Schwarz-Christoffel Transformations by Philip P. Bergonio (Under the Direction of Edward Azoff) Abstract the Riemann Mapping
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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^). -
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. -
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. -
Riemann's Mapping Theorem
4. Del Riemann’s mapping theorem version 0:21 | Tuesday, October 25, 2016 6:47:46 PM very preliminary version| more under way. One dares say that the Riemann mapping theorem is one of more famous theorem in the whole science of mathematics. Together with its generalization to Riemann surfaces, the so called Uniformisation Theorem, it is with out doubt the corner-stone of function theory. The theorem classifies all simply connected Riemann-surfaces uo to biholomopisms; and list is astonishingly short. There are just three: The unit disk D, the complex plane C and the Riemann sphere C^! Riemann announced the mapping theorem in his inaugural dissertation1 which he defended in G¨ottingenin . His version a was weaker than full version of today, in that he seems only to treat domains bounded by piecewise differentiable Jordan curves. His proof was not waterproof either, lacking arguments for why the Dirichlet problem has solutions. The fault was later repaired by several people, so his method is sound (of course!). In the modern version there is no further restrictions on the domain than being simply connected. William Fogg Osgood was the first to give a complete proof of the theorem in that form (in ), but improvements of the proof continued to come during the first quarter of the th century. We present Carath´eodory's version of the proof by Lip´otFej´erand Frigyes Riesz, like Reinholdt Remmert does in his book [?], and we shall closely follow the presentation there. This chapter starts with the legendary lemma of Schwarz' and a study of the biho- lomorphic automorphisms of the unit disk. -
Use of Conformal Mappings for Solution of 2D PDE Problems 1. Use
Use of conformal mappings for solution of 2D PDE problems 1. Use of conformal mappings onto a circle, for 2D Dirichlet problems. Consider a Dirichlet problem for the Laplace equation: 8 < ¢u(x; y) = 0; (x; y) 2 D; (1) : u(x; y)j@D = g(x; y): We will solve this problem using Conformal Mappings. iÁ Remark 1. Mean Value Theorem for Analytic Functions. If Cr = fz = z0 + re ; 0 · Á < 2¼g is a circle centered at z0 with radius r, and f(z); z = x + iy 2 C, is analytic inside Cr and continuous inside and on Cr, then the function value in the center of the circle is expressed via the boundary integral: Z 2¼ I 1 iÁ 1 f(z0) = f(z0 + re )dÁ = f(z)jdzj; (2) 2¼ 0 2¼r Cr where jdzj = rdÁ is a differential arc length. Corollary. Mean Value Theorem for Harmonic Functions. If u(x; y) is a harmonic function iÁ inside Cr = fz = z0 + re ; 0 · Á < 2¼g, i.e. ¢u = uxx + uyy = 0, then it is a real part of some analytic function f(z) = u(x; y) + iv(x; y) (this is true since a circle is simply connected.) Hence, taking the real part of (2), we get the value of u(x; y) at z0 = x0 + iy0 (in the center of the circle) is also expressed as the boundary integral: I 1 u(x0; y0) = u(x; y)jdzj; (3) 2¼r Cr where in the integrand (x; y) 2 Cr is a point on the circle. -
Arxiv:1602.04855V4 [Math.NA] 2 Nov 2018 1 Z Dσ(X) = − Σ(Y)N ˆ · ∇Y Log |Y − X| Ds(Y), X∈ / Γ
CONFORMAL MAPPING VIA A DENSITY CORRESPONDENCE FOR THE DOUBLE-LAYER POTENTIAL ¨ MATT WALA∗ AND ANDREAS KLOCKNER∗ Abstract. We derive a representation formula for harmonic polynomials and Laurent polynomials in terms of densities of the double-layer potential on bounded piecewise smooth and simply connected domains. From this result, we obtain a method for the numerical computation of conformal maps that applies to both exterior and interior regions. We present analysis and numerical experiments supporting the accuracy and broad applicability of the method. Key words. conformal map, integral equations, Faber polynomial, high-order methods AMS subject classifications. 65E05, 30C30, 65R20 1. Introduction. This paper presents an integral equation method for numerical conformal mapping, using an integral equation based on the Faber polynomials (on the interior) and their counterpart, Faber-Laurent polynomials (on the exterior). Our method is applicable to computing the conformal map from the interior and exterior of domains bounded by a piecewise smooth Jordan curve Γ onto the interior/exterior of the unit disk. Like most techniques for conformal mapping, this method relies on computing a boundary correspondence function between Γ and the boundary of the target domain. From the boundary correspondence, the mapping function can be derived via a Cauchy integral [25, p. 381]. The numerical construction of a function that maps the exterior of a simply connected region conformally onto the exterior of some other region arises in a number of applications including fluid mechanics [8, Ch. 4.5], the generation of finite element meshes for problems in fracture mechanics [45], the design of optical media [31], the analysis of iterative methods [15,16,40], and the solution of initial value problems [32]. -
A Note on the Schwarz Lemma for Harmonic Functions
Filomat 34:11 (2020), 3711–3720 Published by Faculty of Sciences and Mathematics, https://doi.org/10.2298/FIL2011711S University of Nis,ˇ Serbia Available at: http://www.pmf.ni.ac.rs/filomat A Note on the Schwarz Lemma for Harmonic Functions Marek Svetlika aUniversity of Belgrade, Faculty of Mathematics 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 tz P C : |z| 1u to the interval p¡1; 1q (or to itself). First, we cite a theorem which is known as the Schwarz lemma for harmonic functions and is considered a classical result. Theorem 1 ([10],[9, p.77]). Let f : U Ñ U be a harmonic function such that f p0q 0. Then 4 | f pzq| ¤ arctan |z|; for all z P U; π and this inequality is sharp for each point z P U. In 1977, H. W. Hethcote [11] improved this result by removing the assumption f p0q 0 and proved the following theorem. Theorem 2 ([11, Theorem 1] and [29, Theorem 3.6.1]). Let f : U Ñ U be a harmonic function. Then § § § 2 § § 1 ¡ |z| § 4 § f pzq ¡ f p0q§ ¤ arctan |z|; for all z P U: 1 |z|2 π As was written in [25], it seems that researchers had some difficulties handling the case f p0q 0, where f is a harmonic mapping from U to itself.