MAT218A NOTES December 10, 2017
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Arxiv:0704.2891V3 [Math.AG] 5 Dec 2007 Schwartz Functions on Nash Manifolds
Schwartz functions on Nash manifolds Avraham Aizenbud and Dmitry Gourevitch ∗ July 11, 2011 Abstract In this paper we extend the notions of Schwartz functions, tempered func- tions and generalized Schwartz functions to Nash (i.e. smooth semi-algebraic) manifolds. We reprove for this case classically known properties of Schwartz functions on Rn and build some additional tools which are important in rep- resentation theory. Contents 1 Introduction 2 1.1 Mainresults................................ 3 1.2 Schwartz sections of Nash bundles . 4 1.3 Restricted topologyand sheaf properties . .... 4 1.4 Possibleapplications ........................... 5 1.5 Summary ................................. 6 1.6 Remarks.................................. 6 2 Semi-algebraic geometry 8 2.1 Basicnotions ............................... 8 arXiv:0704.2891v3 [math.AG] 5 Dec 2007 2.2 Tarski-Seidenberg principle of quantifier elimination anditsapplications............................ 8 2.3 Additional preliminary results . .. 10 ∗Avraham Aizenbud and Dmitry Gourevitch, Faculty of Mathematics and Computer Science, The Weizmann Institute of Science POB 26, Rehovot 76100, ISRAEL. E-mails: [email protected], [email protected]. Keywords: Schwartz functions, tempered functions, generalized functions, distributions, Nash man- ifolds. 1 3 Nash manifolds 11 3.1 Nash submanifolds of Rn ......................... 11 3.2 Restricted topological spaces and sheaf theory over them........ 12 3.3 AbstractNashmanifolds . 14 3.3.1 ExamplesandRemarks. 14 3.4 Nashvectorbundles ........................... 15 3.5 Nashdifferentialoperators . 16 3.5.1 Algebraic differential operators on a Nash manifold . .... 17 3.6 Nashtubularneighborhood . 18 4 Schwartz and tempered functions on affine Nash manifolds 19 4.1 Schwartzfunctions ............................ 19 4.2 Temperedfunctions. .. .. .. 20 4.3 Extension by zero of Schwartz functions . .. 20 4.4 Partitionofunity ............................. 21 4.5 Restriction and sheaf property of tempered functions . -
Geometric Integration Theory Contents
Steven G. Krantz Harold R. Parks Geometric Integration Theory Contents Preface v 1 Basics 1 1.1 Smooth Functions . 1 1.2Measures.............................. 6 1.2.1 Lebesgue Measure . 11 1.3Integration............................. 14 1.3.1 Measurable Functions . 14 1.3.2 The Integral . 17 1.3.3 Lebesgue Spaces . 23 1.3.4 Product Measures and the Fubini–Tonelli Theorem . 25 1.4 The Exterior Algebra . 27 1.5 The Hausdorff Distance and Steiner Symmetrization . 30 1.6 Borel and Suslin Sets . 41 2 Carath´eodory’s Construction and Lower-Dimensional Mea- sures 53 2.1 The Basic Definition . 53 2.1.1 Hausdorff Measure and Spherical Measure . 55 2.1.2 A Measure Based on Parallelepipeds . 57 2.1.3 Projections and Convexity . 57 2.1.4 Other Geometric Measures . 59 2.1.5 Summary . 61 2.2 The Densities of a Measure . 64 2.3 A One-Dimensional Example . 66 2.4 Carath´eodory’s Construction and Mappings . 67 2.5 The Concept of Hausdorff Dimension . 70 2.6 Some Cantor Set Examples . 73 i ii CONTENTS 2.6.1 Basic Examples . 73 2.6.2 Some Generalized Cantor Sets . 76 2.6.3 Cantor Sets in Higher Dimensions . 78 3 Invariant Measures and the Construction of Haar Measure 81 3.1 The Fundamental Theorem . 82 3.2 Haar Measure for the Orthogonal Group and the Grassmanian 90 3.2.1 Remarks on the Manifold Structure of G(N,M).... 94 4 Covering Theorems and the Differentiation of Integrals 97 4.1 Wiener’s Covering Lemma and its Variants . -
Uniform Boundedness Principle for Unbounded Operators
UNIFORM BOUNDEDNESS PRINCIPLE FOR UNBOUNDED OPERATORS C. GANESA MOORTHY and CT. RAMASAMY Abstract. A uniform boundedness principle for unbounded operators is derived. A particular case is: Suppose fTigi2I is a family of linear mappings of a Banach space X into a normed space Y such that fTix : i 2 Ig is bounded for each x 2 X; then there exists a dense subset A of the open unit ball in X such that fTix : i 2 I; x 2 Ag is bounded. A closed graph theorem and a bounded inverse theorem are obtained for families of linear mappings as consequences of this principle. Some applications of this principle are also obtained. 1. Introduction There are many forms for uniform boundedness principle. There is no known evidence for this principle for unbounded operators which generalizes classical uniform boundedness principle for bounded operators. The second section presents a uniform boundedness principle for unbounded operators. An application to derive Hellinger-Toeplitz theorem is also obtained in this section. A JJ J I II closed graph theorem and a bounded inverse theorem are obtained for families of linear mappings in the third section as consequences of this principle. Go back Let us assume the following: Every vector space X is over R or C. An α-seminorm (0 < α ≤ 1) is a mapping p: X ! [0; 1) such that p(x + y) ≤ p(x) + p(y), p(ax) ≤ jajαp(x) for all x; y 2 X Full Screen Close Received November 7, 2013. 2010 Mathematics Subject Classification. Primary 46A32, 47L60. Key words and phrases. -
On the Use of Discrete Fourier Transform for Solving Biperiodic Boundary Value Problem of Biharmonic Equation in the Unit Rectangle
On the Use of Discrete Fourier Transform for Solving Biperiodic Boundary Value Problem of Biharmonic Equation in the Unit Rectangle Agah D. Garnadi 31 December 2017 Department of Mathematics, Faculty of Mathematics and Natural Sciences, Bogor Agricultural University Jl. Meranti, Kampus IPB Darmaga, Bogor, 16680 Indonesia Abstract This note is addressed to solving biperiodic boundary value prob- lem of biharmonic equation in the unit rectangle. First, we describe the necessary tools, which is discrete Fourier transform for one di- mensional periodic sequence, and then extended the results to 2- dimensional biperiodic sequence. Next, we use the discrete Fourier transform 2-dimensional biperiodic sequence to solve discretization of the biperiodic boundary value problem of Biharmonic Equation. MSC: 15A09; 35K35; 41A15; 41A29; 94A12. Key words: Biharmonic equation, biperiodic boundary value problem, discrete Fourier transform, Partial differential equations, Interpola- tion. 1 Introduction This note is an extension of a work by Henrici [2] on fast solver for Poisson equation to biperiodic boundary value problem of biharmonic equation. This 1 note is organized as follows, in the first part we address the tools needed to solve the problem, i.e. introducing discrete Fourier transform (DFT) follows Henrici's work [2]. The second part, we apply the tools already described in the first part to solve discretization of biperiodic boundary value problem of biharmonic equation in the unit rectangle. The need to solve discretization of biharmonic equation is motivated by its occurence in some applications such as elasticity and fluid flows [1, 4], and recently in image inpainting [3]. Note that the work of Henrici [2] on fast solver for biperiodic Poisson equation can be seen as solving harmonic inpainting. -
Introduction to Sobolev Spaces
Introduction to Sobolev Spaces Lecture Notes MM692 2018-2 Joa Weber UNICAMP December 23, 2018 Contents 1 Introduction1 1.1 Notation and conventions......................2 2 Lp-spaces5 2.1 Borel and Lebesgue measure space on Rn .............5 2.2 Definition...............................8 2.3 Basic properties............................ 11 3 Convolution 13 3.1 Convolution of functions....................... 13 3.2 Convolution of equivalence classes................. 15 3.3 Local Mollification.......................... 16 3.3.1 Locally integrable functions................. 16 3.3.2 Continuous functions..................... 17 3.4 Applications.............................. 18 4 Sobolev spaces 19 4.1 Weak derivatives of locally integrable functions.......... 19 1 4.1.1 The mother of all Sobolev spaces Lloc ........... 19 4.1.2 Examples........................... 20 4.1.3 ACL characterization.................... 21 4.1.4 Weak and partial derivatives................ 22 4.1.5 Approximation characterization............... 23 4.1.6 Bounded weakly differentiable means Lipschitz...... 24 4.1.7 Leibniz or product rule................... 24 4.1.8 Chain rule and change of coordinates............ 25 4.1.9 Equivalence classes of locally integrable functions..... 27 4.2 Definition and basic properties................... 27 4.2.1 The Sobolev spaces W k;p .................. 27 4.2.2 Difference quotient characterization of W 1;p ........ 29 k;p 4.2.3 The compact support Sobolev spaces W0 ........ 30 k;p 4.2.4 The local Sobolev spaces Wloc ............... 30 4.2.5 How the spaces relate.................... 31 4.2.6 Basic properties { products and coordinate change.... 31 i ii CONTENTS 5 Approximation and extension 33 5.1 Approximation............................ 33 5.1.1 Local approximation { any domain............. 33 5.1.2 Global approximation on bounded domains....... -
Proving the Regularity of the Reduced Boundary of Perimeter Minimizing Sets with the De Giorgi Lemma
PROVING THE REGULARITY OF THE REDUCED BOUNDARY OF PERIMETER MINIMIZING SETS WITH THE DE GIORGI LEMMA Presented by Antonio Farah In partial fulfillment of the requirements for graduation with the Dean's Scholars Honors Degree in Mathematics Honors, Department of Mathematics Dr. Stefania Patrizi, Supervising Professor Dr. David Rusin, Honors Advisor, Department of Mathematics THE UNIVERSITY OF TEXAS AT AUSTIN May 2020 Acknowledgements I deeply appreciate the continued guidance and support of Dr. Stefania Patrizi, who supervised the research and preparation of this Honors Thesis. Dr. Patrizi kindly dedicated numerous sessions to this project, motivating and expanding my learning. I also greatly appreciate the support of Dr. Irene Gamba and of Dr. Francesco Maggi on the project, who generously helped with their reading and support. Further, I am grateful to Dr. David Rusin, who also provided valuable help on this project in his role of Honors Advisor in the Department of Mathematics. Moreover, I would like to express my gratitude to the Department of Mathematics' Faculty and Administration, to the College of Natural Sciences' Administration, and to the Dean's Scholars Honors Program of The University of Texas at Austin for my educational experience. 1 Abstract The Plateau problem consists of finding the set that minimizes its perimeter among all sets of a certain volume. Such set is known as a minimal set, or perimeter minimizing set. The problem was considered intractable until the 1960's, when the development of geometric measure theory by researchers such as Fleming, Federer, and De Giorgi provided the necessary tools to find minimal sets. -
TERMINOLOGY UNIT- I Finite Element Method (FEM)
TERMINOLOGY UNIT- I The Finite Element Method (FEM) is a numerical technique to find Finite Element approximate solutions of partial differential equations. It was originated from Method (FEM) the need of solving complex elasticity and structural analysis problems in Civil, Mechanical and Aerospace engineering. Any continuum/domain can be divided into a number of pieces with very Finite small dimensions. These small pieces of finite dimension are called Finite Elements Elements. Field The field variables, displacements (strains) & stresses or stress resultants must Conditions satisfy the governing condition which can be mathematically expressed. A set of independent functions satisfying the boundary conditions is chosen Functional and a linear combination of a finite number of them is taken to approximately Approximation specify the field variable at any point. A structure can have infinite number of displacements. Approximation with a Degrees reasonable level of accuracy can be achieved by assuming a limited number of of Freedom displacements. This finite number of displacements is the number of degrees of freedom of the structure. The formulation for structural analysis is generally based on the three Numerical fundamental relations: equilibrium, constitutive and compatibility. There are Methods two major approaches to the analysis: Analytical and Numerical. Analytical approach which leads to closed-form solutions is effective in case of simple geometry, boundary conditions, loadings and material properties. Analytical However, in reality, such simple cases may not arise. As a result, various approach numerical methods are evolved for solving such problems which are complex in nature. For numerical approach, the solutions will be approximate when any of these Numerical relations are only approximately satisfied. -
Mean Growth of the Derivative of Analytic Functions, Bounded Mean Oscillation and Normal Functions
MEAN GROWTH OF THE DERIVATIVE OF ANALYTIC FUNCTIONS, BOUNDED MEAN OSCILLATION AND NORMAL FUNCTIONS Oscar Blasco, Daniel Girela and M. Auxiliadora Marquez´ Abstract. For a given positive function φ defined in [0, 1) and 1 ≤ p<∞, we consider L the space (p, φ) which consists of all functions f analytic in the unit disc ∆ for which 1/p 1 π iθ p → 2π −π f (re ) dθ =O(φ(r)), as r 1.A result of Bourdon, Shapiro and Sledd 1 −1 implies that such a space is contained in BMOA for φ(r)=(1− r) p .Among other results, in this paper we prove that this result is sharp in a very strong sense, showing that, 1 −1 for a large class of weight functions φ, the function φ(r)=(1− r) p is the best one to 1− 1 get L(p, φ) ⊂ BMOA.Actually, if φ(r)(1 − r) p ↑∞,asr ↑ 1, we construct a function f ∈L(p, φ) which is not a normal function.These results improve other obtained recently by the second author.We also characterize the functions φ, among a certain class of weight functions, to be able to embedd L(p, φ)intoHq for q>por into the space B of Bloch functions. 1. Introduction and statement of results. Let ∆ denote the unit disc {z ∈ C : |z| < 1} and T the unit circle {ξ ∈ C : |ξ| =1}.If 0 <r<1 and g is a function which is analytic in ∆, we set π 1/p 1 iθ p Mp(r, g)= g(re ) dθ , 0 <p<∞, 2π −π M∞(r, g) = max |g(z)|. -
Bibliography
Bibliography [1] E. Abe, Hopf algebras. Cambridge University Press, 1980. [2] M. Abramowitz and I.A. Stegun, Handbook of mathematical functions. United States Department of Commerce, 1965. [3] M.S. Agranovich, Spectral properties of elliptic pseudodifferential operators on a closed curve. (Russian) Funktsional. Anal. i Prilozhen. 13 (1979), no. 4, 54–56. (English translation in Functional Analysis and Its Applications. 13, p. 279–281.) [4] M.S. Agranovich, Elliptic pseudodifferential operators on a closed curve. (Russian) Trudy Moskov. Mat. Obshch. 47 (1984), 22–67, 246. (English translation in Transactions of Moscow Mathematical Society. 47, p. 23–74.) [5] M.S. Agranovich, Elliptic operators on closed manifolds (in Russian). Itogi Nauki i Tehniki, Ser. Sovrem. Probl. Mat. Fund. Napravl. 63 (1990), 5–129. (English translation in Encyclopaedia Math. Sci. 63 (1994), 1–130.) [6] B.A. Amosov, On the theory of pseudodifferential operators on the circle. (Russian) Uspekhi Mat. Nauk 43 (1988), 169–170; translation in Russian Math. Surveys 43 (1988), 197–198. [7] B.A. Amosov, Approximate solution of elliptic pseudodifferential equations on a smooth closed curve. (Russian) Z. Anal. Anwendungen 9 (1990), 545– 563. [8] P. Antosik, J. Mikusi´nski and R. Sikorski, Theory of distributions. The se- quential approach. Warszawa. PWN – Polish Scientific Publishers, 1973. [9] A. Baker, Matrix Groups. An Introduction to Lie Group Theory. Springer- Verlag, 2002. [10] J. Barros-Neto, An introduction to the theory of distributions . Marcel Dekker, Inc., 1973. [11] R. Beals, Advanced mathematical analysis. Springer-Verlag, 1973. [12] R. Beals, Characterization of pseudodifferential operators and applications. Duke Mathematical Journal. 44 (1977), 45–57. -
Lecture 7: the Complex Fourier Transform and the Discrete Fourier Transform (DFT)
Lecture 7: The Complex Fourier Transform and the Discrete Fourier Transform (DFT) c Christopher S. Bretherton Winter 2014 7.1 Fourier analysis and filtering Many data analysis problems involve characterizing data sampled on a regular grid of points, e. g. a time series sampled at some rate, a 2D image made of regularly spaced pixels, or a 3D velocity field from a numerical simulation of fluid turbulence on a regular grid. Often, such problems involve characterizing, detecting, separating or ma- nipulating variability on different scales, e. g. finding a weak systematic signal amidst noise in a time series, edge sharpening in an image, or quantifying the energy of motion across the different sizes of turbulent eddies. Fourier analysis using the Discrete Fourier Transform (DFT) is a fun- damental tool for such problems. It transforms the gridded data into a linear combination of oscillations of different wavelengths. This partitions it into scales which can be separately analyzed and manipulated. The computational utility of Fourier methods rests on the Fast Fourier Transform (FFT) algorithm, developed in the 1960s by Cooley and Tukey, which allows efficient calculation of discrete Fourier coefficients of a periodic function sampled on a regular grid of 2p points (or 2p3q5r with slightly reduced efficiency). 7.2 Example of the FFT Using Matlab, take the FFT of the HW1 wave height time series (length 24 × 60=25325) and plot the result (Fig. 1): load hw1 dat; zhat = fft(z); plot(abs(zhat),’x’) A few elements (the second and last, and to a lesser extent the third and the second from last) have magnitudes that stand above the noise. -
Discretization of Integro-Differential Equations
Discretization of Integro-Differential Equations Modeling Dynamic Fractional Order Viscoelasticity K. Adolfsson1, M. Enelund1,S.Larsson2,andM.Racheva3 1 Dept. of Appl. Mech., Chalmers Univ. of Technology, SE–412 96 G¨oteborg, Sweden 2 Dept. of Mathematics, Chalmers Univ. of Technology, SE–412 96 G¨oteborg, Sweden 3 Dept. of Mathematics, Technical University of Gabrovo, 5300 Gabrovo, Bulgaria Abstract. We study a dynamic model for viscoelastic materials based on a constitutive equation of fractional order. This results in an integro- differential equation with a weakly singular convolution kernel. We dis- cretize in the spatial variable by a standard Galerkin finite element method. We prove stability and regularity estimates which show how the convolution term introduces dissipation into the equation of motion. These are then used to prove a priori error estimates. A numerical ex- periment is included. 1 Introduction Fractional order operators (integrals and derivatives) have proved to be very suit- able for modeling memory effects of various materials and systems of technical interest. In particular, they are very useful when modeling viscoelastic materials, see, e.g., [3]. Numerical methods for quasistatic viscoelasticity problems have been studied, e.g., in [2] and [8]. The drawback of the fractional order viscoelastic models is that the whole strain history must be saved and included in each time step. The most commonly used algorithms for this integration are based on the Lubich convolution quadrature [5] for fractional order operators. In [1, 2], we develop an efficient numerical algorithm based on sparse numerical quadrature earlier studied in [6]. While our earlier work focused on discretization in time for the quasistatic case, we now study space discretization for the fully dynamic equations of mo- tion, which take the form of an integro-differential equation with a weakly singu- lar convolution kernel. -
University of Alberta
University of Alberta Extensions of Skorohod’s almost sure representation theorem by Nancy Hernandez Ceron A thesis submitted to the Faculty of Graduate Studies and Research in partial fulfillment of the requirements for the degree of Master of Science in Mathematics Department of Mathematical and Statistical Sciences ©Nancy Hernandez Ceron Fall 2010 Edmonton, Alberta Permission is hereby granted to the University of Alberta Libraries to reproduce single copies of this thesis and to lend or sell such copies for private, scholarly or scientific research purposes only. Where the thesis is converted to, or otherwise made available in digital form, the University of Alberta will advise potential users of the thesis of these terms. The author reserves all other publication and other rights in association with the copyright in the thesis and, except as herein before provided, neither the thesis nor any substantial portion thereof may be printed or otherwise reproduced in any material form whatsoever without the author's prior written permission. Library and Archives Bibliothèque et Canada Archives Canada Published Heritage Direction du Branch Patrimoine de l’édition 395 Wellington Street 395, rue Wellington Ottawa ON K1A 0N4 Ottawa ON K1A 0N4 Canada Canada Your file Votre référence ISBN:978-0-494-62500-2 Our file Notre référence ISBN: 978-0-494-62500-2 NOTICE: AVIS: The author has granted a non- L’auteur a accordé une licence non exclusive exclusive license allowing Library and permettant à la Bibliothèque et Archives Archives Canada to reproduce, Canada de reproduire, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par télécommunication ou par l’Internet, prêter, telecommunication or on the Internet, distribuer et vendre des thèses partout dans le loan, distribute and sell theses monde, à des fins commerciales ou autres, sur worldwide, for commercial or non- support microforme, papier, électronique et/ou commercial purposes, in microform, autres formats.