitrary integer N ≥ 1 and any integer n ≥ 1. In particular we study local normal matrix homotopies which preserve commutativity and also satisfy some additional constraints, like being rectifiable or piecewise analytic. We build on some homotopic techniques introduced initially by Bratteli, Elliot, Evans and Kishimoto in [3] and generalized by Lin in [18] and [22]. We combine the homotopic techniques with some techniques introduced here and some other techniques from matrix geometry and noncommutative topology developed by Lor- ing [24, 27], Shulman [27], Bhatia [1], Chu [7], Brockett [4], Choi [6, -
A Continuous Geometry As a Mathematical Model for Quantum Mechanics
Commentationes Mathematicae Universitatis Carolinae Christopher J. Duckenfield A continuous geometry as a mathematical model for quantum mechanics Commentationes Mathematicae Universitatis Carolinae, Vol. 10 (1969), No. 2, 217--236 Persistent URL: http://dml.cz/dmlcz/105229 Terms of use: © Charles University in Prague, Faculty of Mathematics and Physics, 1969 Institute of Mathematics of the Academy of Sciences of the Czech Republic provides access to digitized documents strictly for personal use. Each copy of any part of this document must contain these Terms of use. This paper has been digitized, optimized for electronic delivery and stamped with digital signature within the project DML-CZ: The Czech Digital Mathematics Library http://project.dml.cz Comment at i ones Mathematicae Universitatis Carolinae 10,2 (1969) A CONTINUOUS GEOMETRY AS A MATHEMATICAL MODEL FOR QUANTUM MECHANICS Christopher J. DUCKEHFIELD, &TOERS, Conn.. Introduction. The usual as3ertions of quantum mecha- nica are that observablea are aelf-adjoint operatora in Hilbert apace, atates are vectors in this space, and the expectation value of an obaervable A in the state "Sf is ( AUC 7 V) . The "pure" statea are aasociated with unit vectors (i.e. "points") in the Hilbert space» G. Mackey [1] has produced a set of axioms for the standard model for quantum mechanics which gives a mathematical theory in accordance with the above as3ertions. The spec tral theory for operators on a Hilbert space plays a vi tal role in this analysi9. Thi3 theory is developed from the basic assumption that underlying every physical system is an orthocomple- mented lattice, namely the lattice of experimentally ve rifiable propositions about the system. -
Algebraic Approach to Quantum Theory: a Finite-Dimensional Guide
Algebraic approach to quantum theory: a finite-dimensional guide Cédric Bény Florian Richter arXiv:1505.03106v8 [quant-ph] 26 May 2020 Contents 1 Introduction 1 2 States and effects 1 2.1 Basic Quantum Mechanics . .1 2.2 Positive operators . .1 2.3 Generalized States . .3 2.3.1 Ensembles . .3 2.3.2 Tensor Product and Reduced States . .5 2.3.3 Density Operator/Matrix . .7 2.3.4 Example: Entanglement . .8 2.3.5 Example: Bloch Sphere . .9 2.4 Generalised propositions . .9 2.5 Abstract State/Effect Formalism . 10 2.5.1 Example: Quantum Theory . 11 2.5.2 Example: Classical Probability Theory . 11 2.6 Algebraic Formulation . 12 2.6.1 Example: Quantum Theory . 13 2.6.2 Example: Classical Probability Theory . 14 2.6.3 Example: C∗-Algebra . 15 2.7 Structure of matrix algebras . 15 2.8 Hybrid quantum/classical systems . 21 3 Channels 23 3.1 Schrödinger Picture . 24 3.1.1 Example: Partial Transpose . 25 3.1.2 Example: Homomorphisms . 25 3.1.3 Example: Mixture of unitaries . 26 3.1.4 Example: Classical channels . 26 3.2 Heisenberg Picture . 26 3.3 Observables as channels with classical output . 28 3.3.1 Example: Observable associated with an effect . 28 3.3.2 Coarse-graining of observables . 30 3.3.3 Accessible observables . 31 3.4 Stinespring dilation . 32 1 Introduction This document is meant as a pedagogical introduction to the modern language used to talk about quantum theories, especially in the field of quantum information. It assumes that the reader has taken a first traditional course on quantum mechanics, and is familiar with the concept of Hilbert space and elementary linear algebra.