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Arxiv:1911.03589V1 [Math.CV] 9 Nov 2019 1 Hoe 1 Result
A NOTE ON THE SCHWARZ LEMMA FOR HARMONIC FUNCTIONS MAREK SVETLIK Abstract. In this note we consider some generalizations of the Schwarz lemma for harmonic functions on the unit disk, whereby values of such functions and the norms of their differentials at the point z = 0 are given. 1. Introduction 1.1. A summary of some results. In this paper we consider some generalizations of the Schwarz lemma for harmonic functions from the unit disk U = {z ∈ C : |z| < 1} to the interval (−1, 1) (or to itself). First, we cite a theorem which is known as the Schwarz lemma for harmonic functions and is considered as a classical result. Theorem 1 ([10],[9, p.77]). Let f : U → U be a harmonic function such that f(0) = 0. Then 4 |f(z)| 6 arctan |z|, for all z ∈ U, π and this inequality is sharp for each point z ∈ U. In 1977, H. W. Hethcote [11] improved this result by removing the assumption f(0) = 0 and proved the following theorem. Theorem 2 ([11, Theorem 1] and [26, Theorem 3.6.1]). Let f : U → U be a harmonic function. Then 1 − |z|2 4 f(z) − f(0) 6 arctan |z|, for all z ∈ U. 1+ |z|2 π As it was written in [23], it seems that researchers have had some difficulties to arXiv:1911.03589v1 [math.CV] 9 Nov 2019 handle the case f(0) 6= 0, where f is harmonic mapping from U to itself. Before explaining the essence of these difficulties, it is necessary to recall one mapping and some of its properties. -
The Riemann Mapping Theorem Christopher J. Bishop
The Riemann Mapping Theorem Christopher J. Bishop C.J. Bishop, Mathematics Department, SUNY at Stony Brook, Stony Brook, NY 11794-3651 E-mail address: [email protected] 1991 Mathematics Subject Classification. Primary: 30C35, Secondary: 30C85, 30C62 Key words and phrases. numerical conformal mappings, Schwarz-Christoffel formula, hyperbolic 3-manifolds, Sullivan’s theorem, convex hulls, quasiconformal mappings, quasisymmetric mappings, medial axis, CRDT algorithm The author is partially supported by NSF Grant DMS 04-05578. Abstract. These are informal notes based on lectures I am giving in MAT 626 (Topics in Complex Analysis: the Riemann mapping theorem) during Fall 2008 at Stony Brook. We will start with brief introduction to conformal mapping focusing on the Schwarz-Christoffel formula and how to compute the unknown parameters. In later chapters we will fill in some of the details of results and proofs in geometric function theory and survey various numerical methods for computing conformal maps, including a method of my own using ideas from hyperbolic and computational geometry. Contents Chapter 1. Introduction to conformal mapping 1 1. Conformal and holomorphic maps 1 2. M¨obius transformations 16 3. The Schwarz-Christoffel Formula 20 4. Crowding 27 5. Power series of Schwarz-Christoffel maps 29 6. Harmonic measure and Brownian motion 39 7. The quasiconformal distance between polygons 48 8. Schwarz-Christoffel iterations and Davis’s method 56 Chapter 2. The Riemann mapping theorem 67 1. The hyperbolic metric 67 2. Schwarz’s lemma 69 3. The Poisson integral formula 71 4. A proof of Riemann’s theorem 73 5. Koebe’s method 74 6. -
The Chazy XII Equation and Schwarz Triangle Functions
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 13 (2017), 095, 24 pages The Chazy XII Equation and Schwarz Triangle Functions Oksana BIHUN and Sarbarish CHAKRAVARTY Department of Mathematics, University of Colorado, Colorado Springs, CO 80918, USA E-mail: [email protected], [email protected] Received June 21, 2017, in final form December 12, 2017; Published online December 25, 2017 https://doi.org/10.3842/SIGMA.2017.095 Abstract. Dubrovin [Lecture Notes in Math., Vol. 1620, Springer, Berlin, 1996, 120{348] showed that the Chazy XII equation y000 − 2yy00 + 3y02 = K(6y0 − y2)2, K 2 C, is equivalent to a projective-invariant equation for an affine connection on a one-dimensional complex manifold with projective structure. By exploiting this geometric connection it is shown that the Chazy XII solution, for certain values of K, can be expressed as y = a1w1 +a2w2 +a3w3 where wi solve the generalized Darboux{Halphen system. This relationship holds only for certain values of the coefficients (a1; a2; a3) and the Darboux{Halphen parameters (α; β; γ), which are enumerated in Table2. Consequently, the Chazy XII solution y(z) is parametrized by a particular class of Schwarz triangle functions S(α; β; γ; z) which are used to represent the solutions wi of the Darboux{Halphen system. The paper only considers the case where α + β +γ < 1. The associated triangle functions are related among themselves via rational maps that are derived from the classical algebraic transformations of hypergeometric functions. The Chazy XII equation is also shown to be equivalent to a Ramanujan-type differential system for a triple (P;^ Q;^ R^). -
THE IMPACT of RIEMANN's MAPPING THEOREM in the World
THE IMPACT OF RIEMANN'S MAPPING THEOREM GRANT OWEN In the world of mathematics, scholars and academics have long sought to understand the work of Bernhard Riemann. Born in a humble Ger- man home, Riemann became one of the great mathematical minds of the 19th century. Evidence of his genius is reflected in the greater mathematical community by their naming 72 different mathematical terms after him. His contributions range from mathematical topics such as trigonometric series, birational geometry of algebraic curves, and differential equations to fields in physics and philosophy [3]. One of his contributions to mathematics, the Riemann Mapping Theorem, is among his most famous and widely studied theorems. This theorem played a role in the advancement of several other topics, including Rie- mann surfaces, topology, and geometry. As a result of its widespread application, it is worth studying not only the theorem itself, but how Riemann derived it and its impact on the work of mathematicians since its publication in 1851 [3]. Before we begin to discover how he derived his famous mapping the- orem, it is important to understand how Riemann's upbringing and education prepared him to make such a contribution in the world of mathematics. Prior to enrolling in university, Riemann was educated at home by his father and a tutor before enrolling in high school. While in school, Riemann did well in all subjects, which strengthened his knowl- edge of philosophy later in life, but was exceptional in mathematics. He enrolled at the University of G¨ottingen,where he learned from some of the best mathematicians in the world at that time. -
Algebraicity Criteria and Their Applications
Algebraicity Criteria and Their Applications The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters Citation Tang, Yunqing. 2016. Algebraicity Criteria and Their Applications. Doctoral dissertation, Harvard University, Graduate School of Arts & Sciences. Citable link http://nrs.harvard.edu/urn-3:HUL.InstRepos:33493480 Terms of Use This article was downloaded from Harvard University’s DASH repository, and is made available under the terms and conditions applicable to Other Posted Material, as set forth at http:// nrs.harvard.edu/urn-3:HUL.InstRepos:dash.current.terms-of- use#LAA Algebraicity criteria and their applications A dissertation presented by Yunqing Tang to The Department of Mathematics in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the subject of Mathematics Harvard University Cambridge, Massachusetts May 2016 c 2016 – Yunqing Tang All rights reserved. DissertationAdvisor:ProfessorMarkKisin YunqingTang Algebraicity criteria and their applications Abstract We use generalizations of the Borel–Dwork criterion to prove variants of the Grothedieck–Katz p-curvature conjecture and the conjecture of Ogus for some classes of abelian varieties over number fields. The Grothendieck–Katz p-curvature conjecture predicts that an arithmetic differential equation whose reduction modulo p has vanishing p-curvatures for all but finitely many primes p,hasfinite monodromy. It is known that it suffices to prove the conjecture for differential equations on P1 − 0, 1, . We prove a variant of this conjecture for P1 0, 1, , which asserts that if the equation { ∞} −{ ∞} satisfies a certain convergence condition for all p, then its monodromy is trivial. -
The Measurable Riemann Mapping Theorem
CHAPTER 1 The Measurable Riemann Mapping Theorem 1.1. Conformal structures on Riemann surfaces Throughout, “smooth” will always mean C 1. All surfaces are assumed to be smooth, oriented and without boundary. All diffeomorphisms are assumed to be smooth and orientation-preserving. It will be convenient for our purposes to do local computations involving metrics in the complex-variable notation. Let X be a Riemann surface and z x iy be a holomorphic local coordinate on X. The pair .x; y/ can be thoughtD C of as local coordinates for the underlying smooth surface. In these coordinates, a smooth Riemannian metric has the local form E dx2 2F dx dy G dy2; C C where E; F; G are smooth functions of .x; y/ satisfying E > 0, G > 0 and EG F 2 > 0. The associated inner product on each tangent space is given by @ @ @ @ a b ; c d Eac F .ad bc/ Gbd @x C @y @x C @y D C C C Äc a b ; D d where the symmetric positive definite matrix ÄEF (1.1) D FG represents in the basis @ ; @ . In particular, the length of a tangent vector is f @x @y g given by @ @ p a b Ea2 2F ab Gb2: @x C @y D C C Define two local sections of the complexified cotangent bundle T X C by ˝ dz dx i dy WD C dz dx i dy: N WD 2 1 The Measurable Riemann Mapping Theorem These form a basis for each complexified cotangent space. The local sections @ 1 Â @ @ Ã i @z WD 2 @x @y @ 1 Â @ @ Ã i @z WD 2 @x C @y N of the complexified tangent bundle TX C will form the dual basis at each point. -
The Riemann Mapping Theorem
University of Toronto – MAT334H1-F – LEC0101 Complex Variables 18 – The Riemann mapping theorem Jean-Baptiste Campesato December 2nd, 2020 and December 4th, 2020 Theorem 1 (The Riemann mapping theorem). Let 푈 ⊊ ℂ be a simply connected open subset which is not ℂ. −1 Then there exists a biholomorphism 푓 ∶ 푈 → 퐷1(0) (i.e. 푓 is holomorphic, bijective and 푓 is holomorphic). We say that 푈 and 퐷1(0) are conformally equivalent. Remark 2. Note that if 푓 ∶ 푈 → 푉 is bijective and holomorphic then 푓 −1 is holomorphic too. Indeed, we proved that if 푓 is injective and holomorphic then 푓 ′ never vanishes (Nov 30). Then we can conclude using the inverse function theorem. Note that this remark is false for ℝ-differentiability: define 푓 ∶ ℝ → ℝ by 푓(푥) = 푥3 then 푓 ′(0) = 0 and 푓 −1(푥) = √3 푥 is not differentiable at 0. Remark 3. The theorem is false if 푈 = ℂ. Indeed, by Liouville’s theorem, if 푓 ∶ ℂ → 퐷1(0) is holomorphic then it is constant (as a bounded entire function), so it can’t be bijective. The Riemann mapping theorem states that up to biholomorphic transformations, the unit disk is a model for open simply connected sets which are not ℂ. Otherwise stated, up to a biholomorphic transformation, there are only two open simply connected sets: 퐷1(0) and ℂ. Formally: Corollary 4. Let 푈, 푉 ⊊ ℂ be two simply connected open subsets, none of which is ℂ. Then there exists a biholomorphism 푓 ∶ 푈 → 푉 (i.e. 푓 is holomorphic, bijective and 푓 −1 is holomorphic). -
Math 311: Complex Analysis — Automorphism Groups Lecture
MATH 311: COMPLEX ANALYSIS | AUTOMORPHISM GROUPS LECTURE 1. Introduction Rather than study individual examples of conformal mappings one at a time, we now want to study families of conformal mappings. Ensembles of conformal mappings naturally carry group structures. 2. Automorphisms of the Plane The automorphism group of the complex plane is Aut(C) = fanalytic bijections f : C −! Cg: Any automorphism of the plane must be conformal, for if f 0(z) = 0 for some z then f takes the value f(z) with multiplicity n > 1, and so by the Local Mapping Theorem it is n-to-1 near z, impossible since f is an automorphism. By a problem on the midterm, we know the form of such automorphisms: they are f(z) = az + b; a; b 2 C; a 6= 0: This description of such functions one at a time loses track of the group structure. If f(z) = az + b and g(z) = a0z + b0 then (f ◦ g)(z) = aa0z + (ab0 + b); f −1(z) = a−1z − a−1b: But these formulas are not very illuminating. For a better picture of the automor- phism group, represent each automorphism by a 2-by-2 complex matrix, a b (1) f(z) = ax + b ! : 0 1 Then the matrix calculations a b a0 b0 aa0 ab0 + b = ; 0 1 0 1 0 1 −1 a b a−1 −a−1b = 0 1 0 1 naturally encode the formulas for composing and inverting automorphisms of the plane. With this in mind, define the parabolic group of 2-by-2 complex matrices, a b P = : a; b 2 ; a 6= 0 : 0 1 C Then the correspondence (1) is a natural group isomorphism, Aut(C) =∼ P: 1 2 MATH 311: COMPLEX ANALYSIS | AUTOMORPHISM GROUPS LECTURE Two subgroups of the parabolic subgroup are its Levi component a 0 M = : a 2 ; a 6= 0 ; 0 1 C describing the dilations f(z) = ax, and its unipotent radical 1 b N = : b 2 ; 0 1 C describing the translations f(z) = z + b. -
Applications of the Cauchy Theory
Chapter 4 Applications Of The Cauchy Theory This chapter contains several applications of the material developed in Chapter 3. In the first section, we will describe the possible behavior of an analytic function near a singularity of that function. 4.1 Singularities We will say that f has an isolated singularity at z0 if f is analytic on D(z0,r) \{z0} for some r. What, if anything, can be said about the behavior of f near z0? The basic tool needed to answer this question is the Laurent series, an expansion of f(z)in powers of z − z0 in which negative as well as positive powers of z − z0 may appear. In fact, the number of negative powers in this expansion is the key to determining how f behaves near z0. From now on, the punctured disk D(z0,r) \{z0} will be denoted by D (z0,r). We will need a consequence of Cauchy’s integral formula. 4.1.1 Theorem Let f be analytic on an open set Ω containing the annulus {z : r1 ≤|z − z0|≤r2}, 0 <r1 <r2 < ∞, and let γ1 and γ2 denote the positively oriented inner and outer boundaries of the annulus. Then for r1 < |z − z0| <r2, we have 1 f(w) − 1 f(w) f(z)= − dw − dw. 2πi γ2 w z 2πi γ1 w z Proof. Apply Cauchy’s integral formula [part (ii)of (3.3.1)]to the cycle γ2 − γ1. ♣ 1 2 CHAPTER 4. APPLICATIONS OF THE CAUCHY THEORY 4.1.2 Definition For 0 ≤ s1 <s2 ≤ +∞ and z0 ∈ C, we will denote the open annulus {z : s1 < |z−z0| <s2} by A(z0,s1,s2). -
Lectures on Non-Archimedean Function Theory Advanced
Lectures on Non-Archimedean Function Theory Advanced School on p-Adic Analysis and Applications The Abdus Salam International Centre for Theoretical Physics Trieste, Italy William Cherry Department of Mathematics University of North Texas August 31 – September 4, 2009 Lecture 1: Analogs of Basic Complex Function Theory Lecture 2: Valuation Polygons and a Poisson-Jensen Formula Lecture 3: Non-Archimedean Value Distribution Theory Lecture 4: Benedetto’s Non-Archimedean Island Theorems arXiv:0909.4509v1 [math.CV] 24 Sep 2009 Non-Archimedean Function Theory: Analogs of Basic Complex Function Theory 3 This lecture series is an introduction to non-Archimedean function theory. The audience is assumed to be familiar with non-Archimedean fields and non-Archimedean absolute values, as well as to have had a standard introductory course in complex function theory. A standard reference for the later could be, for example, [Ah 2]. No prior exposure to non-Archimedean function theory is supposed. Full details on the basics of non-Archimedean absolute values and the construction of p-adic number fields, the most important of the non-Archimedean fields, can be found in [Rob]. 1 Analogs of Basic Complex Function Theory 1.1 Non-Archimedean Fields Let A be a commutative ring. A non-Archimedean absolute value | | on A is a function from A to the non-negative real numbers R≥0 satisfying the following three properties: AV 1. |a| = 0 if and only if a = 0; AV 2. |ab| = |a| · |b| for all a, b ∈ A; and AV 3. |a + b|≤ max{|a|, |b|} for all a, b ∈ A. Exercise 1.1.1. -
Conjugacy Classification of Quaternionic M¨Obius Transformations
CONJUGACY CLASSIFICATION OF QUATERNIONIC MOBIUS¨ TRANSFORMATIONS JOHN R. PARKER AND IAN SHORT Abstract. It is well known that the dynamics and conjugacy class of a complex M¨obius transformation can be determined from a simple rational function of the coef- ficients of the transformation. We study the group of quaternionic M¨obius transforma- tions and identify simple rational functions of the coefficients of the transformations that determine dynamics and conjugacy. 1. Introduction The motivation behind this paper is the classical theory of complex M¨obius trans- formations. A complex M¨obiustransformation f is a conformal map of the extended complex plane of the form f(z) = (az + b)(cz + d)−1, where a, b, c and d are complex numbers such that the quantity σ = ad − bc is not zero (we sometimes write σ = σf in order to avoid ambiguity). There is a homomorphism from SL(2, C) to the group a b of complex M¨obiustransformations which takes the matrix ( c d ) to the map f. This homomorphism is surjective because the coefficients of f can always be scaled so that σ = 1. The collection of all complex M¨obius transformations for which σ takes the value 1 forms a group which can be identified with PSL(2, C). A member f of PSL(2, C) is simple if it is conjugate in PSL(2, C) to an element of PSL(2, R). The map f is k–simple if it may be expressed as the composite of k simple transformations but no fewer. Let τ = a + d (and likewise we write τ = τf where necessary). -
Conformal Mapping Solution of Laplace's Equation on a Polygon
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Journal of Computational and Applied Mathematics 14 (1986) 227-249 227 North-Holland Conformal mapping solution of Laplace’s equation on a polygon with oblique derivative boundary conditions Lloyd N. TREFETHEN * Department of Mathematics, Massachusetts Institute of Technology, Cambridge, MA 02139, U.S.A. Ruth J. WILLIAMS ** Department of Mathematics, University of California at San Diego, La Jolla, CA 92093, U.S.A. Received 6 July 1984 Abstract: We consider Laplace’s equation in a polygonal domain together with the boundary conditions that along each side, the derivative in the direction at a specified oblique angle from the normal should be zero. First we prove that solutions to this problem can always be constructed by taking the real part of an analytic function that maps the domain onto another region with straight sides oriented according to the angles given in the boundary conditions. Then we show that this procedure can be carried out successfully in practice by the numerical calculation of Schwarz-Christoffel transformations. The method is illustrated by application to a Hall effect problem in electronics, and to a reflected Brownian motion problem motivated by queueing theory. Keywor& Laplace equation, conformal mapping, Schwarz-Christoffel map, oblique derivative, Hall effect, Brownian motion, queueing theory. Mathematics Subject CIassi/ication: 3OC30, 35525, 60K25, 65EO5, 65N99. 1. The oblique derivative problem and conformal mapping Let 52 by a polygonal domain in the complex plane C, by which we mean a possibly unbounded simply connected open subset of C whose boundary aa consists of a finite number of straight lines, rays, and line segments.