Banach Algebras of Lipschitz Functions
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On the Space of Generalized Fluxes for Loop Quantum Gravity
Home Search Collections Journals About Contact us My IOPscience On the space of generalized fluxes for loop quantum gravity This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2013 Class. Quantum Grav. 30 055008 (http://iopscience.iop.org/0264-9381/30/5/055008) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 194.94.224.254 The article was downloaded on 07/03/2013 at 11:02 Please note that terms and conditions apply. IOP PUBLISHING CLASSICAL AND QUANTUM GRAVITY Class. Quantum Grav. 30 (2013) 055008 (24pp) doi:10.1088/0264-9381/30/5/055008 On the space of generalized fluxes for loop quantum gravity B Dittrich1,2, C Guedes1 and D Oriti1 1 Max Planck Institute for Gravitational Physics, Am Muhlenberg¨ 1, D-14476 Golm, Germany 2 Perimeter Institute for Theoretical Physics, 31 Caroline St N, Waterloo ON N2 L 2Y5, Canada E-mail: [email protected], [email protected] and [email protected] Received 5 September 2012, in final form 13 January 2013 Published 5 February 2013 Online at stacks.iop.org/CQG/30/055008 Abstract We show that the space of generalized fluxes—momentum space—for loop quantum gravity cannot be constructed by Fourier transforming the projective limit construction of the space of generalized connections—position space— due to the non-Abelianess of the gauge group SU(2). From the Abelianization of SU(2),U(1)3, we learn that the space of generalized fluxes turns out to be an inductive limit, and we determine the consistency conditions the fluxes should satisfy under coarse graining of the underlying graphs. -
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. -
Banach Algebras
Banach Algebras Yurii Khomskii Bachelor Thesis Department of Mathematics, Leiden University Supervisor: Dr. Marcel de Jeu April 18, 2005 i Contents Foreword iv 1. Algebraic Concepts 1 1.1. Preliminaries . 1 1.2. Regular Ideals . 3 1.3. Adjoining an Identity . 4 1.4. Quasi-inverses . 8 2. Banach Algebras 10 2.1. Preliminaries of Normed and Banach Algebras . 10 2.2. Inversion and Quasi-inversion in Banach Algebras . 14 3. Spectra 18 3.1. Preliminaries . 18 3.2. Polynomial Spectral Mapping Theorem and the Spectral Radius Formula . 22 4. Gelfand Representation Theory 25 4.1. Multiplicative Linear Functionals and the Maximal Ideal Space . 25 4.2. The Gelfand Topology . 30 4.3. The Gelfand Representation . 31 4.4. The Radical and Semi-simplicity . 33 4.5. Generators of Banach algebras . 34 5. Examples of Gelfand Representations 36 5.1. C (X ) for X compact and Hausdorff . 36 5.2. C 0(X ) for X locally compact and Hausdorff. 41 5.3. Stone-Cecˇ h compactification . 42 5.4. A(D) . 44 5.5. AC (Γ) . 46 5.6. H 1 . 47 ii iii Foreword The study of Banach algebras began in the twentieth century and originated from the observation that some Banach spaces show interesting properties when they can be supplied with an extra multiplication operation. A standard exam- ple was the space of bounded linear operators on a Banach space, but another important one was function spaces (of continuous, bounded, vanishing at infin- ity etc. functions as well as functions with absolutely convergent Fourier series). Nowadays Banach algebras is a wide discipline with a variety of specializations and applications. -
Mathematical Tripos Part III Lecture Courses in 2013-2014
Mathematical Tripos Part III Lecture Courses in 2013-2014 Department of Pure Mathematics & Mathematical Statistics Department of Applied Mathematics & Theoretical Physics Notes and Disclaimers. • Students may take any combination of lectures that is allowed by the timetable. The examination timetable corresponds to the lecture timetable and it is therefore not possible to take two courses for examination that are lectured in the same timetable slot. There is no requirement that students study only courses offered by one Department. • The code in parentheses after each course name indicates the term of the course (M: Michaelmas; L: Lent; E: Easter), and the number of lectures in the course. Unless indicated otherwise, a 16 lecture course is equivalent to 2 credit units, while a 24 lecture course is equivalent to 3 credit units. Please note that certain courses are non-examinable, and are indicated as such after the title. Some of these courses may be the basis for Part III essays. • At the start of some sections there is a paragraph indicating the desirable previous knowledge for courses in that section. On one hand, such paragraphs are not exhaustive, whilst on the other, not all courses require all the pre-requisite material indicated. However you are strongly recommended to read up on the material with which you are unfamiliar if you intend to take a significant number of courses from a particular section. • The courses described in this document apply only for the academic year 2013-14. Details for subsequent years are often broadly similar, but not necessarily identical. The courses evolve from year to year. -
Spectral Theory
SPECTRAL THEORY EVAN JENKINS Abstract. These are notes from two lectures given in MATH 27200, Basic Functional Analysis, at the University of Chicago in March 2010. The proof of the spectral theorem for compact operators comes from [Zim90, Chapter 3]. 1. The Spectral Theorem for Compact Operators The idea of the proof of the spectral theorem for compact self-adjoint operators on a Hilbert space is very similar to the finite-dimensional case. Namely, we first show that an eigenvector exists, and then we show that there is an orthonormal basis of eigenvectors by an inductive argument (in the form of an application of Zorn's lemma). We first recall a few facts about self-adjoint operators. Proposition 1.1. Let V be a Hilbert space, and T : V ! V a bounded, self-adjoint operator. (1) If W ⊂ V is a T -invariant subspace, then W ? is T -invariant. (2) For all v 2 V , hT v; vi 2 R. (3) Let Vλ = fv 2 V j T v = λvg. Then Vλ ? Vµ whenever λ 6= µ. We will need one further technical fact that characterizes the norm of a self-adjoint operator. Lemma 1.2. Let V be a Hilbert space, and T : V ! V a bounded, self-adjoint operator. Then kT k = supfjhT v; vij j kvk = 1g. Proof. Let α = supfjhT v; vij j kvk = 1g. Evidently, α ≤ kT k. We need to show the other direction. Given v 2 V with T v 6= 0, setting w0 = T v=kT vk gives jhT v; w0ij = kT vk. -
MAT 449 : Representation Theory
MAT 449 : Representation theory Sophie Morel December 17, 2018 Contents I Representations of topological groups5 I.1 Topological groups . .5 I.2 Haar measures . .9 I.3 Representations . 17 I.3.1 Continuous representations . 17 I.3.2 Unitary representations . 20 I.3.3 Cyclic representations . 24 I.3.4 Schur’s lemma . 25 I.3.5 Finite-dimensional representations . 27 I.4 The convolution product and the group algebra . 28 I.4.1 Convolution on L1(G) and the group algebra of G ............ 28 I.4.2 Representations of G vs representations of L1(G) ............. 33 I.4.3 Convolution on other Lp spaces . 39 II Some Gelfand theory 43 II.1 Banach algebras . 43 II.1.1 Spectrum of an element . 43 II.1.2 The Gelfand-Mazur theorem . 47 II.2 Spectrum of a Banach algebra . 48 II.3 C∗-algebras and the Gelfand-Naimark theorem . 52 II.4 The spectral theorem . 55 III The Gelfand-Raikov theorem 59 III.1 L1(G) ....................................... 59 III.2 Functions of positive type . 59 III.3 Functions of positive type and irreducible representations . 65 III.4 The convex set P1 ................................. 68 III.5 The Gelfand-Raikov theorem . 73 IV The Peter-Weyl theorem 75 IV.1 Compact operators . 75 IV.2 Semisimplicity of unitary representations of compact groups . 77 IV.3 Matrix coefficients . 80 IV.4 The Peter-Weyl theorem . 86 IV.5 Characters . 87 3 Contents IV.6 The Fourier transform . 90 IV.7 Characters and Fourier transforms . 93 V Gelfand pairs 97 V.1 Invariant and bi-invariant functions . -
Israel Moiseevich Gelfand, (1913 - 2009)
1 Israel Moiseevich Gelfand, (1913 - 2009) V.S.Sunder The Institute of Mathematical Sciences, Taramani, Chennai 600113, India e-mail: [email protected] January 17, 2011 When Gelfand passed away on October 5th, 2009, the world might have seen the last of the classical scholars (in the mould of Henri Poincare or John von Neumann) whose accomplishments/scholarship were not confined by artificial borders. The wikipedia ‘paraphrases’ his work thus: ‘Israel Gelfand is known for many developments including: • the Gelfand representation in Banach algebra theory; • the Gelfand Mazur theorem in Banach algebra theory; • the Gelfand Naimark theorem; • the Gelfand Naimark Segal construction; • Gelfand Shilov spaces • the Gelfand Pettis integral; • the representation theory of the complex classical Lie groups; • contributions to the theory of Verma modules in the represen- tation theory of semisimple Lie algebras (with I.N. Bernstein and S.I. Gelfand); • contributions to distribution theory and measures on infinite- dimensional spaces; • the first observation of the connection of automorphic forms with representations (with Sergei Fomin); • conjectures about the index theorem; 2 • Ordinary differential equations (Gelfand Levitan theory); • work on calculus of variations and soliton theory (Gelfand Dikii equations); • contributions to the philosophy of cusp forms; • Gelfand Fuks cohomology of foliations; • Gelfand Kirillov dimension; • integral geometry; • combinatorial definition of the Pontryagin class; • Coxeter functors; • generalised hypergeometric series; • Gelfand - Tsetlin patterns; • and many other results, particularly in the representation the- ory for the classical groups.’ When I was requested to write something about Gelfand, my first reaction was to say ‘how can I hope to do justice to his breadth and depth of mathematical contributions?’ and at once realised that no one can. -
MATHEMATICAL TRIPOS Part III PAPER 106 FUNCTIONAL ANALYSIS
MATHEMATICAL TRIPOS Part III Monday, 30 May, 2016 9:00 am to 12:00 pm PAPER 106 FUNCTIONAL ANALYSIS Attempt no more than FOUR questions. There are FIVE questions in total. The questions carry equal weight. STATIONERY REQUIREMENTS SPECIAL REQUIREMENTS Coversheet None Treasury Tag Script paper You may not start to read the questions printed on the subsequent pages until instructed to do so by the Invigilator. 2 1 Let A be a unital Banach algebra. Prove that the group G(A) of invertible elements of A is open and that the map x → x−1 : G(A) → G(A) is continuous. Let A be a Banach algebra and x ∈ A. Define the spectrum σA(x) of x in A both in the case that A is unital and in the case A is not unital. Let A be a Banach algebra and x ∈ A. Prove that σA(x) is a non-empty compact subset of C. [You may assume any version of the Hahn–Banach theorem without proof.] State and prove the Gelfand–Mazur theorem concerning complex unital normed division algebras. Let K be an arbitrary set. Let A be an algebra of complex-valued functions on K with pointwise operations and assume that · is a complete algebra norm on A. Prove carefully that supK|f| 6 f for all f ∈ A. 2 State and prove Mazur’s theorem on the weak-closure and norm-closure of a convex set in a Banach space. [Any version of the Hahn–Banach theorem can be assumed without proof provided it is clearly stated.] Let (xn) be a sequence in a Banach space X. -
Analysis Notes
Analysis notes Aidan Backus December 2019 Contents I Preliminaries2 1 Functional analysis3 1.1 Locally convex spaces...............................3 1.2 Hilbert spaces...................................6 1.3 Bochner integration................................6 1.4 Duality....................................... 11 1.5 Vector lattices................................... 13 1.6 Positive Radon measures............................. 14 1.7 Baire categories.................................. 17 2 Complex analysis 20 2.1 Cauchy-Green formula.............................. 20 2.2 Conformal mappings............................... 22 2.3 Approximation by polynomials.......................... 24 2.4 Sheaves...................................... 26 2.5 Subharmonicity.................................. 28 2.6 Operator theory.................................. 30 II Dynamical systems 31 3 Elementary dynamical systems 32 3.1 Types of dynamical systems........................... 32 3.2 Properties of the irrational rotation....................... 34 4 Ergodic theory 37 4.1 The mean ergodic theorem............................ 37 4.2 Pointwise ergodic theorem............................ 41 4.3 Ergodic systems.................................. 45 4.4 Properties of ergodic transformations...................... 47 4.5 Mixing transformations.............................. 48 4.6 The Hopf argument................................ 54 1 5 Flows on manifolds 59 5.1 Ergodic theorems for flows............................ 59 5.2 Geodesic flows in hyperbolic space....................... -
Spectral Theory - Wikipedia, the Free Encyclopedia Spectral Theory from Wikipedia, the Free Encyclopedia
6/2/12 Spectral theory - Wikipedia, the free encyclopedia Spectral theory From Wikipedia, the free encyclopedia In mathematics, spectral theory is an inclusive term for theories extending the eigenvector and eigenvalue theory of a single square matrix to a much broader theory of the structure of operators in a variety of mathematical spaces.[1] It is a result of studies of linear algebra and the solutions of systems of linear equations and their generalizations.[2] The theory is connected to that of analytic functions because the spectral properties of an operator are related to analytic functions of the spectral parameter.[3] Contents 1 Mathematical background 2 Physical background 3 A definition of spectrum 4 What is spectral theory, roughly speaking? 5 Resolution of the identity 6 Resolvent operator 7 Operator equations 8 Notes 9 General references 10 See also 11 External links Mathematical background The name spectral theory was introduced by David Hilbert in his original formulation of Hilbert space theory, which was cast in terms of quadratic forms in infinitely many variables. The original spectral theorem was therefore conceived as a version of the theorem on principal axes of an ellipsoid, in an infinite-dimensional setting. The later discovery in quantum mechanics that spectral theory could explain features of atomic spectra was therefore fortuitous. There have been three main ways to formulate spectral theory, all of which retain their usefulness. After Hilbert's initial formulation, the later development of abstract Hilbert space and the spectral theory of a single normal operator on it did very much go in parallel with the requirements of physics; particularly at the hands of von Neumann.[4] The further theory built on this to include Banach algebras, which can be given abstractly. -
A Gelfand-Naimark Theorem for C*-Algebras
pacific journal of mathematics Vol. 184, No. 1, 1998 A GELFAND-NAIMARK THEOREM FOR C*-ALGEBRAS Ichiro Fujimoto We generalize the Gelfand-Naimark theorem for non-com- mutative C*-algebras in the context of CP-convexity theory. We prove that any C*-algebra A is *-isomorphic to the set of all B(H)-valued uniformly continuous quivariant functions on the irreducible representations Irr(A : H) of A on H vanishing at the limit 0 where H is a Hilbert space with a sufficiently large dimension. As applications, we consider the abstract Dirichlet problem for the CP-extreme boundary, and gen- eralize the notion of semi-perfectness to non-separable C*- algebras and prove its Stone-Weierstrass property. We shall also discuss a generalized spectral theory for non-normal op- erators. Introduction. The classical Gelfand-Naimark theorem states that every commutative C*- algebra A is *-isomorphic to the algebra C0(Ω) of all continuous functions on the characters Ω of A which vanish at infinity (cf. [28]). This theorem eventually opened the gate to the subject of C*-algebras, and is legitimately called “the fundamental theorem of C*-algebras” (cf. [16, 17] for the history of this theorem). Since then, there have been various attempts to general- ize this beautiful representation theorem for non-commutative C*-algebras, i.e., to reconstruct the original algebra as a certain function space on some “generalized spectrum”, or the duality theory in the broad sense, for which we can refer to e.g., [2], [3], [4], [11], [14], [19], [29], [32], [37], [39]. Among them, we cite the following notable directions which motivated our present work. -
Gelfand Representation - Wikipedia, the Free Encyclopedia
Gelfand representation - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Gelfand_isomorphism Gelfand representation From Wikipedia, the free encyclopedia (Redirected from Gelfand isomorphism) In mathematics, the Gelfand representation in functional analysis (named after I. M. Gelfand) has two related meanings: a way of representing commutative Banach algebras as algebras of continuous functions; the fact that for commutative C*-algebras, this representation is an isometric isomorphism. In the former case, one may regard the Gelfand representation as a far-reaching generalization of the Fourier transform of an integrable function. In the latter case, the Gelfand-Naimark representation theorem is one avenue in the development of spectral theory for normal operators, and generalizes the notion of diagonalizing a normal matrix. Contents 1 Historical remarks 2 The model algebra 3 Gelfand representation of a commutative Banach algebra 3.1 Examples 4 The C*-algebra case 4.1 The spectrum of a commutative C*-algebra 4.2 Statement of the commutative Gelfand-Naimark theorem 5 Applications 6 References Historical remarks One of Gelfand's original applications (and one which historically motivated much of the study of Banach algebras[citation needed]) was to give a much shorter and more conceptual proof of a celebrated lemma of Norbert Wiener (see the citation below), characterizing the elements of the group algebras L1(R) and whose translates span dense subspaces in the respective algebras. The model algebra For any locally compact Hausdorff topological space X, the space C0(X) of continuous complex-valued functions on X which vanish at infinity is in a natural way a commutative C*-algebra: The structure of algebra over the complex numbers is obtained by considering the pointwise operations of addition and multiplication.