Evaluarea Ordinului De Aproximare Prin Operatori Liniari Si Pozitivi
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NORMS of POSITIVE OPERATORS on Lp-SPACES
NORMS OF POSITIVE OPERATORS ON Lp-SPACES Ralph Howard* Anton R. Schep** University of South Carolina p q ct. ≤ → Abstra Let 0 T : L (Y,ν) L (X,µ) be a positive linear operator and let kT kp,q denote its operator norm. In this paper a method is given to compute kT kp,q exactly or to bound kT kp,q from above. As an application the exact norm kV kp,q of R x the Volterra operator Vf(x)= 0 f(t)dt is computed. 1. Introduction ≤ ∞ p For 1 p< let L [0, 1] denote the Banach space of (equivalenceR classes of) 1 1 k k | |p p Lebesgue measurable functions on [0,1] with the usual norm f p =( 0 f dt) . For a pair p, q with 1 ≤ p, q < ∞ and a continuous linear operator T : Lp[0, 1] → Lq[0, 1] the operator norm is defined as usual by (1-1) kT kp,q =sup{kTfkq : kfkp =1}. Define the Volterra operator V : Lp[0, 1] → Lq[0, 1] by Z x (1-2) Vf(x)= f(t)dt. 0 The purpose of this note is to show that for a class of linear operators T between Lp spaces which are positive (i.e. f ≥ 0 a.e. implies Tf ≥ 0 a.e.) the problem of computing the exact value of kT kp,q can be reduced to showing that a certain nonlinear functional equation has a nonnegative solution. We shall illustrate this by computing the value of kV kp,q for V defined by (1-2) above. -
ON the SPECTRUM of POSITIVE OPERATORS by Cheban P
ON THE SPECTRUM OF POSITIVE OPERATORS by Cheban P. Acharya A Dissertation Submitted to the Faculty of The Charles E. Schmidt College of Science in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy Florida Atlantic University Boca Raton, FL August 2012 Copyright by Cheban P. Acharya 2012 ii ACKNOWLEDGEMENTS I would like to express my sincere gratitude to my Ph.D. advisor, Prof. Dr. X. D. Zhang, for his precious guidance and encouragement throughout the research. I am sure it would have not been possible without his help. Besides I would like to thank the faculty and the staffs of the Department of Mathematics who always gave me support by various ways. I will never forget their help during my whole graduate study. And I also would like to thank all members of my thesis's committee. I would like to thank my wife Parbati for her personal support and great pa- tience all the time. My sons (Shishir and Sourav), mother, father, brother, and cousin have given me their support throughout, as always, for which my mere expression of thanks does not suffice. Last, but by no means least, I thank my colleagues in Mathematics department of Florida Atlantic University for their support and encouragement throughout my stay in school. iv ABSTRACT Author: Cheban P. Acharya Title: On The Spectrum of Positive Operators Institution: Florida Atlantic University Dissertation Advisor: Dr. Xiao Dong Zhang Degree: Doctor of Philosophy Year: 2012 It is known that lattice homomorphisms and G-solvable positive operators on Banach lattices have cyclic peripheral spectrum (see [17]). -
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. -
IRJET-V3I8330.Pdf
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395 -0056 Volume: 03 Issue: 08 | Aug-2016 www.irjet.net p-ISSN: 2395-0072 A comprehensive study on different approximation methods of Fractional order system Asif Iqbal and Rakesh Roshon Shekh P.G Scholar, Dept. of Electrical Engineering, NITTTR, Kolkata, West Bengal, India P.G Scholar, Dept. of Electrical Engineering, NITTTR, Kolkata, West Bengal, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Many natural phenomena can be more infinite dimensional (i.e. infinite memory). So for analysis, accurately modeled using non-integer or fractional order controller design, signal processing etc. these infinite order calculus. As the fractional order differentiator is systems are approximated by finite order integer order mathematically equivalent to infinite dimensional filter, it’s system in a proper range of frequencies of practical interest proper integer order approximation is very much important. [1], [2]. In this paper four different approximation methods are given and these four approximation methods are applied on two different examples and the results are compared both in time 1.1 FRACTIONAL CALCULAS: INRODUCTION domain and in frequency domain. Continued Fraction Expansion method is applied on a fractional order plant model Fractional Calculus [3], is a generalization of integer order and the approximated model is converted to its equivalent calculus to non-integer order fundamental operator D t , delta domain model. Then step response of both delta domain l and continuous domain model is shown. where 1 and t is the lower and upper limit of integration and Key Words: Fractional Order Calculus, Delta operator the order of operation is . -
High Order Gradient, Curl and Divergence Conforming Spaces, with an Application to NURBS-Based Isogeometric Analysis
High order gradient, curl and divergence conforming spaces, with an application to compatible NURBS-based IsoGeometric Analysis R.R. Hiemstraa, R.H.M. Huijsmansa, M.I.Gerritsmab aDepartment of Marine Technology, Mekelweg 2, 2628CD Delft bDepartment of Aerospace Technology, Kluyverweg 2, 2629HT Delft Abstract Conservation laws, in for example, electromagnetism, solid and fluid mechanics, allow an exact discrete representation in terms of line, surface and volume integrals. We develop high order interpolants, from any basis that is a partition of unity, that satisfy these integral relations exactly, at cell level. The resulting gradient, curl and divergence conforming spaces have the propertythat the conservationlaws become completely independent of the basis functions. This means that the conservation laws are exactly satisfied even on curved meshes. As an example, we develop high ordergradient, curl and divergence conforming spaces from NURBS - non uniform rational B-splines - and thereby generalize the compatible spaces of B-splines developed in [1]. We give several examples of 2D Stokes flow calculations which result, amongst others, in a point wise divergence free velocity field. Keywords: Compatible numerical methods, Mixed methods, NURBS, IsoGeometric Analyis Be careful of the naive view that a physical law is a mathematical relation between previously defined quantities. The situation is, rather, that a certain mathematical structure represents a given physical structure. Burke [2] 1. Introduction In deriving mathematical models for physical theories, we frequently start with analysis on finite dimensional geometric objects, like a control volume and its bounding surfaces. We assign global, ’measurable’, quantities to these different geometric objects and set up balance statements. -
Reflexive Cones
Reflexive cones∗ E. Casini† E. Miglierina‡ I.A. Polyrakis§ F. Xanthos¶ November 10, 2018 Abstract Reflexive cones in Banach spaces are cones with weakly compact in- tersection with the unit ball. In this paper we study the structure of this class of cones. We investigate the relations between the notion of reflexive cones and the properties of their bases. This allows us to prove a characterization of reflexive cones in term of the absence of a subcone isomorphic to the positive cone of ℓ1. Moreover, the properties of some specific classes of reflexive cones are investigated. Namely, we consider the reflexive cones such that the intersection with the unit ball is norm compact, those generated by a Schauder basis and the reflexive cones re- garded as ordering cones in Banach spaces. Finally, it is worth to point out that a characterization of reflexive spaces and also of the Schur spaces by the properties of reflexive cones is given. Keywords Cones, base for a cone, vector lattices, ordered Banach spaces, geometry of cones, weakly compact sets, reflexivity, positive Schauder bases. Mathematics Subject Classification (2010) 46B10, 46B20, 46B40, 46B42 1 Introduction The study of cones is central in many fields of pure and applied mathematics. In Functional Analysis, the theory of partially ordered spaces and Riesz spaces arXiv:1201.4927v2 [math.FA] 28 May 2012 ∗The last two authors of this research have been co-financed by the European Union (Euro- pean Social Fund - ESF)and Greek national funds through the Operational Program "Educa- tion and Lifelong Learning" of the National Strategic Reference Framework (NSRF) - Research Funding Program: Heracleitus II. -
Numerical Integration and Differentiation Growth And
Numerical Integration and Differentiation Growth and Development Ra¨ulSantaeul`alia-Llopis MOVE-UAB and Barcelona GSE Spring 2017 Ra¨ulSantaeul`alia-Llopis(MOVE,UAB,BGSE) GnD: Numerical Integration and Differentiation Spring 2017 1 / 27 1 Numerical Differentiation One-Sided and Two-Sided Differentiation Computational Issues on Very Small Numbers 2 Numerical Integration Newton-Cotes Methods Gaussian Quadrature Monte Carlo Integration Quasi-Monte Carlo Integration Ra¨ulSantaeul`alia-Llopis(MOVE,UAB,BGSE) GnD: Numerical Integration and Differentiation Spring 2017 2 / 27 Numerical Differentiation The definition of the derivative at x∗ is 0 f (x∗ + h) − f (x∗) f (x∗) = lim h!0 h Ra¨ulSantaeul`alia-Llopis(MOVE,UAB,BGSE) GnD: Numerical Integration and Differentiation Spring 2017 3 / 27 • Hence, a natural way to numerically obtain the derivative is to use: f (x + h) − f (x ) f 0(x ) ≈ ∗ ∗ (1) ∗ h with a small h. We call (1) the one-sided derivative. • Another way to numerically obtain the derivative is to use: f (x + h) − f (x − h) f 0(x ) ≈ ∗ ∗ (2) ∗ 2h with a small h. We call (2) the two-sided derivative. We can show that the two-sided numerical derivative has a smaller error than the one-sided numerical derivative. We can see this in 3 steps. Ra¨ulSantaeul`alia-Llopis(MOVE,UAB,BGSE) GnD: Numerical Integration and Differentiation Spring 2017 4 / 27 • Step 1, use a Taylor expansion of order 3 around x∗ to obtain 0 1 00 2 1 000 3 f (x) = f (x∗) + f (x∗)(x − x∗) + f (x∗)(x − x∗) + f (x∗)(x − x∗) + O3(x) (3) 2 6 • Step 2, evaluate the expansion (3) at x -
Quadrature Formulas and Taylor Series of Secant and Tangent
QUADRATURE FORMULAS AND TAYLOR SERIES OF SECANT AND TANGENT Yuri DIMITROV1, Radan MIRYANOV2, Venelin TODOROV3 1 University of Forestry, Sofia, Bulgaria [email protected] 2 University of Economics, Varna, Bulgaria [email protected] 3 Bulgarian Academy of Sciences, IICT, Department of Parallel Algorithms, Sofia, Bulgaria [email protected] Abstract. Second-order quadrature formulas and their fourth-order expansions are derived from the Taylor series of the secant and tangent functions. The errors of the approximations are compared to the error of the midpoint approximation. Third and fourth order quadrature formulas are constructed as linear combinations of the second- order approximations and the trapezoidal approximation. Key words: Quadrature formula, Fourier transform, generating function, Euler- Mclaurin formula. 1. Introduction Numerical quadrature is a term used for numerical integration in one dimension. Numerical integration in more than one dimension is usually called cubature. There is a broad class of computational algorithms for numerical integration. The Newton-Cotes quadrature formulas (1.1) are a group of formulas for numerical integration where the integrand is evaluated at equally spaced points. Let . The two most popular approximations for the definite integral are the trapezoidal approximation (1.2) and the midpoint approximation (1.3). The midpoint approximation and the trapezoidal approximation for the definite integral are Newton-Cotes quadrature formulas with accuracy . The trapezoidal and the midpoint approximations are constructed by dividing the interval to subintervals of length and interpolating the integrand function by Lagrange polynomials of degree zero and one. Another important Newton-Cotes quadrat -order accuracy and is obtained by interpolating the function by a second degree Lagrange polynomial. -
Inapril 3, 1970
AN ABSTRACT OF THE THESIS OF Ralph Leland James for theDoctor of Philosophy (Name) (Degree) inAprilMathematics 3,presented 1970on (Major) (Date) Title: CONVERGENCE OF POSITIVE OPERATORS Abstract approved: Redacted for Privacy P. M. Anselone The extension and convergence of positiveoperators is investi- gated by means of a monotone approximation technique.Some gener- alizations and extensions of Korovkin's monotoneoperator theorem on C[0, 1] are given. The concept of a regular set is introduced and it is shownthat pointwise convergence is uniform on regular sets.Regular sets are investigated in various spaces andsome characterizations are obtained. These concepts are applied to the approximate solutionof a large class of integral equations. Convergence of Positive Operators by Ralph Leland James A THESIS submitted to Oregon State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy June 1970 APPROVED: Redacted for Privacy P nf eS ::33r of _Department of Ma,thernat ic s in charge of major Redacted for Privacy ActingChairman o Department of Mathematics Redacted for Privacy Dean of Graduate School Date thesis is presented April 3, 1970 Typed by Barbara Eby for Ralph Leland James ACKNOWLEDGEMENT I wish to express my appreciation to Professor P. M.Anselone for his guidance and encouragement during the preparation ofthis thesis. CONVERGENCE OF POSITIVE OPERATORS I.INTRODUCTION §1.Historical Remarks The ordinary Riemann integral can be regarded as an extension of the integral of a continuous function to a larger space in the follow- ing way.Let (1,03,C denote respectively the linear spaces of all, bounded, and continuous real valued functions on [0, 1] .For x in define 1 P0 x = x(t)dt is posi- thenP0is a linear functional defined on C. -
Interpolation Polynomials Which Give Best Order Of
transactions of the american mathematical society Volume 200, 1974 INTERPOLATIONPOLYNOMIALS WHICH GIVE BEST ORDER OF APPROXIMATIONAMONG CONTINUOUSLY DIFFERENTIABLE FUNCTIONSOF ARBITRARYFIXED ORDER ON [-1, +1] by A. K. VARMA Dedicated to Professor P. Turan ABSTRACT. The object of this paper is to show that there exists a poly- nomial Pn(x) of degree < 2n — 1 which interpolates a given function exactly at the zeros of nth Tchebycheff polynomial and for which \\f —Pn\\ < Ckwk(iln> f) where wfc(l/n, /) is the modulus of continuity of / of fcth order. 1. Introduction. The classical theorems of D. Jackson extend the Weierstrass approximation theorem by giving quantitative information on the degree of ap- proximation to a continuous function in terms of its smoothness. Specifically, Jackson proved Theorem 1. Let f(x) be continuous for \x\ < 1 and have modulus of continuity w(t). Then there exists a polynomial P(x) of degree n at most suchthat \f(x)-P(x)\ <Aw(l/n) for \x\ < 1, where A is a positive numer- ical constant. In 1951 S. B. Steckin [3] made an important generalization of the Jackson theorem. Theorem 2 (S. B. Steckin). Let k be a positive integer; then there exists a positive constant Ck such that for every fE C[-\, +1] we can find an algebraic polynomial Pn(x) of degree n so that (1.1) Hf-Pn\\<Ckwk(l/n,f), where wk(l/n, f) is the modulus of continuity of f(x) of kth order. During personal conversation in Poznan, S. B. Steckin raised the following Presented to the Society, April 20, 1973; received by the editors March 23, 1973 and, in revised form, December 7, 1973. -
"FOSLS on Curved Boundaries"
Approximated Flux Boundary Conditions for Raviart-Thomas Finite Elements on Domains with Curved Boundaries and Applications to First-Order System Least Squares von der Fakultät für Mathematik und Physik der Gottfried Wilhelm Leibniz Universität Hannover zur Erlangung des akademischen Grades Doktor der Naturwissenschaften Dr. rer. nat. genehmigte Dissertation von Dipl.-Math. Fleurianne Bertrand geboren am 06.06.1987 in Caen (Frankreich) 2014 2 Referent: Prof. Dr. Gerhard Starke Universität Duisburg-Essen Fakultät für Mathematik Thea-Leymann-Straße 9 45127 Essen Korreferent: Prof. Dr. James Adler Department of Mathematics Tufts University Bromfield-Pearson Building 503 Boston Avenue Medford, MA 02155 Korreferent: Prof. Dr. Joachim Escher Institut für Angewandte Mathematik Gottfried Wilhelm Leibniz Universität Hannover Welfengarten 1 30167 Hannover Tag der Promotion: 15.07.2014 Acknowledgement: This work was supported by the German Research Foundation (DFG) under grant STA402/10-1. 3 Abstract Optimal order convergence of a first-order system least squares method using lowest-order Raviart-Thomas elements combined with linear conforming elements is shown for domains with curved boundaries. Parametric Raviart-Thomas elements are presented in order to retain the optimal order of convergence in the higher-order case in combination with the isoparametric scalar elements. In particular, an estimate for the normal flux of the Raviart-Thomas elements on interpolated boundaries is derived in both cases. This is illustrated numerically for the Pois- son problem on the unit disk. As an application of the analysis derived for the Poisson problem, the effect of interpolated interface condition for a stationary two-phase flow problem is then studied. Keywords: Raviart-Thomas, Curved Boundaries, First-Order System Least Squares 4 Zusammenfassung Für Gebiete mit gekrümmten Rändern wird die optimale Konvergenzordnung einer Least Squares finite Elemente Methode für Systeme erster Ordnung mit Raviart-Thomas Elementen niedrig- ster Ordnung und linearen konformen Elementen gezeigt. -
Order of Approximation of Functions of Two Variables by New Type Gamma Operators1 Aydın Izgi˙
General Mathematics Vol. 17, No. 1 (2009), 23–32 Order of approximation of functions of two variables by new type gamma operators1 Aydın Izgi˙ Abstract The theorems on weighetd approximation and order of approxi- mation of continuous functions of two variables by new type Gamma operators on all positive square region are established. 2000 Mathematics Subject Classification: 41A25,41A36 Key words and phrases: Order of approximation,weighted approximation,new type Gamma operators. 1 Introduction Lupa¸sand M¨uller[11] introduced the sequence of linear positive ope- rators {Gn},Gn : C(0, ∞) → C(0, ∞) defined by ∞ n G (f; x)= g (x, u)f( )du n n u Z0 xn+1 G is called Gamma operator, where g (x, u)= e−xuun,x> 0. n n n! 1Received 15 February, 2008 Accepted for publication (in revised form) 21 March, 2008 23 24 Aydın Izgi˙ Mazhar [12] used same gn(x, u) of Gamma operator and introduced the following sequence of linear positive operators: ∞ ∞ Fn(f; x) = gn(x, u)du gn−1(u, t)f(t)dt Z0 Z0 ∞ (2n)!xn+1 tn−1 = f(t)dt, n > 1,x> 0 n!(n − 1)! (x + t)2n+1 Z0 for any f which the last integral is convergent. Now we will modify the ope- rators Fn(f; x) as the following operators An(f; x) (see [9]) which confirm 2 2 An(t ; x) = x . Many linear operators Ln (f; x) confirm, Ln (1; x) = 1, 2 2 Ln (t; x)= x but don’t confirm Ln (t ; x)= x (see [2],[10]).