Local Distortion of M-Conformal Mappings
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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 Extended Relativity Theory in Clifford Spaces
THE EXTENDED RELATIVITY THEORY IN CLIFFORD SPACES C. Castroa and M. Pav·si·cb May 21, 2004 aCenter for Theoretical Studies of Physical Systems, Clark Atlanta University, Atlanta bJo·zef Stefan Institute, Jamova 39, SI-1000 Ljubljana, Slovenia; Email: [email protected] Abstract A brief review of some of the most important features of the Extended Rela- tivity theory in Cli®ord-spaces (C-spaces) is presented whose " point" coordinates are noncommuting Cli®ord-valued quantities and which incorporate the lines, ar- eas, volumes,.... degrees of freedom associated with the collective particle, string, membrane,... dynamics of p-loops (closed p-branes) living in target D-dimensional spacetime backgrounds. C-space Relativity naturally incorporates the ideas of an invariant length (Planck scale), maximal acceleration, noncommuting coordinates, supersymmetry, holography, higher derivative gravity with torsion and variable di- mensions/signatures that allows to study the dynamics of all (closed) p-branes, for all values of p, on a uni¯ed footing. It resolves the ordering ambiguities in QFT and the problem of time in Cosmology. A discussion of the maximal-acceleration Rela- tivity principle in phase-spaces follows along with the study of the invariance group of symmetry transformations in phase-space that allows to show why Planck areas are invariant under acceleration-boosts transformations and which seems to suggest that a maximal-string tension principle may be operating in Nature. We continue by pointing out how the relativity of signatures of the underlying n-dimensional spacetime results from taking di®erent n-dimensional slices through C-space. The conformal group emerges as a natural subgroup of the Cli®ord group and Relativity in C-spaces involves natural scale changes in the sizes of physical objects without the introduction of forces nor Weyl's gauge ¯eld of dilations. -
Algebraic Foundations of Split Hypercomplex Nonlinear Adaptive
Mathematical Methods in the Research Article Applied Sciences Received XXXX (www.interscience.wiley.com) DOI: 10.1002/sim.0000 MOS subject classification: 60G35; 15A66 Algebraic foundations of split hypercomplex nonlinear adaptive filtering E. Hitzer∗ A split hypercomplex learning algorithm for the training of nonlinear finite impulse response adaptive filters for the processing of hypercomplex signals of any dimension is proposed. The derivation strictly takes into account the laws of hypercomplex algebra and hypercomplex calculus, some of which have been neglected in existing learning approaches (e.g. for quaternions). Already in the case of quaternions we can predict improvements in performance of hypercomplex processes. The convergence of the proposed algorithms is rigorously analyzed. Copyright c 2011 John Wiley & Sons, Ltd. Keywords: Quaternionic adaptive filtering, Hypercomplex adaptive filtering, Nonlinear adaptive filtering, Hypercomplex Multilayer Perceptron, Clifford geometric algebra 1. Introduction Split quaternion nonlinear adaptive filtering has recently been treated by [23], who showed its superior performance for Saito’s Chaotic Signal and for wind forecasting. The quaternionic methods constitute a generalization of complex valued adaptive filters, treated in detail in [19]. A method of quaternionic least mean square algorithm for adaptive quaternionic has previously been developed in [22]. Additionally, [24] successfully proposes the usage of local analytic fully quaternionic functions in the Quaternion Nonlinear Gradient Descent (QNGD). Yet the unconditioned use of analytic fully quaternionic activation functions in neural networks faces problems with poles due to the Liouville theorem [3]. The quaternion algebra of Hamilton is a special case of the higher dimensional Clifford algebras [10]. The problem with poles in nonlinear analytic functions does not generally occur for hypercomplex activation functions in Clifford algebras, where the Dirac and the Cauchy-Riemann operators are not elliptic [21], as shown, e.g., for hyperbolic numbers in [17]. -
Hermitian Clifford Analysis on Superspace
Hermitian Clifford analysis on superspace Hennie De Schepper, Alí Guzmán Adán, Frank Sommen Clifford Research Group, Department of Mathematical Analysis, Faculty of Engineering and Architecture, Ghent University, Galglaan 2, 9000 Ghent, Belgium. Abstract In this paper we first recall the proper algebraic framework, i.e. the radial algebra, needed to extend Hermitian Clifford analysis to the superspace setting. The fundamental objects for this extension then are introduced by means of an abstract complex structure on the Hermitian radial algebra. This leads to a natural representation of this Hermitian radial algebra on superspace. Keywords. Hemitian Clifford analysis, Superspace, Radial algebra Mathematics Subject Classification (2010). 1 Introduction Clifford analysis nowadays is a well established mathematical discipline constituting a natural refinement of harmonic analysis. In its most simple setting, it focusses on the null solutions of the Dirac operator Pm m @x = j=1 ej@xj , where the elements (e1; : : : ; em) form an orthonormal basis for the Euclidean space R leading to the construction of the real Clifford algebra R0;m. This setting is known as the orthogonal case since the fundamental group leaving the Dirac operator invariant is Spin(m) which is a double covering of SO(m). By taking the dimension even, say 2m, and introducing a so-called complex structure J 2 SO(2m), the fundamental elements of Hermitian Clifford analysis arise in a natural way from the orthogonal setting. The Hermitian case focusses on h-monogenic functions, h-monogenicity being expressed by means of two mutually adjoint Dirac operators which are invariant under the realization of the unitary group U(m) 1 in Spin(2m). -
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). -
Representations of the Lie Superalgebra Osp(1L2n)
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 17 (2021), 031, 27 pages Representations of the Lie Superalgebra osp(1j2n) with Polynomial Bases Asmus K. BISBO a, Hendrik DE BIE b and Joris VAN DER JEUGT a a) Department of Applied Mathematics, Computer Science and Statistics, Ghent University, Krijgslaan 281-S9, B-9000 Gent, Belgium E-mail: [email protected], [email protected] b) Department of Electronics and Information Systems, Faculty of Engineering and Architecture, Ghent University, Krijgslaan 281-S8, B-9000 Gent, Belgium E-mail: [email protected] Received June 30, 2020, in final form March 10, 2021; Published online March 25, 2021 https://doi.org/10.3842/SIGMA.2021.031 Abstract. We study a particular class of infinite-dimensional representations of osp(1j2n). These representations Ln(p) are characterized by a positive integer p, and are the lowest com- ponent in the p-fold tensor product of the metaplectic representation of osp(1j2n). We con- struct a new polynomial basis for Ln(p) arising from the embedding osp(1j2np) ⊃ osp(1j2n). The basis vectors of Ln(p) are labelled by semi-standard Young tableaux, and are expressed as Clifford algebra valued polynomials with integer coefficients in np variables. Using com- binatorial properties of these tableau vectors it is deduced that they form indeed a basis. The computation of matrix elements of a set of generators of osp(1j2n) on these basis vectors requires further combinatorics, such as the action of a Young subgroup on the horizontal strips of the tableau. Key words: representation theory; Lie superalgebras; Young tableaux; Clifford analysis; parabosons 2020 Mathematics Subject Classification: 17B10; 05E10; 81R05; 15A66 1 Introduction In representation theory of Lie algebras, Lie superalgebras or their deformations, there are often three problems to be tackled. -
Linking Clifford Analysis and Combinatorics Through Bijective Methods
9th International Conference on Clifford Algebras and their Applications in Mathematical Physics K. Gurlebeck¨ (ed.) Weimar, Germany, 15–20 July 2011 LINKING CLIFFORD ANALYSIS AND COMBINATORICS THROUGH BIJECTIVE METHODS H. R. Maloneka;c and M. I. Falcao˜ b;c a Department of Mathematics, University of Aveiro, Portugal. b Department of Mathematics and Applications, University of Minho, Portugal. c Center for Research and Development in Mathematics and Applications, Portugal. Keywords: Monogenic polynomials, Special Functions, Appell sequences, combinatorial iden- tities Abstract. The application of Clifford Analysis methods in Combinatorics has some peculiari- ties due to the use of noncommutative algebras. But it seems natural to expect from here some new results different from those obtained by using approaches based on several complex vari- able. For instances, the fact that in Clifford Analysis the point-wise multiplication of monogenic functions as well as their composition are not algebraically closed in this class of generalized holomorphic functions causes serious problems. Indeed, this is one of the reasons why in poly- nomial approximation almost every problem needs the construction of specially adapted poly- nomial bases. Our aim is to show that the analysis and comparison of different representations of the same polynomial or entire function allow to link Clifford Analysis and Combinatorics by means of bijective methods. In this context we also stress the central role of the hypercomplex derivative for power series representations in connection with the concept of Appell sequences as analytic tools for establishing this link. 1 1 INTRODUCTION “Remember, it’s supposed to be fun” Richard Feynman, quoted in Some time with Feynman by L. -
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. -
A Theory of Neural Computation with Clifford Algebras
A Theory of Neural Computation with Clifford Algebras Dissertation zur Erlangung des akademischen Grades Doktor der Ingenieurwissenschaften (Dr.–Ing.) der Technischen Fakult¨at der Christian-Albrechts-Universit¨at zu Kiel Sven Buchholz Kiel 2005 1. Gutachter Prof. Dr. Gerald Sommer (Kiel) 2. Gutachter Prof. Dr. Reinhold Schneider (Kiel) 3. Gutachter Prof. Dr. Thomas Martinetz (L ¨ubeck) Datumderm¨undlichenPr¨ufung: 16.03.2005 Abstract The present thesis introduces Clifford Algebra as a framework for neural compu- tation. Clifford Algebra subsumes, for example, the reals, complex numbers and quaternions. Neural computation with Clifford algebras is model–based. This principle is established by constructing Clifford algebras from quadratic spaces. Then the subspace grading inherent to any Clifford algebra is introduced, which allows the representation of different geometric entities like points, lines, and so on. The above features of Clifford algebras are then taken as motivation for introducing the Basic Clifford Neuron (BCN), which is solely based on the geometric product of the underlying Clifford algebra. Using BCNs the Linear Associator is generalized to the Clifford associator. As a second type of Clifford neuron the Spinor Clifford Neuron (SCN) is presented. The propagation function of a SCN is an orthogonal transformation. Examples of how Clifford neurons can be used advantageously are given, including the linear computation of M¨obius transformations by a SCN. A systematic basis for Clifford neural computation is provided by the important notions of isomorphic Clifford neurons and isomorphic representations. After the neuron level is established, the discussion continues with (Spinor) Clifford Multi- layer Perceptrons. The treatment is divided into two parts according to the type of activation function used. -
Schwarz-Christoffel Transformations by Philip P. Bergonio (Under the Direction of Edward Azoff) Abstract the Riemann Mapping
Schwarz-Christoffel Transformations by Philip P. Bergonio (Under the direction of Edward Azoff) Abstract The Riemann Mapping Theorem guarantees that the upper half plane is conformally equivalent to the interior domain determined by any polygon. Schwarz-Christoffel transfor- mations provide explicit formulas for the maps that work. Popular textbook treatments of the topic range from motivational and contructive to proof-oriented. The aim of this paper is to combine the strengths of these expositions, filling in details and adding more information when necessary. In particular, careful attention is paid to the crucial fact, taken for granted in most elementary texts, that all conformal equivalences between the domains in question extend continuously to their closures. Index words: Complex Analysis, Schwarz-Christoffel Transformations, Polygons in the Complex Plane Schwarz-Christoffel Transformations by Philip P. Bergonio B.S., Georgia Southwestern State University, 2003 A Thesis Submitted to the Graduate Faculty of The University of Georgia in Partial Fulfillment of the Requirements for the Degree Master of Arts Athens, Georgia 2007 c 2007 Philip P. Bergonio All Rights Reserved Schwarz-Christoffel Transformations by Philip P. Bergonio Approved: Major Professor: Edward Azoff Committee: Daniel Nakano Shuzhou Wang Electronic Version Approved: Maureen Grasso Dean of the Graduate School The University of Georgia December 2007 Table of Contents Page Chapter 1 Introduction . 1 2 Background Information . 5 2.1 Preliminaries . 5 2.2 Linear Curves and Polygons . 8 3 Two Examples and Motivation for the Formula . 13 3.1 Prototypical Examples . 13 3.2 Motivation for the Formula . 16 4 Properties of Schwarz-Christoffel Candidates . 19 4.1 Well-Definedness of f ..................... -
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.