Quasiconformal Mappings, from Ptolemy's Geography to the Work Of
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4.Murtomäki 2017.10192 Words
Sibelius in the Context of the Finnish-German History Veijo Murtomäki Introduction The life and career of a composer cannot be considered as an isolated case without taking into account the wider context. The history of ideas and ideologies is always part of any serious enquiry into an artist’s personal history. Therefore we must bear in mind at least four points when considering the actions of artist and his or her country. Firstly, as the eminent Finnish historian Matti Klinge has observed, "the biggest challenge for understanding history is trying to situate oneself in the preconditions of the time-period under scrutiny while remembering that it did not know what the posterity knows."[1] Writing history is not primarily a task whereby the historian provides lines for actors to speak, but rather is an attempt to understand and explain why something happened, and to construct a context including all of the possible factors involved in a certain historical process. Secondly, supporting (or not opposing) an ideology prevailing at a certain time does not mean that the supporter (or non-opponent) is committing a crime. We could easily condemn half of the European intellectuals for supporting Fascism, Nazism, Communism or Maoism, or just for having become too easily attracted by these – in their mind – fascinating, visionary ideologies to shape European or world history. Thirdly, history has always been written by the winners – and thus, historiography tends to be distorted by exaggerating the evil of the enemy and the goodness of the victor. A moral verdict must be reached when we are dealing with absolute evil, but it is rare to find exclusively good or bad persons or civilizations; therefore history is rarely an issue of black and white. -
Elliptic Systems on Riemann Surfaces
Lecture Notes of TICMI, Vol.13, 2012 Giorgi Akhalaia, Grigory Giorgadze, Valerian Jikia, Neron Kaldani, Giorgi Makatsaria, Nino Manjavidze ELLIPTIC SYSTEMS ON RIEMANN SURFACES © Tbilisi University Press Tbilisi Abstract. Systematic investigation of Elliptic systems on Riemann surface and new results from the theory of generalized analytic functions and vectors are pre- sented. Complete analysis of the boundary value problem of linear conjugation and Riemann-Hilbert monodromy problem for the Carleman-Bers-Vekua irregular systems are given. 2000 Mathematics Subject Classi¯cation: 57R45 Key words and phrases: Generalized analytic function, Generalized analytic vector, irregular Carleman-Bers-Vekua equation, linear conjugation problem, holo- morphic structure, Beltrami equation Giorgi Akhalaia, Grigory Giorgadze*, Valerian Jikia, Neron Kaldani I.Vekua Institute of Applied Mathematics of I. Javakhishvili Tbilisi State University 2 University st., Tbilisi 0186, Georgia Giorgi Makatsaria St. Andrews Georgian University 53a Chavchavadze Ave., Tbilisi 0162, Georgia Nino Manjavidze Georgian Technical University 77 M. Kostava st., Tbilisi 0175, Georgia * Corresponding Author. email: [email protected] Contents Preface 5 1 Introduction 7 2 Functional spaces induced from regular Carleman-Bers-Vekua equations 15 2.1 Some functional spaces . 15 2.2 The Vekua-Pompej type integral operators . 16 2.3 The Carleman-Bers-Vekua equation . 18 2.4 The generalized polynomials of the class Ap;2(A; B; C), p > 2 . 20 2.5 Some properties of the generalized power functions . 22 2.6 The problem of linear conjugation for generalized analytic functions . 26 3 Beltrami equation 28 4 The pseudoanalytic functions 36 4.1 Relation between Beltrami and holomorphic disc equations . 38 4.2 The periodicity of the space of generalized analytic functions . -
The Origins of the Propagation of Smallness Property and Its Utility in Controllability Problems
The Origins of the Propagation of Smallness Property and its Utility in Controllability Problems. Jone Apraiz University of the Basque Country, Spain Seminario control en tiempos de crisis May 4th 2020 Jone Apraiz (UPV/EHU) Control en tiempos de crisis 04/05/2020 1 / 37 Index 1 Definition of the propagation of smallness property 2 Origin of the propagation of smallness property Harmonic measure Two-constants and Hamard three-circles theorems Phragmén-Lindelöf theorem and Hadamard three-lines lemma 3 Applications to Control Theory Higher dimensions: three-balls and three-regions theorems Null-control for some parabolic problems Jone Apraiz (UPV/EHU) Control en tiempos de crisis 04/05/2020 2 / 37 Definition of the propagation of smallness property Index 1 Definition of the propagation of smallness property 2 Origin of the propagation of smallness property Harmonic measure Two-constants and Hamard three-circles theorems Phragmén-Lindelöf theorem and Hadamard three-lines lemma 3 Applications to Control Theory Higher dimensions: three-balls and three-regions theorems Null-control for some parabolic problems Jone Apraiz (UPV/EHU) Control en tiempos de crisis 04/05/2020 3 / 37 Definition of the propagation of smallness property Definition of the propagation of smallness property Definition (Propagation of smallness) n Given three subsets of R , E, B1 and B2, verifying E ⊂ B1 ⊂ B2 and a class of functions A ⊂ C(B2), we say that E is a propagation of smallness set for A if, for any u 2 A, there exists α = α(E; B1; B2) 2 (0; 1) such that jjujj ≤ jjujjα jjujj1−α : 1;B1 1;E 1;B2 The “information of the function” on the smaller domain is propagating or affecting over bigger domains in some sense. -
Of Triangles, Gas, Price, and Men
OF TRIANGLES, GAS, PRICE, AND MEN Cédric Villani Univ. de Lyon & Institut Henri Poincaré « Mathematics in a complex world » Milano, March 1, 2013 Riemann Hypothesis (deepest scientific mystery of our times?) Bernhard Riemann 1826-1866 Riemann Hypothesis (deepest scientific mystery of our times?) Bernhard Riemann 1826-1866 Riemannian (= non-Euclidean) geometry At each location, the units of length and angles may change Shortest path (= geodesics) are curved!! Geodesics can tend to get closer (positive curvature, fat triangles) or to get further apart (negative curvature, skinny triangles) Hyperbolic surfaces Bernhard Riemann 1826-1866 List of topics named after Bernhard Riemann From Wikipedia, the free encyclopedia Riemann singularity theorem Cauchy–Riemann equations Riemann solver Compact Riemann surface Riemann sphere Free Riemann gas Riemann–Stieltjes integral Generalized Riemann hypothesis Riemann sum Generalized Riemann integral Riemann surface Grand Riemann hypothesis Riemann theta function Riemann bilinear relations Riemann–von Mangoldt formula Riemann–Cartan geometry Riemann Xi function Riemann conditions Riemann zeta function Riemann curvature tensor Zariski–Riemann space Riemann form Riemannian bundle metric Riemann function Riemannian circle Riemann–Hilbert correspondence Riemannian cobordism Riemann–Hilbert problem Riemannian connection Riemann–Hurwitz formula Riemannian cubic polynomials Riemann hypothesis Riemannian foliation Riemann hypothesis for finite fields Riemannian geometry Riemann integral Riemannian graph Bernhard -
Chapter 6 Riemann Solvers I
Chapter 6 Riemann solvers I The numerical hydrodynamics algorithms we have devised in Chapter 5 were based on the idea of operator splitting between the advection and pressure force terms. The advection was done, for all conserved quantities, using the gas velocity, while the pressure force and work terms were treated as source terms. From Chapter 2 we know, however, thatthecharacteristicsoftheEuler equations are not necessarily all equal to the gas velocity. We have seen that there exist an eigen- vector which indeed has the gas velocity as eigenvectors, λ0 = u,buttherearetwoeigenvectors which have eigenvalues λ = u C which belong to the forward and backward sound propa- ± ± s gation. Mathematically speaking one should do the advectioninthesethreeeigenvectors,using their eigenvalues as advection velocity. The methods in Chapter 5 do not do this. By extracting the pressure terms out of the advection part and adding them asasourceterm,theadvectionpart has been reduced essentially to Burger’s equation,andthepropagationofsoundwavesisentirely driven by the addition of the source terms. Such methods therefore do not formally propagate the sound waves using advection, even though mathematically they should be. All the effort we have done in Chapters 3 and 4 to create the best advection schemes possible will therefore have no effect on the propagation of sound waves. Once could say that for two out of three characteristics our ingeneous advection scheme is useless. Riemann solvers on the other hand keep the pressure terms within the to-be-advected sys- tem. There is no pressure source term in these equations. The mathematical character of the equations remains intact. Such solvers therefore propagateallthecharacteristicsonequalfoot- ing. -
Riemann, Schottky, and Schwarz on Conformal Representation
Appendix 1 Riemann, Schottky, and Schwarz on Conformal Representation In his Thesis [1851], Riemann sought to prove that if a function u satisfies cer- tain conditions on the boundary of a surface T, then it is the real part of a unique complex function which can be defined on the whole of T. He was then able to show that any two simply connected surfaces (other than the complex plane itself Riemann was considering bounded surfaces) can be mapped conformally onto one another, and that the map is unique once the images of one boundary point and one interior point are specified; he claimed analogous results for any two surfaces of the same connectivity [w To prove that any two simply connected surfaces are conformally equivalent, he observed that it is enough to take for one surface the unit disc K = {z : Izl _< l} and he gave [w an account of how this result could be proved by means of what he later [1857c, 103] called Dirichlet's principle. He considered [w (i) the class of functions, ~., defined on a surface T and vanishing on the bound- ary of T, which are continuous, except at some isolated points of T, for which the integral t= rx + ry dt is finite; and (ii) functions ct + ~. = o9, say, satisfying dt=f2 < oo Ox Oy + for fixed but arbitrary continuous functions a and ft. 224 Appendix 1. Riemann, Schottky, and Schwarz on Conformal Representation He claimed that f2 and L vary continuously with varying ,~. but cannot be zero, and so f2 takes a minimum value for some o9. -
Solving Beltrami Equations by Circle Packing
transactions of the american mathematical society Volume 322, Number 2, December 1990 SOLVING BELTRAMI EQUATIONS BY CIRCLE PACKING ZHENG-XU HE Abstract. We use Andreev-Thurston's theorem on the existence of circle pack- ings to construct approximating solutions to the Beltrami equations on Riemann surfaces. The convergence of the approximating solutions on compact subsets will be shown. This gives a constructive proof of the existence theorem for Beltrami equations. 1. Introduction A circle packing in the plane or in a closed Riemannian 2-manifold of con- stant curvature is a collection of closed round disks with disjoint interiors. The nerve of such circle packing is the embedded graph whose vertices are the centers of the disks and whose edges are the shortest geodesic arcs joining the centers of each pair of intersecting disks. By Andreev-Thurston's theorem, for any tri- 2 2 angulation of the Riemann sphere S , there is a circle packing on S , unique up to a Möbius transformation, whose nerve is isotopic to the 1-skeleton of the triangulation (see [T, Corollary 13.6.2, or MR]). Based on this fact, William P. Thurston suggested a geometric approach to the Riemann mapping theorem. Recently, Burt Rodin and Dennis Sullivan [RS] carried out this ap- proach and verified the convergence of Thurston's scheme. In this paper, we will use this circle packing method to construct approximations to solutions /:fi-»C of the Beltrami equation: (1.1) d,fi(z) = k(z)dzfi(z) a.e. z = x + iyeSi, where Q. is some open Jordan domain in C, and k: Q —>C is some measurable function with (1.2) ||A||00= esssup|A(z)|<l. -
Georg Friedrich Bernhard Riemann
Georg Friedrich Bernhard Riemann By: Supervised: Sandra Hanbo Dr. Vágó Zsuzsanna Biography • Born in 17 September 1826 in Breselenz, Kingdom of Hannover (Germany now) • Father : Friedrich Bernhard Riemann. Poor Lutheran pastor • Mother: Charlotte Ebell • Wife: Elise Koch and they had a daughter Elda • Universities : University of Göttingen (1846) studying math under Gauss, University of Berlin (1847) continuing study by : Carl Gustav Jacob Jacobi, Peter Gustav Lejeune Dirichlet, Jakob Steiner, and Gotthold Eisenstein • Doctoral supervisor : Carl Friedrich Gauss • Honors awarded to Bernhard Riemann 1. Fellow of the Royal Society: 1866 2. Lunar features: Crater Riemann 3. Popular biographies list: Number 18 • Dead : 20 July 1866 in Selasca (Italy) Some of his Articles • Basics for a general theory of functions of a changeable complex Size.- 1851 • On the Number of Primes Less Than a Given –1859 • On the laws of the distribution of voltage electricity in ponderable bodies, if these are not regarded as perfect conductors or non-conductors, but as reluctant to contain voltage electricity with finite force- - 1854 • On the theory of Nobili's color rings -1855 • Contributions to the theory of the functions that can be represented by the Gaussian series F (α, β, γ,( .- 1857 • Theory of Abel's functions -1857 • About the disappearance of the theta functions - 1866 Some topics named after Riemann • Cauchy–Riemann equations • Riemann form • Riemann Geometry • Riemann mapping theorem • Riemann problem • Riemann surface • Riemann solver • Riemann's differential equation • Riemann's explicit formula Riemann surface for f(z) = z1/2. Image by Leonid 2. • Riemann's minimal surface Famous Scientists – Bernard Riemann And others … References: • Articles: • "Bernhard Riemann." Famous Scientists. -
Nevanlinna Theory on Meromorphic Functions and Their Value Distribution Theory
Nevanlinna Theory On Meromorphic Functions and Their Value Distribution Theory Niko Laaksonen [email protected] October 26th 2010 Value distribution theory is the study of how often a complex function assumes different values. By the Fundamental Theorem of Algebra we know that any polynomial over C is completely determined by its zeros up to a constant multiple. But what can we say about general entire functions? How many zeros must, or can, these functions have? How many times can two meromorphic functions assume the same value on the same set? How does Nevanlinna fit into all this? If you wish to hear the answers to these questions come and join us on the 26th of October. “Rolf Nevanlinna, creator of the modern theory of meromorphic functions” -Hayman, W.K. 1 With this talk I’m hoping to introduce some concepts that were just out of reach in the first complex analysis course at UCL. Eventually my goal is to naturally end up at a point where, in order to make further progress, it is essential to introduce the theory of Nevanlinna. No previous knowledge is assumed from the audience, but some familiarity with basic complex analysis can be helpful. 1 Polynomials Value distribution theory tries to answer the question of how many times does a certain function take different complex values, and what is the distribution — or density — of these points. We begin by looking at the simple case of a polynomial f : C → C of degree n. This well serve to introduce the ideas of the theory and to suggest parallels to a wider class of functions. -
Curriculum Vitae and Publications
Lasse Holmstr¨om November 20, 2020 CURRICULUM VITAE AND PUBLICATIONS Name and current address Lasse Holmstr¨om University of Oulu Research Unit of Mathematical Sciences P.O.Box 3000 90014 University of Oulu Finland Homepage: http://cc.oulu.fi/~llh/ Date and place of birth, marital status June 27, 1951, Helsinki, Finland Married, three children Education University of Helsinki (1971-1978): B.S. (Mathematics), 1974 M.S. (Mathematics), 1975 Licentiate in Philosophy (Mathematics), 1977 Clarkson College of Technology, Potsdam, New York, USA (1978 - 1979): Ph.D. (Mathematics), 1980 Doctoral Thesis: A Study on the Structure of Nuclear K¨othe Spaces Thesis advisor: Professor Ed Dubinsky Positions held In Finland 1 University of Oulu, Department of Mathematical Sciences: Professor (2003 - 2017) Department Chair (2006 - 2013, 2015) Chair of the Research Unit of Applied Mathematics and Statistics (2016) Rolf Nevanlinna Institute (University of Helsinki): Director (1999 - 2000, 2002 - 2003) Research Division Head (1995 - 2003) Associate Professor (1994 - 1995) Senior Fellow (1992 - 1993) Acting Director (1992) Research Fellow (1988 - 1989) Academy of Finland (Research Council for Natural Sciences and Engineering): Senior Scientist (2008) Academy of Finland (Research Council for Technology): Senior Fellow (1990 - 1992) Helsinki University of Technology, Laboratory of Information Processing Sci- ence: Research Fellow (1984 - 1988) University of Helsinki, Department of Mathematics: Assistant (1977 - 1978, 1979 - 1981, 1983 - 1984) Lecturer (Fall 1980) -
The Universal Properties of Teichm¨Uller Spaces
THE UNIVERSAL PROPERTIES OF TEICHMULLERÄ SPACES VLADIMIR MARKOVIC AND DRAGOMIR SARI· C¶ Abstract. We discuss universal properties of general TeichmÄullerspaces. Our topics include the TeichmÄullermetric and the Kobayashi metric, extremality and unique extremality of quasiconformal mappings, biholomorphic maps be- tween TeichmÄullerspace, earthquakes and Thurston boundary. 1. Introduction Today, TeichmÄullertheory is a substantial area of mathematics that has inter- actions with many other subjects. The bulk of this theory is focused on studying TeichmÄullerspaces of ¯nite type Riemann surfaces. In this article we survey the theory that investigates all TeichmÄullerspaces regardless of their dimension. We aim to present theorems (old and recent) that illustrate universal properties of TeichmÄullerspaces. TeichmÄullerspaces of ¯nite type Riemann surfaces (or just ¯nite Riemann sur- faces) are ¯nite-dimensional complex manifolds with rich geometric structures. Te- ichmÄullerspaces of in¯nite type Riemann surfaces are in¯nite-dimensional Banach manifolds whose geometry di®ers signi¯cantly from the ¯nite case. However, some statements hold for both ¯nite and in¯nite cases. The intent is to describe these universal properties of all TeichmÄullerspaces and to point out to di®erences between ¯nite and in¯nite cases when these are well understood. The following is the list of topics covered. In the second section we briefly in- troduce quasiconformal maps and mention their basic properties. Then we proceed to give the analytic de¯nition of TeichmÄullerspaces, regardless whether the un- derlying Riemann surface is of ¯nite or in¯nite type. We de¯ne the TeichmÄuller metric and introduce the complex structure on TeichmÄullerspaces. Next we dis- cuss the Kobayashi metric, the tangent space and the barycentric extensions. -
On the Birti{ of the Neyanlinna Theory
Annales Academic Scientiarum Fennicre Commentationes in memoriam Series A. I. Mathematica Rolf Nevanlinna Volumert T, 1982, 5-23 ON THE BIRTI{ OF THE NEYANLINNA THEORY OLLI LEIITO Classical value distribution theory deals with the study of the density of the points in the plane at which an analytic function takes a prescribed value. Poly- nomials, for which complete results can at once be obtained, served as a model when the study of entire functions was started about a hundred years ago. By the turn of the century, Borel had succeeded in combining and improving results of picard, Poincar6 and Hadamard in such a way that a value distribution theory began to take shape. Further progress was made during the first two decades of this century by a greatly'increased number of mathematicians, albeit without any particularly striking results. The theory of meromorphic functions resisted such a development: apart from a few exceptions, it was difficult even to formulate the problems studied in connection with entire functions. In the early twenties the state of affairs underwent a discontinuous change due to Rolf Nevanlinna. He succeeded in creating a far-reaching value distribution theory for meromorphic functions, in such away that it contained as a special case the theory of entire functions in an improved form. The Nevanlinna theory came into being through the work he did in the years 1922-24. However, the impact of the new theory was so profound that the process of birth persisted for a period of about ten years. Our description of this period will be preceded by a brief summary of the ante- Nevanlinna value distribution theory.