The Semi-M Property for Normed Riesz Spaces Compositio Mathematica, Tome 34, No 2 (1977), P
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Burkholder's Inequalities in Noncommutative Lorentz
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 138, Number 7, July 2010, Pages 2431–2441 S 0002-9939(10)10267-6 Article electronically published on March 24, 2010 BURKHOLDER’S INEQUALITIES IN NONCOMMUTATIVE LORENTZ SPACES YONG JIAO (Communicated by Marius Junge) Abstract. We prove Burkholder’s inequalities in noncommutative Lorentz spaces Lp,q(M), 1 <p<∞, 1 ≤ q<∞, associated with a von Neumann algebra M equipped with a faithful normal tracial state. These estimates generalize the classical inequalities in the commutative case. 1. Introduction Martingale inequalities and sums of independent random variables are important tools in classical harmonic analysis. A fundamental result due to Burkholder [1, 2] can be stated as follows. Given a probability space (Ω, F ,P), let {Fn}n≥1 be a nondecreasing sequence of σ-fields of F such that F = ∨Fn and let En be the conditional expectation operator relative to Fn. Given 2 ≤ p<∞ and an p L -bounded martingale f =(fn)n≥1, we have ∞ ∞ 1/2 1/p 2 p (1.1) fLp ≈ Ek−1(|df k| ) + |df k| . Lp Lp k=1 k=1 The first term on the right is called the conditioned square function of f, while the second is called the p-variation of f. Rosenthal’s inequalities [14] can be regarded as the particular case where the sequence df =(df 1,df2, ...) is a family of independent mean-zero random variables df k = ak. In this case it is easy to reduce Rosenthal’s inequalities to ∞ ∞ ∞ 1/2 1/p ≈ 2 p (1.2) ak Lp ak 2 + ak p . -
Vector Lattice Covers of Ideals and Bands in Pre-Riesz Spaces
Vector lattice covers of ideals and bands in pre-Riesz spaces Anke Kalauch,∗ Helena Malinowski† November 12, 2018 Abstract Pre-Riesz spaces are ordered vector spaces which can be order densely embedded into vector lattices, their so-called vector lattice covers. Given a vector lattice cover Y for a pre-Riesz space X, we address the question how to find vector lattice covers for subspaces of X, such as ideals and bands. We provide conditions such that for a directed ideal I in X its smallest extension ideal in Y is a vector lattice cover. We show a criterion for bands in X and their extension bands in Y as well. Moreover, we state properties of ideals and bands in X which are generated by sets, and of their extensions in Y . 1 Introduction In the analysis of partially ordered vector spaces, subspaces as ideals and bands play a central role. In vector lattices, problems involving those subspaces are broadly discussed in the literature, see e.g. [1, 15, 22]. Directed ideals in partially ordered vector spaces were introduced in [6, Definition 2.2] and studied in [2, 3, 14, 5]; for a more recent overview see [12]. The investigation of disjointness and bands in partially ordered vector spaces starts in [9], where for the definition of disjointness sets of upper bounds are used instead of lattice operations. Here a band is defined to be a set that equals its double-disjoint complement, analogously to the notion in arXiv:1801.07191v2 [math.FA] 8 Nov 2018 Archimedean vector lattices. Ideals and bands are mostly considered in pre-Riesz spaces. -
Locally Solid Riesz Spaces with Applications to Economics / Charalambos D
http://dx.doi.org/10.1090/surv/105 alambos D. Alipr Lie University \ Burkinshaw na University-Purdue EDITORIAL COMMITTEE Jerry L. Bona Michael P. Loss Peter S. Landweber, Chair Tudor Stefan Ratiu J. T. Stafford 2000 Mathematics Subject Classification. Primary 46A40, 46B40, 47B60, 47B65, 91B50; Secondary 28A33. Selected excerpts in this Second Edition are reprinted with the permissions of Cambridge University Press, the Canadian Mathematical Bulletin, Elsevier Science/Academic Press, and the Illinois Journal of Mathematics. For additional information and updates on this book, visit www.ams.org/bookpages/surv-105 Library of Congress Cataloging-in-Publication Data Aliprantis, Charalambos D. Locally solid Riesz spaces with applications to economics / Charalambos D. Aliprantis, Owen Burkinshaw.—2nd ed. p. cm. — (Mathematical surveys and monographs, ISSN 0076-5376 ; v. 105) Rev. ed. of: Locally solid Riesz spaces. 1978. Includes bibliographical references and index. ISBN 0-8218-3408-8 (alk. paper) 1. Riesz spaces. 2. Economics, Mathematical. I. Burkinshaw, Owen. II. Aliprantis, Char alambos D. III. Locally solid Riesz spaces. IV. Title. V. Mathematical surveys and mono graphs ; no. 105. QA322 .A39 2003 bib'.73—dc22 2003057948 Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society. -
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:1712.01188V2 [Math.AP]
GREEN’S FUNCTION FOR SECOND ORDER ELLIPTIC EQUATIONS WITH SINGULAR LOWER ORDER COEFFICIENTS SEICK KIM AND GEORGIOS SAKELLARIS Abstract. We construct Green’s function for second order elliptic operators of the form Lu = −∇ · (A∇u + bu) + c · ∇u + du in a domain and obtain pointwise bounds, as well as Lorentz space bounds. We assume that the matrix of principal coefficients A is uniformly elliptic and bounded and the lower order coefficients b, c, and d belong to certain Lebesgue classes and satisfy the condition d −∇· b ≥ 0. In particular, we allow the lower order coefficients to be singular. We also obtain the global pointwise bounds for the gradient of Green’s function in the case when the mean oscillations of the coefficients A and b satisfy the Dini conditions and the domain is C1,Dini. 1. Introduction Let Ω be a domain (i.e., an open connected set) in Rn with n ≥ 3. We consider second order elliptic operators in divergence form n n ij i i Lu = − Di(a (x)Dju + b (x)u) + c (x)Diu + d(x)u, iX,j=1 Xi=1 which hereafter shall be abbreviated as Lu = − div(A∇u + bu) + c · ∇u + du. We assume that the principal coefficients A = (aij) are measurable n × n matrices that are bounded and uniformly elliptic; i.e. there is a constant λ> 0 such that n λ|ξ|2 ≤ A(x)ξ · ξ = aij(x)ξiξj, ∀x ∈ Ω, ∀ξ ∈ Rn. (1.1) iX,j=1 We also assume that the lower order coefficients b = (b1,..., bn), c = (c1,..., cn), and d are such that b ∈ Lq(Ω), c ∈ Lr(Ω), d ∈ Ls(Ω) for some q, r ≥ n, s ≥ n/2. -
Fourier Analysis in Function Space Theory
Course No. 401-4463-62L Fourier Analysis in Function Space Theory Dozent: Tristan Rivi`ere Assistant: Alessandro Pigati Contents 1 The Fourier transform of tempered distributions 1 1.1 The Fourier transforms of L1 functions . 1 1.2 The Schwartz Space S(Rn)........................... 4 1.3 Frechet Spaces . 6 1.4 The space of tempered distributions S0(Rn).................. 12 1.5 Convolutions in S0(Rn)............................. 21 2 The Hardy-Littlewood Maximal Function 26 2.1 Definition and elementary properties. 26 2.2 Hardy-Littlewood Lp−theorem for the Maximal Function. 27 2.3 The limiting case p =1. ............................ 30 3 Quasi-normed vector spaces 32 3.1 The Metrizability of quasi-normed vector spaces . 32 3.2 The Lorentz spaces Lp;1 ............................ 36 3.3 Decreasing rearrangement . 37 3.4 The Lorentz spaces Lp;q ............................ 39 3.5 Functional inequalities for Lorentz spaces . 44 3.6 Dyadic characterization of some Lorentz spaces and another proof of Lorentz{ Sobolev embedding (optional) . 49 4 The Lp−theory of Calder´on-Zygmund convolution operators. 52 4.1 Calder´on-Zygmund decompositions. 52 4.2 An application of Calder´on-Zygmund decomposition . 54 4.3 The Marcinkiewicz Interpolation Theorem - The Lp case . 56 4.4 Calderon Zygmund Convolution Operators over Lp ............. 58 4.4.1 A \primitive" formulation . 60 4.4.2 A singular integral type formulation . 64 4.4.3 The case of homogeneous kernels . 69 4.4.4 A multiplier type formulation . 71 4.4.5 Applications: The Lp theory of the Riesz Transform and the Laplace and Bessel Operators . 74 4.4.6 The limiting case p =1........................ -
Weak-Type Weights and Normable Lorentz Spaces 1
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 124, Number 3, March 1996 WEAK-TYPE WEIGHTS AND NORMABLE LORENTZ SPACES MAR´IA J. CARRO, ALEJANDRO GARC´IA DEL AMO, AND JAVIER SORIA (Communicated by J. Marshall Ash) Abstract. We show that the Lorentz space Λ1(w) is a Banach space if and only if the Hardy-Littlewood maximal operator M satisfies a certain weak-type estimate. We also consider the case of general measures. Finally, we study some properties of several indices associated to these spaces. 1. Introduction We are going to study weighted Lorentz spaces of functions defined in Rn as follows (for standard notation we refer to [BS] and [GR]): If u is a weight in Rn, + w is a weight in R , fu∗ denotes the decreasing rearrangement of f with respect to the measure u(x) dx and 0 <p< , we define ∞ 1/p ∞ p p p Λu(w)= f; f Λu(w) = fu∗(t) w(t)dt < . k k 0 ∞ Z If u 1, we will only write Λp(w). Classical examples are obtained by choosing ≡ (p/q) 1 p q,p w(t)=t − .InthiscaseΛ(w)=L . A classical result of G.G. Lorentz (see [Lo]) shows that Λ1(w) is a norm, if and only if, w is a decreasing function. The problem of findingk·k conditions on w so that Λp(w) is a Banach space (that is, there exists a norm equivalent to Λp(w)) was solved, for p>1, by E. Sawyer ([Sa]). This condition is that the Hardy-Littlewoodk·k maximal operator is bounded on Λp(w). -
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. -
HARDY-TYPE OPERATORS in LORENTZ-TYPE SPACES DEFINED on MEASURE SPACES1 Qinxiu Sun∗, Xiao Yu∗∗ and Hongliang Li∗∗∗
Indian J. Pure Appl. Math., 51(3): 1105-1132, September 2020 °c Indian National Science Academy DOI: 10.1007/s13226-020-0453-1 HARDY-TYPE OPERATORS IN LORENTZ-TYPE SPACES DEFINED ON MEASURE SPACES1 Qinxiu Sun¤, Xiao Yu¤¤ and Hongliang Li¤¤¤ ¤Department of Mathematics, Zhejiang University of Science and Technology, Hangzhou 310023, China ¤¤Department of Mathematics, Shangrao Normal University, Shangrao 334001, China ¤¤¤Department of Mathematics, Zhejiang International Studies University, Hangzhou 310012, China e-mail: [email protected] (Received 2 June 2018; accepted 12 June 2019) Weight criteria for the boundedness and compactness of generalized Hardy-type operators Z T f(x) = u1(x) f(y)u2(y)v0(y) d¹(y); x 2 X; (0.1) fÁ(y)·Ã(x)g in Orlicz-Lorentz spaces defined on measure spaces is investigated where the functions Á; Ã; u1; u2; v0 are positive measurable functions. Some sufficient conditions of boundedness of G0 G1 G0 G1;1 T :Λv0 (w0) ! Λv1 (w1) and T :Λv0 (w0) ! Λv1 (w1) are obtained on Orlicz-Lorentz spaces. Furthermore, we achieve sufficient and necessary conditions for T to be bounded and p0 p1;q1 compact from a weighted Lorentz space Λv0 (w0) to another Λv1 (w1). It is notable that the function spaces concerned here are quasi-Banach spaces instead of Banach spaces. Key words : Hardy operator; Orlicz-Lorentz spaces; weighted Lorentz spaces; boundedness; compactness. 2010 Mathematics Subject Classification : 46E30, 46B42. 1. INTRODUCTION R x For the Hardy operator S defined by Sf(x) = 0 f(t)dt, the weighted Lebesgue-norm inequalities have been characterized by many authors (e.g. -
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.