Stats 310A (Math 230A) Lecture Notes Sourav Chatterjee
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Arxiv:1508.00389V3 [Math.OA]
LIFTING THEOREMS FOR COMPLETELY POSITIVE MAPS JAMES GABE Abstract. We prove lifting theorems for completely positive maps going out of exact C∗- algebras, where we remain in control of which ideals are mapped into which. A consequence is, that if X is a second countable topological space, A and B are separable, nuclear C∗- algebras over X, and the action of X on A is continuous, then E(X; A, B) =∼ KK(X; A, B) naturally. As an application, we show that a separable, nuclear, strongly purely infinite C∗-algebra A absorbs a strongly self-absorbing C∗-algebra D if and only if I and I ⊗ D are KK- equivalent for every two-sided, closed ideal I in A. In particular, if A is separable, nuclear, and strongly purely infinite, then A ⊗O2 =∼ A if and only if every two-sided, closed ideal in A is KK-equivalent to zero. 1. Introduction Arveson was perhaps the first to recognise the importance of lifting theorems for com- pletely positive maps. In [Arv74], he uses a lifting theorem to give a simple and operator theoretic proof of the fact that the Brown–Douglas–Fillmore semigroup Ext(X) is actually a group. This was already proved by Brown, Douglas, and Fillmore in [BDF73], but the proof was somewhat complicated and very topological in nature. All the known lifting theorems at that time were generalised by Choi and Effros [CE76], when they proved that any nuclear map going out of a separable C∗-algebra is liftable. This result, together with the dilation theorem of Stinespring [Sti55] and the Weyl–von Neumann type theorem of Voiculescu [Voi76], was used by Arveson [Arv77] to prove that the (generalised) Brown– Douglas–Fillmore semigroup Ext(A) defined in [BDF77] is a group for any unital, separable, nuclear C∗-algebra A. -
Continuous Selections of Multivalued Mappings 3
Continuous selections of multivalued mappings Duˇsan Repovˇsand Pavel V. Semenov Abstract This survey covers in our opinion the most important results in the theory of continuous selections of multivalued mappings (approximately) from 2002 through 2012. It extends and continues our previous such survey which appeared in Recent Progress in General Topology, II which was pub- lished in 2002. In comparison, our present survey considers more restricted and specific areas of mathematics. We remark that we do not consider the theory of selectors (i.e. continuous choices of elements from subsets of topo- logical spaces) since this topics is covered by another survey in this volume. 1 Preliminaries A selection of a given multivalued mapping F : X Y with nonempty values F (x) = , for every x X, is a mapping Φ : X → Y (in general, also multivalued)6 which∅ for every ∈x X, selects a nonempty→ subset Φ(x) F (x). When all Φ(x) are singletons, a selection∈ is called singlevalued and is identified⊂ with the usual singlevalued mapping f : X Y, f(x) = Φ(x). As a rule, we shall use small letters f, g, h, φ, ψ, ... for singlevalued→ { mappings} and capital letters F, G, H, Φ, Ψ, ... for multivalued mappings. There exist a great number of theorems on existence of selections in the category of topological spaces and their continuous (in various senses) map- arXiv:1401.2257v1 [math.GN] 10 Jan 2014 Duˇsan Repovˇs Faculty of Education and Faculty of Mathematics and Physics, University of Ljubljana, P. O. Box 2964, Ljubljana, Slovenia 1001 e-mail: [email protected] Pavel V. -
Selection Theorems
SELECTION THEOREMS STEPHANIE HICKS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE IN MATHEMATICS NIPISSING UNIVERSITY SCHOOL OF GRADUATE STUDIES NORTH BAY, ONTARIO © Stephanie Hicks August 2012 I hereby declare that I am the sole author of this Major Research Paper. I authorize Nipissing University to lend this Major Research Paper to other institutions or individuals for the purpose of scholarly research. I further authorize Nipissing University to reproduce this Major Research Paper by photocopying or by other means, in total or in part, at the request of other institutions or individuals for the purpose of scholarly research. v Acknowledgements I would like to thank several important individuals who played an integral role in the development of this paper. Most importantly, I would like to thank my fiancé Dan for his ability to believe in my success at times when I didn’t think possible. Without his continuous support, inspiration and devotion, this paper would not have been possible. I would also like to thank my parents and my sister for their encouragement and love throughout the years I have spent pursuing my post secondary education. Many thanks are due to my advisor Dr. Vesko Valov for his expertise and guidance throughout this project. Additionally, I would like to thank my external examiner Vasil Gochev and my second reader Dr. Logan Hoehn for their time. Lastly, I would like to thank Dr. Wenfeng Chen and Dr. Murat Tuncali for passing on their invaluable knowledge and encouragement to pursue higher education throughout my time as a Mathematics student at Nipissing University. -
Dynkin (Λ-) and Π-Systems; Monotone Classes of Sets, and of Functions – with Some Examples of Application (Mainly of a Probabilistic flavor)
Dynkin (λ-) and π-systems; monotone classes of sets, and of functions { with some examples of application (mainly of a probabilistic flavor) Matija Vidmar February 7, 2018 1 Dynkin and π-systems Some basic notation: Throughout, for measurable spaces (A; A) and (B; B), (i) A=B will denote the class of A=B-measurable maps, and (ii) when A = B, A_B := σA(A[B) will be the smallest σ-field on A containing both A and B (this notation has obvious extensions to arbitrary families of σ-fields on a given space). Furthermore, for a measure µ on F, µf := µ(f) := R fdµ will signify + − the integral of an f 2 F=B[−∞;1] against µ (assuming µf ^ µf < 1). Finally, for a probability space (Ω; F; P) and a sub-σ-field G of F, PGf := PG(f) := EP[fjG] will denote the conditional + − expectation of an f 2 F=B[−∞;1] under P w.r.t. G (assuming Pf ^ Pf < 1; in particular, for F 2 F, PG(F ) := P(F jG) = EP[1F jG] will be the conditional probability of F under P given G). We consider first Dynkin and π-systems. Definition 1. Let Ω be a set, D ⊂ 2Ω a collection of its subsets. Then D is called a Dynkin system, or a λ-system, on Ω, if (i) Ω 2 D, (ii) fA; Bg ⊂ D and A ⊂ B, implies BnA 2 D, and (iii) whenever (Ai)i2N is a sequence in D, and Ai ⊂ Ai+1 for all i 2 N, then [i2NAi 2 D. -
Problem Set 1 This Problem Set Is Due on Friday, September 25
MA 2210 Fall 2015 - Problem set 1 This problem set is due on Friday, September 25. All parts (#) count 10 points. Solve the problems in order and please turn in for full marks (140 points) • Problems 1, 2, 6, 8, 9 in full • Problem 3, either #1 or #2 (not both) • Either Problem 4 or Problem 5 (not both) • Problem 7, either #1 or #2 (not both) 1. Let D be the dyadic grid on R and m denote the Lebesgue outer measure on R, namely for A ⊂ R ( ¥ ¥ ) [ m(A) = inf ∑ `(Ij) : A ⊂ Ij; Ij 2 D 8 j : j=1 j=1 −n #1 Let n 2 Z. Prove that m does not change if we restrict to intervals with `(Ij) ≤ 2 , namely ( ¥ ¥ ) (n) (n) [ −n m(A) = m (A); m (A) := inf ∑ `(Ij) : A ⊂ Ij; Ij 2 D 8 j;`(Ij) ≤ 2 : j=1 j=1 N −n #2 Let t 2 R be of the form t = ∑n=−N kn2 for suitable integers N;k−N;:::;kN. Prove that m is invariant under translations by t, namely m(A) = m(A +t) 8A ⊂ R: −n −m Hints. For #2, reduce to the case t = 2 for some n. Then use #1 and that Dm = fI 2 D : `(I) = 2 g is invariant under translation by 2−n whenever m ≥ n. d d 2. Let O be the collection of all open cubes I ⊂ R and define the outer measure on R given by ( ¥ ¥ ) [ n(A) = inf ∑ jRnj : A ⊂ R j; R j 2 O 8 j n=0 n=0 where jRj is the Euclidean volume of the cube R. -
Dynkin Systems and Regularity of Finite Borel Measures Homework 10
Math 105, Spring 2012 Professor Mariusz Wodzicki Dynkin systems and regularity of finite Borel measures Homework 10 due April 13, 2012 1. Let p 2 X be a point of a topological space. Show that the set fpg ⊆ X is closed if and only if for any point q 6= p, there exists a neighborhood N 3 q such that p 2/ N . Derive from this that X is a T1 -space if and only if every singleton subset is closed. Let C , D ⊆ P(X) be arbitrary families of subsets of a set X. We define the family D:C as D:C ˜ fE ⊆ X j C \ E 2 D for every C 2 C g. 2. The Exchange Property Show that, for any families B, C , D ⊆ P(X), one has B ⊆ D:C if and only if C ⊆ D:B. Dynkin systems1 We say that a family of subsets D ⊆ P(X) of a set X is a Dynkin system (or a Dynkin class), if it satisfies the following three conditions: c (D1) if D 2 D , then D 2 D ; S (D2) if fDigi2I is a countable family of disjoint members of D , then i2I Di 2 D ; (D3) X 2 D . 3. Show that any Dynkin system satisfies also: 0 0 0 (D4) if D, D 2 D and D ⊆ D, then D n D 2 D . T 4. Show that the intersection, i2I Di , of any family of Dynkin systems fDigi2I on a set X is a Dynkin system on X. It follows that, for any family F ⊆ P(X), there exists a smallest Dynkin system containing F , namely the intersection of all Dynkin systems containing F . -
THE DYNKIN SYSTEM GENERATED by BALLS in Rd CONTAINS ALL BOREL SETS Let X Be a Nonempty Set and S ⊂ 2 X. Following [B, P. 8] We
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 128, Number 2, Pages 433{437 S 0002-9939(99)05507-0 Article electronically published on September 23, 1999 THE DYNKIN SYSTEM GENERATED BY BALLS IN Rd CONTAINS ALL BOREL SETS MIROSLAV ZELENY´ (Communicated by Frederick W. Gehring) Abstract. We show that for every d N each Borel subset of the space Rd with the Euclidean metric can be generated2 from closed balls by complements and countable disjoint unions. Let X be a nonempty set and 2X. Following [B, p. 8] we say that is a Dynkin system if S⊂ S (D1) X ; (D2) A ∈S X A ; ∈S⇒ \ ∈S (D3) if A are pairwise disjoint, then ∞ A . n ∈S n=1 n ∈S Some authors use the name -class instead of Dynkin system. The smallest Dynkin σ S system containing a system 2Xis denoted by ( ). Let P be a metric space. The system of all closed ballsT⊂ in P (of all Borel subsetsD T of P , respectively) will be denoted by Balls(P ) (Borel(P ), respectively). We will deal with the problem of whether (?) (Balls(P )) = Borel(P ): D One motivation for such a problem comes from measure theory. Let µ and ν be finite Radon measures on a metric space P having the same values on each ball. Is it true that µ = ν?If (Balls(P )) = Borel(P ), then obviously µ = ν.IfPis a Banach space, then µ =Dν again (Preiss, Tiˇser [PT]). But Preiss and Keleti ([PK]) showed recently that (?) is false in infinite-dimensional Hilbert spaces. We prove the following result. -
A General Product Measurability Theorem with Applications to Variational Inequalities
Electronic Journal of Differential Equations, Vol. 2016 (2016), No. 90, pp. 1{12. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu A GENERAL PRODUCT MEASURABILITY THEOREM WITH APPLICATIONS TO VARIATIONAL INEQUALITIES KENNETH L. KUTTLER, JI LI, MEIR SHILLOR Abstract. This work establishes the existence of measurable weak solutions to evolution problems with randomness by proving and applying a novel the- orem on product measurability of limits of sequences of functions. The mea- surability theorem is used to show that many important existence theorems within the abstract theory of evolution inclusions or equations have straightfor- ward generalizations to settings that include random processes or coefficients. Moreover, the convex set where the solutions are sought is not fixed but may depend on the random variables. The importance of adding randomness lies in the fact that real world processes invariably involve randomness and variabil- ity. Thus, this work expands substantially the range of applications of models with variational inequalities and differential set-inclusions. 1. Introduction This article concerns the existence of P-measurable solutions to evolution prob- lems in which some of the input data, such as the operators, forcing functions or some of the system coefficients, is random. Such problems, often in the form of evolutionary variational inequalities, abound in many fields of mathematics, such as optimization and optimal control, and in applications such as in contact me- chanics, populations dynamics, and many more. The interest in random inputs in variational inequalities arises from the uncertainty in the identification of the sys- tem inputs or parameters, possibly due to the process of construction or assembling of the system, and to the imprecise knowledge of the acting forces or environmental processes that may have stochastic behavior. -
Measure and Integration
¦ Measure and Integration Man is the measure of all things. — Pythagoras Lebesgue is the measure of almost all things. — Anonymous ¦.G Motivation We shall give a few reasons why it is worth bothering with measure the- ory and the Lebesgue integral. To this end, we stress the importance of measure theory in three different areas. ¦.G.G We want a powerful integral At the end of the previous chapter we encountered a neat application of Banach’s fixed point theorem to solve ordinary differential equations. An essential ingredient in the argument was the observation in Lemma 2.77 that the operation of differentiation could be replaced by integration. Note that differentiation is an operation that destroys regularity, while in- tegration yields further regularity. It is a consequence of the fundamental theorem of calculus that the indefinite integral of a continuous function is a continuously differentiable function. So far we used the elementary notion of the Riemann integral. Let us quickly recall the definition of the Riemann integral on a bounded interval. Definition 3.1. Let [a, b] with −¥ < a < b < ¥ be a compact in- terval. A partition of [a, b] is a finite sequence p := (t0,..., tN) such that a = t0 < t1 < ··· < tN = b. The mesh size of p is jpj := max1≤k≤Njtk − tk−1j. Given a partition p of [a, b], an associated vector of sample points (frequently also called tags) is a vector x = (x1,..., xN) such that xk 2 [tk−1, tk]. Given a function f : [a, b] ! R and a tagged 51 3 Measure and Integration partition (p, x) of [a, b], the Riemann sum S( f , p, x) is defined by N S( f , p, x) := ∑ f (xk)(tk − tk−1). -
Measures 1 Introduction
Measures These preliminary lecture notes are partly based on textbooks by Athreya and Lahiri, Capinski and Kopp, and Folland. 1 Introduction Our motivation for studying measure theory is to lay a foundation for mod- eling probabilities. I want to give a bit of motivation for the structure of measures that has developed by providing a sort of history of thought of measurement. Not really history of thought, this is more like a fictionaliza- tion (i.e. with the story but minus the proofs of assertions) of a standard treatment of Lebesgue measure that you can find, for example, in Capin- ski and Kopp, Chapter 2, or in Royden, books that begin by first studying Lebesgue measure on <. For studying probability, we have to study measures more generally; that will follow the introduction. People were interested in measuring length, area, volume etc. Let's stick to length. How was one to extend the notion of the length of an interval (a; b), l(a; b) = b − a to more general subsets of <? Given an interval I of any type (closed, open, left-open-right-closed, etc.), let l(I) be its length (the difference between its larger and smaller endpoints). Then the notion of Lebesgue outer measure (LOM) of a set A 2 < was defined as follows. Cover A with a countable collection of intervals, and measure the sum of lengths of these intervals. Take the smallest such sum, over all countable collections of ∗ intervals that cover A, to be the LOM of A. That is, m (A) = inf ZA, where 1 1 X 1 ZA = f l(In): A ⊆ [n=1Ing n=1 ∗ (the In referring to intervals). -
Nonlinear Differential Inclusions of Semimonotone and Condensing Type in Hilbert Spaces
Bull. Korean Math. Soc. 52 (2015), No. 2, pp. 421–438 http://dx.doi.org/10.4134/BKMS.2015.52.2.421 NONLINEAR DIFFERENTIAL INCLUSIONS OF SEMIMONOTONE AND CONDENSING TYPE IN HILBERT SPACES Hossein Abedi and Ruhollah Jahanipur Abstract. In this paper, we study the existence of classical and gen- eralized solutions for nonlinear differential inclusions x′(t) ∈ F (t, x(t)) in Hilbert spaces in which the multifunction F on the right-hand side is hemicontinuous and satisfies the semimonotone condition or is condens- ing. Our existence results are obtained via the selection and fixed point methods by reducing the problem to an ordinary differential equation. We first prove the existence theorem in finite dimensional spaces and then we generalize the results to the infinite dimensional separable Hilbert spaces. Then we apply the results to prove the existence of the mild solution for semilinear evolution inclusions. At last, we give an example to illustrate the results obtained in the paper. 1. Introduction Our aim is to study the nonlinear differential inclusion of first order x′(t) ∈ F (t, x(t)), (1.1) x(0) = x0, in a Hilbert spaces in which F may be condensing or semimonotone set-valued map. An approach to investigating the existence of solution for a differential inclusion is to reduce it to a problem for ordinary differential equations. In this setting, we are interested to know under what conditions the solution of the corresponding ordinary differential equation belongs to the right side of the given differential inclusion; in other words, under what conditions a continuous function such as f(·, ·) exists so that f(t, x) ∈ F (t, x) for every (t, x) and x′(t)= f(t, x(t)). -
Arxiv:1706.03690V2 [Math.OA] 9 Apr 2018 Whether Alone
A NEW PROOF OF KIRCHBERG’S O2-STABLE CLASSIFICATION JAMES GABE Abstract. I present a new proof of Kirchberg’s O2-stable classification theorem: two ∗ separable, nuclear, stable/unital, O2-stable C -algebras are isomorphic if and only if their ideal lattices are order isomorphic, or equivalently, their primitive ideal spaces are home- omorphic. Many intermediate results do not depend on pure infiniteness of any sort. 1. Introduction After classifying all AT-algebras of real rank zero [Ell93], Elliott initiated a highly am- bitious programme of classifying separable, nuclear C∗-algebras by K-theoretic and tracial invariants. During the past three decades much effort has been put into verifying such classification results. In the special case of simple C∗-algebras the classification has been verified under the very natural assumptions that the C∗-algebras are separable, unital, sim- ple, with finite nuclear dimension and in the UCT class of Rosenberg and Schochet [RS87]. The purely infinite case is due to Kirchberg [Kir94] and Phillips [Phi00], and the stably finite case was recently solved by the work of many hands; in particular work of Elliott, Gong, Lin, and Niu [GLN15], [EGLN15], and by Tikuisis, White, and Winter [TWW15]. This makes this the right time to gain a deeper understanding of the classification of non-simple C∗-algebras which is the main topic of this paper. The Cuntz algebra O2 plays a special role in the classification programme as this has the properties of being separable, nuclear, unital, simple, purely infinite, and is KK-equivalent ∗ to zero. Hence if A is any separable, nuclear C -algebra then A ⊗ O2 has no K-theoretic nor tracial data to determine potential classification, and one may ask if such C∗-algebras are classified by their primitive ideal space alone.