The $ O\Tau $-Continuous, Lebesgue, KB, and Levi Operators Between
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Isometries of Absolute Order Unit Spaces
ISOMETRIES OF ABSOLUTE ORDER UNIT SPACES ANIL KUMAR KARN AND AMIT KUMAR Abstract. We prove that for a bijective, unital, linear map between absolute order unit spaces is an isometry if, and only if, it is absolute value preserving. We deduce that, on (unital) JB-algebras, such maps are precisely Jordan isomorphisms. Next, we introduce the notions of absolutely matrix ordered spaces and absolute matrix order unit spaces and prove that for a bijective, unital, linear map between absolute matrix order unit spaces is a complete isometry if, and only if, it is completely absolute value preserving. We obtain that on (unital) C∗-algebras such maps are precisely C∗-algebra isomorphism. 1. Introduction In 1941, Kakutani proved that an abstract M-space is precisely a concrete C(K, R) space for a suitable compact and Hausdorff space K [10]. In 1943, Gelfand and Naimark proved that an abstract (unital) commutative C∗-algebra is precisely a concrete C(K, C) space for a suitable compact and Hausdorff space K [6]. Thus Gelfand-Naimark theorem for commutative C∗-algebras, in the light of Kakutani theorem, yields that the self-adjoint part of a commutative C∗-algebra is, in particular, a vector lattice. On the other hand, Kadison’s anti-lattice theorem suggest that the self-adjoint part of a general C∗-algebra can not be a vector lattice [8]. Nevertheless, the order structure of a C∗- algebra has many other properties which encourages us to expect a ‘non-commutative vector lattice’ or a ‘near lattice’ structure in it. Keeping this point of view, the first author introduced the notion of absolutely ordered spaces and that of an absolute order unit spaces [14]. -
The Semi-M Property for Normed Riesz Spaces Compositio Mathematica, Tome 34, No 2 (1977), P
COMPOSITIO MATHEMATICA EP DE JONGE The semi-M property for normed Riesz spaces Compositio Mathematica, tome 34, no 2 (1977), p. 147-172 <http://www.numdam.org/item?id=CM_1977__34_2_147_0> © Foundation Compositio Mathematica, 1977, tous droits réservés. L’accès aux archives de la revue « Compositio Mathematica » (http: //http://www.compositio.nl/) implique l’accord avec les conditions géné- rales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infrac- tion pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ COMPOSITIO MATHEMATICA, Vol. 34, Fasc. 2, 1977, pag. 147-172 Noordhoff International Publishing Printed in the Netherlands THE SEMI-M PROPERTY FOR NORMED RIESZ SPACES Ep de Jonge 1. Introduction It is well-known that if (0394, F, IL) is a u-finite measure space and if 1 ~ p 00, then the Banach dual L *p of the Banach space Lp = Lp(0394, IL) can be identified with Lq = Lq(L1, 03BC), where p-1 + q-1 = 1. For p =00 the situation is different; the space Li is a linear subspace of L*, and only in a very trivial situation (the finite-dimensional case) we have Li = Lfi. Restricting ourselves to the real case, the Banach dual L *~ is a (real) Riesz space, i.e., a vector lattice, and Li is now a band in L*. The disjoint complement (i.e., the set of all elements in L* disjoint to all elements in LI) is also a band in L*, called the band of singular linear functionals on Loo. -
Order Convergence of Vector Measures on Topological Spaces
133 (2008) MATHEMATICA BOHEMICA No. 1, 19–27 ORDER CONVERGENCE OF VECTOR MEASURES ON TOPOLOGICAL SPACES Surjit Singh Khurana, Iowa City (Received May 24, 2006) Abstract. Let X be a completely regular Hausdorff space, E a boundedly complete vector lattice, Cb(X) the space of all, bounded, real-valued continuous functions on X, F the algebra generated by the zero-sets of X, and µ: Cb(X) → E a positive linear map. First we give a new proof that µ extends to a unique, finitely additive measure µ: F → E+ such that ν is inner regular by zero-sets and outer regular by cozero sets. Then some order-convergence theorems about nets of E+-valued finitely additive measures on F are proved, which extend some known results. Also, under certain conditions, the well-known Alexandrov’s theorem about the convergent sequences of σ-additive measures is extended to the case of order convergence. Keywords: order convergence, tight and τ-smooth lattice-valued vector measures, mea- sure representation of positive linear operators, Alexandrov’s theorem MSC 2000 : 28A33, 28B15, 28C05, 28C15, 46G10, 46B42 1. Introduction and notation All vector spaces are taken over reals. E, in this paper, is always assumed to be a boundedly complete vector lattice (and so, necessarily Archimedean) ([??], [??], [??]). ′ ′ If E is a locally convex space and E its topological dual, then h·, ·i : E × E → Ê will stand for the bilinear mapping hx, fi = f(x). For a completely regular Hausdorff space X, B(X) and B1(X) are the classes of Borel and Baire subsets of X, C(X) and Cb(X) are the spaces of all real-valued, and real-valued and bounded, continuous functions on X and X is the Stone-Čech compactification of X respectively. -
A Note on Riesz Spaces with Property-$ B$
Czechoslovak Mathematical Journal Ş. Alpay; B. Altin; C. Tonyali A note on Riesz spaces with property-b Czechoslovak Mathematical Journal, Vol. 56 (2006), No. 2, 765–772 Persistent URL: http://dml.cz/dmlcz/128103 Terms of use: © Institute of Mathematics AS CR, 2006 Institute of Mathematics of the Czech Academy of Sciences provides access to digitized documents strictly for personal use. Each copy of any part of this document must contain these Terms of use. This document has been digitized, optimized for electronic delivery and stamped with digital signature within the project DML-CZ: The Czech Digital Mathematics Library http://dml.cz Czechoslovak Mathematical Journal, 56 (131) (2006), 765–772 A NOTE ON RIESZ SPACES WITH PROPERTY-b S¸. Alpay, B. Altin and C. Tonyali, Ankara (Received February 6, 2004) Abstract. We study an order boundedness property in Riesz spaces and investigate Riesz spaces and Banach lattices enjoying this property. Keywords: Riesz spaces, Banach lattices, b-property MSC 2000 : 46B42, 46B28 1. Introduction and preliminaries All Riesz spaces considered in this note have separating order duals. Therefore we will not distinguish between a Riesz space E and its image in the order bidual E∼∼. In all undefined terminology concerning Riesz spaces we will adhere to [3]. The notions of a Riesz space with property-b and b-order boundedness of operators between Riesz spaces were introduced in [1]. Definition. Let E be a Riesz space. A set A E is called b-order bounded in ⊂ E if it is order bounded in E∼∼. A Riesz space E is said to have property-b if each subset A E which is order bounded in E∼∼ remains order bounded in E. -
Contents 1. Introduction 1 2. Cones in Vector Spaces 2 2.1. Ordered Vector Spaces 2 2.2
ORDERED VECTOR SPACES AND ELEMENTS OF CHOQUET THEORY (A COMPENDIUM) S. COBZAS¸ Contents 1. Introduction 1 2. Cones in vector spaces 2 2.1. Ordered vector spaces 2 2.2. Ordered topological vector spaces (TVS) 7 2.3. Normal cones in TVS and in LCS 7 2.4. Normal cones in normed spaces 9 2.5. Dual pairs 9 2.6. Bases for cones 10 3. Linear operators on ordered vector spaces 11 3.1. Classes of linear operators 11 3.2. Extensions of positive operators 13 3.3. The case of linear functionals 14 3.4. Order units and the continuity of linear functionals 15 3.5. Locally order bounded TVS 15 4. Extremal structure of convex sets and elements of Choquet theory 16 4.1. Faces and extremal vectors 16 4.2. Extreme points, extreme rays and Krein-Milman's Theorem 16 4.3. Regular Borel measures and Riesz' Representation Theorem 17 4.4. Radon measures 19 4.5. Elements of Choquet theory 19 4.6. Maximal measures 21 4.7. Simplexes and uniqueness of representing measures 23 References 24 1. Introduction The aim of these notes is to present a compilation of some basic results on ordered vector spaces and positive operators and functionals acting on them. A short presentation of Choquet theory is also included. They grew up from a talk I delivered at the Seminar on Analysis and Optimization. The presentation follows mainly the books [3], [9], [19], [22], [25], and [11], [23] for the Choquet theory. Note that the first two chapters of [9] contains a thorough introduction (with full proofs) to some basics results on ordered vector spaces. -
Projection Bands and Atoms in Pervasive Pre-Riesz Spaces
Projection bands and atoms in pervasive pre-Riesz spaces Anke Kalauch,∗ Helena Malinowski† March 31, 2020 Abstract In vector lattices, the concept of a projection band is a basic tool. We deal with projection bands in the more general setting of an Archimedean pre-Riesz space X. We relate them to projection bands in a vector lattice cover Y of X. If X is pervasive, then a projection band in X extends to a projection band in Y , whereas the restriction of a projection band B in Y is not a projection band in X, in general. We give conditions under which the restriction of B is a projection band in X. We introduce atoms and discrete elements in X and show that every atom is discrete. The converse implication is true, provided X is pervasive. In this setting, we link atoms in X to atoms in Y . If X contains an atom a> 0, we show that the principal band generated by a is a projection band. Using atoms in a finite dimensional Archimedean pre-Riesz space X, we establish that X is pervasive if and only if it is a vector lattice. Keywords: order projection, projection band, band projection, principal band, atom, discrete element, extremal vector, pervasive, weakly pervasive, Archimedean directed ordered vector space, pre-Riesz space, vector lattice cover Mathematics Subject Classification (2010): 46A40, 06F20, 47B65 1 Introduction arXiv:1904.10420v2 [math.FA] 29 Mar 2020 Projection bands and atoms are both fundamental concepts in the vector lattice theory. For an Archimedean vector lattice Y , a band B in Y is called a projection band if Y = B ⊕ Bd, where Bd is the disjoint complement of B. -
Arxiv:1812.04035V1 [Math.OA]
The order topology on duals of C∗-algebras and von Neumann algebras EMMANUEL CHETCUTI and JAN HAMHALTER Department of Mathematics Faculty of Science University of Malta Msida, Malta [email protected] Department of Mathematics Faculty of Electrical Engineering Czech Technical University in Prague Technicka 2, 166 27 Prague 6, Czech Republic [email protected] Abstract: For a von Neumann algebra M we study the order topology associated to s the hermitian part M∗ and to intervals of the predual M∗. It is shown that the order s topology on M∗ coincides with the topology induced by the norm. In contrast to this, it is proved that the condition of having the order topology associated to the interval [0, ϕ] equal to that induced by the norm for every ϕ M +, is necessary and sufficient for the ∈ ∗ commutativity of M . It is also proved that if ϕ is a positive bounded linear functional on a C∗-algebra A , then the norm-null sequences in [0, ϕ] coincide with the null sequences with ′ respect to the order topology on [0, ϕ] if and only if the von Neumann algebra πϕ(A ) is of finite type (where πϕ denotes the corresponding GNS representation). This fact allows us to give a new topological characterization of finite von Neumann algebras. Moreover, we demonstrate that convergence to zero for norm and order topology on order-bounded parts of dual spaces are nonequivalent for all C∗-algebras that are not of Type I. 2010 MSC: 46L10, 4605, 46L30, 06F30 Key words: dual spaces of C∗-algebras, order topology arXiv:1812.04035v1 [math.OA] 10 Dec 2018 1. -
On the Schur, Positive Schur and Weak Dunford-Pettis Properties in Fr
On the Schur, positive Schur and weak Dunford-Pettis properties in Fr´echet lattices Geraldo Botelho∗ and Jos´eLucas P. Luiz† Abstract We prove some general results on sequential convergence in Fr´echet lattices that yield, as particular instances, the following results regarding a closed ideal I of a Banach lattice E: (i) If two of the lattices E, I and E/I have the positive Schur property (the Schur property, respectively) then the third lattice has the positive Schur property (the Schur property, respectively) as well; (ii) If I and E/I have the dual positive Schur property, then E also has this property; (iii) If I has the weak Dunford-Pettis property and E/I has the positive Schur property, then E has the weak Dunford-Pettis property. Examples and applications are provided. 1 Introduction In the realm of Banach spaces, the Schur property (weakly null sequences are norm null) is a 3-space property in the weak sense that a Banach space E has the Schur property whenever a closed subspace F of E and the quotient space E/F have the Schur property (see, e.g., [8]). But it is not a 3-space property in the strong sense that, given a closed subspace F of the Banach space E, if two of the spaces E, F and E/F have the Schur property, then the third one also has this property. To see that, just remember that c0 is a quotient of ℓ1. In the setting of Banach lattices, for the quotient E/F of a Banach lattice E over a closed subspace F to be a Banach lattice, F should be an ideal of E (see, e.g., [3]). -
Version of 4.9.09 Chapter 35 Riesz Spaces the Next Three Chapters Are
Version of 4.9.09 Chapter 35 Riesz spaces The next three chapters are devoted to an abstract description of the ‘function spaces’ described in Chapter 24, this time concentrating on their internal structure and relationships with their associated measure algebras. I find that any convincing account of these must involve a substantial amount of general theory concerning partially ordered linear spaces, and in particular various types of Riesz space or vector lattice. I therefore provide an introduction to this theory, a kind of appendix built into the middle of the volume. The relation of this chapter to the next two is very like the relation of Chapter 31 to Chapter 32. As with Chapter 31, it is not really meant to be read for its own sake; those with a particular interest in Riesz spaces might be better served by Luxemburg & Zaanen 71, Schaefer 74, Zaanen 83 or my own book Fremlin 74a. I begin with three sections in an easy gradation towards the particular class of spaces which we need to understand: partially ordered linear spaces (§351), general Riesz spaces (§352) and Archimedean Riesz spaces (§353); the last includes notes on Dedekind (σ-)complete spaces. These sections cover the fragments of the algebraic theory of Riesz spaces which I will use. In the second half of the chapter, I deal with normed Riesz spaces (in particular, L- and M-spaces)(§354), spaces of linear operators (§355) and dual Riesz spaces (§356). Version of 16.10.07 351 Partially ordered linear spaces I begin with an account of the most basic structures which involve an order relation on a linear space, partially ordered linear spaces. -
Nonatomic Banach Lattices Can Have /, As a Dual Space E
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 57, Number 1, May 1976 NONATOMIC BANACH LATTICES CAN HAVE /, AS A DUAL SPACE E. LACEYand p. wojtaszczyk Abstract. Examples of nonatomic M spaces whose duals are /, are constructed. In the theory of (separable) Banach lattices it is sometimes true that a space X is purely atomic if and only if X* is (for example, if X is order complete and X* is separable). However, in general, it is not true. The main purpose of this paper is to illustrate this with the following theorem on M spaces. Theorem 1. Let a be a countable ordinal (a > w). Then there is a nonatomic M space X whose dual is linearly order isometric to lx and such that X is linearly isomorphic to C(X,a~). Unexplained terminology shall be that of [5]. By an atom in a Banach lattice we shall mean an element x > 0 such that if 0 < y < x, then y = ax for some a > 0. A purely atomic Banach lattice is one in which every positive element dominates some atom and a nonatomic Banach lattice is one which admits no atoms. By <(1,a) we mean the order interval of ordinals between 1 and a with the usual order topology. The following theorem is known. We state and prove it only as background to the discussion. Theorem 2. Let X be a separable order complete Banach lattice. (a) If X is purely atomic and X* is separable, then X* is purely atomic; (b) If X* is purely atomic, then so is X. -
Hybrid High-Order Methods. a Primer with Application to Solid Mechanics. Matteo Cicuttin, Alexandre Ern, Nicolas Pignet
Hybrid high-order methods. A primer with application to solid mechanics. Matteo Cicuttin, Alexandre Ern, Nicolas Pignet To cite this version: Matteo Cicuttin, Alexandre Ern, Nicolas Pignet. Hybrid high-order methods. A primer with applica- tion to solid mechanics.. 2021. hal-03262027 HAL Id: hal-03262027 https://hal.archives-ouvertes.fr/hal-03262027 Preprint submitted on 16 Jun 2021 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. Hybrid high-order methods. A primer with applications to solid mechanics∗ Matteo Cicuttin†, Alexandre Ern‡, Nicolas Pignet§ June 16, 2021 ∗This is a preprint of the following work: M. Cicuttin, A. Ern, N. Pignet, Hybrid high-order methods. A primer with applications to solid mechanics, Springer, (in press) 2021, reproduced with the permission of the publisher. †University of Liège (Montefiore Institute), Allée de la découverte 10, B-4000 Liège, Belgium ‡CERMICS, École des Ponts, 6 & 8 avenue Blaise Pascal, F-77455 Marne-la-vallée cedex 2, France and INRIA Paris, F-75589 France §EDF R&D, 7 Boulevard Gaspard Monge, F-91120 Palaiseau, France Preface Hybrid high-order (HHO) methods attach discrete unknowns to the cells and to the faces of the mesh. -
RIESZ SPACES " Given by Prof
EUR 3140.Θ ÄO!·'· 1 \n\< tl '*·»ΤΗΗΊ)ίβ§"ίί IJM llHi 'li»**. 'tí fe É!>?jpfc EUROPEAN ATOMIC ENERGY COMMUNITY EURATOM LECTURES ON " RIESZ SPACES " given by Prof. A. C. ZAANEN iiil^{TT"1! i ■ BIT' '.'I . * . Ι'βΗΤ Editor : R. F. GLODEN !!i>M!?ÄÉ«il Siffifi 1966 loint Nuclear Research Center Ispra Establishment - Italy Scientific Information Processing Center - CETIS »»cm*if'-WW;flW4)apro 'BfiW»¡kHh;i.u·^: 2Λ*.;;, tf! :1Γ:«Μ$ ■ ■ J'ÎHO *sUr! if nb-. I;·"'-ii ;Γ^*Ε»"^Β1 hiik*MW!?5?'J.-i,K^ fill"; UP» LEGAL NOTICE This document was prepared under the sponsorship of the Commission of the European Atomic Energy Community (EURATOM). Neither the EURATOM Commission, its contractors nor any person acting- on their behalf : Make any warranty or representation, express or implied, with respect to the accuracy, completeness, or usefulness of the information contained in this document, or that the use of any information, apparatus, method, or process disclosed in this document may not infringe privately owned rights ; or Assume any liability with respect to the use of, or for damages resulting from the use of any information, apparatus, method or process disclosed in this document. This report is on sale at the addresses listed on cover page 4 at the price of FF 8.50 FB 85 DM 6.80 Lit. 1060 Fl. 6.20 When ordering, please quote the EUR number and the titl which are indicated on the cover of each report. m ■pejs!« EUR 3140.e LECTURES ON « RIESZ SPACES » given by Prof. A.C.