The Geometry of the Complex Domain.
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Chapter 13 the Geometry of Circles
Chapter 13 TheR. Connelly geometry of circles Math 452, Spring 2002 Math 4520, Fall 2017 CLASSICAL GEOMETRIES So far we have been studying lines and conics in the Euclidean plane. What about circles, 14. The geometry of circles one of the basic objects of study in Euclidean geometry? One approach is to use the complex numbersSo far .we Recall have thatbeen the studying projectivities lines and of conics the projective in the Euclidean plane overplane., whichWhat weabout call 2, circles, Cone of the basic objects of study in Euclidean geometry? One approachC is to use CP are given by 3 by 3 matrices, and these projectivities restricted to a complex projective the complex numbers 1C. Recall that the projectivities of the projective plane over C, line,v.rhich which we wecall call Cp2, a CPare, given are the by Moebius3 by 3 matrices, functions, and whichthese projectivities themselves correspondrestricted to to a 2-by-2 matrices.complex Theprojective Moebius line, functions which we preservecall a Cpl the, are cross the Moebius ratio. This functions, is where which circles themselves come in. correspond to a 2 by 2 matrix. The Moebius functions preserve the cross ratio. This is 13.1where circles The come cross in. ratio for the complex field We14.1 look The for anothercross ratio geometric for the interpretation complex field of the cross ratio for the complex field, or better 1 yet forWeCP look= Cfor[f1g another. Recall geometric the polarinterpretation decomposition of the cross of a complexratio for numberthe complexz = refield,iθ, where r =orjz betterj is the yet magnitude for Cpl = ofCz U, and{ 00 } .Recallθ is the the angle polar that decomposition the line through of a complex 0 and znumbermakes with thez real -rei9, axis. -
The Integral Geometry of Line Complexes and a Theorem of Gelfand-Graev Astérisque, Tome S131 (1985), P
Astérisque VICTOR GUILLEMIN The integral geometry of line complexes and a theorem of Gelfand-Graev Astérisque, tome S131 (1985), p. 135-149 <http://www.numdam.org/item?id=AST_1985__S131__135_0> © Société mathématique de France, 1985, tous droits réservés. L’accès aux archives de la collection « Astérisque » (http://smf4.emath.fr/ Publications/Asterisque/) implique l’accord avec les conditions générales d’uti- lisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Société Mathématique de France Astérisque, hors série, 1985, p. 135-149 THE INTEGRAL GEOMETRY OF LINE COMPLEXES AND A THEOREM OF GELFAND-GRAEV BY Victor GUILLEMIN 1. Introduction Let P = CP3 be the complex three-dimensional projective space and let G = CG(2,4) be the Grassmannian of complex two-dimensional subspaces of C4. To each point p E G corresponds a complex line lp in P. Given a smooth function, /, on P we will show in § 2 how to define properly the line integral, (1.1) f(\)d\ d\. = f(p). d A complex hypersurface, 5, in G is called admissible if there exists no smooth function, /, which is not identically zero but for which the line integrals, (1,1) are zero for all p G 5. In other words if S is admissible, then, in principle, / can be determined by its integrals over the lines, Zp, p G 5. In the 60's GELFAND and GRAEV settled the problem of characterizing which subvarieties, 5, of G have this property. -
Finite Projective Geometries 243
FINITE PROJECTÎVEGEOMETRIES* BY OSWALD VEBLEN and W. H. BUSSEY By means of such a generalized conception of geometry as is inevitably suggested by the recent and wide-spread researches in the foundations of that science, there is given in § 1 a definition of a class of tactical configurations which includes many well known configurations as well as many new ones. In § 2 there is developed a method for the construction of these configurations which is proved to furnish all configurations that satisfy the definition. In §§ 4-8 the configurations are shown to have a geometrical theory identical in most of its general theorems with ordinary projective geometry and thus to afford a treatment of finite linear group theory analogous to the ordinary theory of collineations. In § 9 reference is made to other definitions of some of the configurations included in the class defined in § 1. § 1. Synthetic definition. By a finite projective geometry is meant a set of elements which, for sugges- tiveness, are called points, subject to the following five conditions : I. The set contains a finite number ( > 2 ) of points. It contains subsets called lines, each of which contains at least three points. II. If A and B are distinct points, there is one and only one line that contains A and B. HI. If A, B, C are non-collinear points and if a line I contains a point D of the line AB and a point E of the line BC, but does not contain A, B, or C, then the line I contains a point F of the line CA (Fig. -
ROBERT L. FOOTE CURRICULUM VITA March 2017 Address
ROBERT L. FOOTE CURRICULUM VITA March 2017 Address/Telephone/E-Mail Department of Mathematics & Computer Science Wabash College Crawfordsville, Indiana 47933 (765) 361-6429 [email protected] Personal Date of Birth: December 2, 1953 Citizenship: USA Education Ph.D., Mathematics, University of Michigan, April 1983 Dissertation: Curvature Estimates for Monge-Amp`ere Foliations Thesis Advisor: Daniel M. Burns Jr. M.A., Mathematics, University of Michigan, April 1978 B.A., Mathematics, Kalamazoo College, June 1976 Magna cum Laude with Honors in Mathematics, Phi Beta Kappa, Heyl Science Scholarship Employment 1989–present, Wabash College Department Chair, 1997–2001, 2009–2012 Full Professor since 2004 Associate Professor, 1993–2004 Assistant Professor, 1991–1993 Byron K. Trippet Assistant Professor, 1989–1991 1983–1989, Texas Tech University, Assistant Professor (granted tenure) 1983, Kalamazoo College, Visiting Instructor 1976–1982, University of Michigan, Graduate Student Teaching Assistant 1976, 1977, The Upjohn Company, Mathematical Analyst Research Visits 2009, Korea Institute for Advanced Study (KIAS), Visiting Scholar Three weeks at the invitation of C. K. Han. 2009, Pennsylvania State Univ., Shapiro Visitor Four weeks at the invitation of Sergei Tabachnikov. 2008–2009, Univ. of Georgia, Visiting Scholar (sabbatical leave) 1996–1997, 2003–2004, Univ. of Illinois at Urbana Champaign, Visiting Scholar (sabbatical leave) 1991, Pohang Institute of Science and Technology, Pohang, Korea Three months at the invitation of C. K. Han. 1990, Texas Tech University Ten weeks at the invitation of Lance D. Drager. Current Fields of Interest Primary: Differential Geometry, Integral Geometry Professional Affiliations American Mathematical Society, Mathematical Association of America. Teaching Experience Graduate courses Differentiable manifolds, real analysis, complex analysis. -
CR Singular Immersions of Complex Projective Spaces
Beitr¨agezur Algebra und Geometrie Contributions to Algebra and Geometry Volume 43 (2002), No. 2, 451-477. CR Singular Immersions of Complex Projective Spaces Adam Coffman∗ Department of Mathematical Sciences Indiana University Purdue University Fort Wayne Fort Wayne, IN 46805-1499 e-mail: Coff[email protected] Abstract. Quadratically parametrized smooth maps from one complex projective space to another are constructed as projections of the Segre map of the complexifi- cation. A classification theorem relates equivalence classes of projections to congru- ence classes of matrix pencils. Maps from the 2-sphere to the complex projective plane, which generalize stereographic projection, and immersions of the complex projective plane in four and five complex dimensions, are considered in detail. Of particular interest are the CR singular points in the image. MSC 2000: 14E05, 14P05, 15A22, 32S20, 32V40 1. Introduction It was shown by [23] that the complex projective plane CP 2 can be embedded in R7. An example of such an embedding, where R7 is considered as a subspace of C4, and CP 2 has complex homogeneous coordinates [z1 : z2 : z3], was given by the following parametric map: 1 2 2 [z1 : z2 : z3] 7→ 2 2 2 (z2z¯3, z3z¯1, z1z¯2, |z1| − |z2| ). |z1| + |z2| + |z3| Another parametric map of a similar form embeds the complex projective line CP 1 in R3 ⊆ C2: 1 2 2 [z0 : z1] 7→ 2 2 (2¯z0z1, |z1| − |z0| ). |z0| + |z1| ∗The author’s research was supported in part by a 1999 IPFW Summer Faculty Research Grant. 0138-4821/93 $ 2.50 c 2002 Heldermann Verlag 452 Adam Coffman: CR Singular Immersions of Complex Projective Spaces This may look more familiar when restricted to an affine neighborhood, [z0 : z1] = (1, z) = (1, x + iy), so the set of complex numbers is mapped to the unit sphere: 2x 2y |z|2 − 1 z 7→ ( , , ), 1 + |z|2 1 + |z|2 1 + |z|2 and the “point at infinity”, [0 : 1], is mapped to the point (0, 0, 1) ∈ R3. -
Complex Analysis and Complex Geometry
Complex Analysis and Complex Geometry Finnur Larusson,´ University of Adelaide Norman Levenberg, Indiana University Rasul Shafikov, University of Western Ontario Alexandre Sukhov, Universite´ des Sciences et Technologies de Lille May 1–6, 2016 1 Overview of the Field Complex analysis and complex geometry form synergy through the geometric ideas used in analysis and an- alytic tools employed in geometry, and therefore they should be viewed as two aspects of the same subject. The fundamental objects of the theory are complex manifolds and, more generally, complex spaces, holo- morphic functions on them, and holomorphic maps between them. Holomorphic functions can be defined in three equivalent ways as complex-differentiable functions, convergent power series, and as solutions of the homogeneous Cauchy-Riemann equation. The threefold nature of differentiability over the complex numbers gives complex analysis its distinctive character and is the ultimate reason why it is linked to so many areas of mathematics. Plurisubharmonic functions are not as well known to nonexperts as holomorphic functions. They were first explicitly defined in the 1940s, but they had already appeared in attempts to geometrically describe domains of holomorphy at the very beginning of several complex variables in the first decade of the 20th century. Since the 1960s, one of their most important roles has been as weights in a priori estimates for solving the Cauchy-Riemann equation. They are intimately related to the complex Monge-Ampere` equation, the second partial differential equation of complex analysis. There is also a potential-theoretic aspect to plurisubharmonic functions, which is the subject of pluripotential theory. In the early decades of the modern era of the subject, from the 1940s into the 1970s, the notion of a complex space took shape and the geometry of analytic varieties and holomorphic maps was developed. -
An Introduction to Complex Analysis and Geometry John P. D'angelo
An Introduction to Complex Analysis and Geometry John P. D'Angelo Dept. of Mathematics, Univ. of Illinois, 1409 W. Green St., Urbana IL 61801 [email protected] 1 2 c 2009 by John P. D'Angelo Contents Chapter 1. From the real numbers to the complex numbers 11 1. Introduction 11 2. Number systems 11 3. Inequalities and ordered fields 16 4. The complex numbers 24 5. Alternative definitions of C 26 6. A glimpse at metric spaces 30 Chapter 2. Complex numbers 35 1. Complex conjugation 35 2. Existence of square roots 37 3. Limits 39 4. Convergent infinite series 41 5. Uniform convergence and consequences 44 6. The unit circle and trigonometry 50 7. The geometry of addition and multiplication 53 8. Logarithms 54 Chapter 3. Complex numbers and geometry 59 1. Lines, circles, and balls 59 2. Analytic geometry 62 3. Quadratic polynomials 63 4. Linear fractional transformations 69 5. The Riemann sphere 73 Chapter 4. Power series expansions 75 1. Geometric series 75 2. The radius of convergence 78 3. Generating functions 80 4. Fibonacci numbers 82 5. An application of power series 85 6. Rationality 87 Chapter 5. Complex differentiation 91 1. Definitions of complex analytic function 91 2. Complex differentiation 92 3. The Cauchy-Riemann equations 94 4. Orthogonal trajectories and harmonic functions 97 5. A glimpse at harmonic functions 98 6. What is a differential form? 103 3 4 CONTENTS Chapter 6. Complex integration 107 1. Complex-valued functions 107 2. Line integrals 109 3. Goursat's proof 116 4. The Cauchy integral formula 119 5. -
Daniel Huybrechts
Universitext Daniel Huybrechts Complex Geometry An Introduction 4u Springer Daniel Huybrechts Universite Paris VII Denis Diderot Institut de Mathematiques 2, place Jussieu 75251 Paris Cedex 05 France e-mail: [email protected] Mathematics Subject Classification (2000): 14J32,14J60,14J81,32Q15,32Q20,32Q25 Cover figure is taken from page 120. Library of Congress Control Number: 2004108312 ISBN 3-540-21290-6 Springer Berlin Heidelberg New York This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilm or in any other way, and storage in data banks. Duplication of this publication or parts thereof is permitted only under the provisions of the German Copyright Law of September 9,1965, in its current version, and permission for use must always be obtained from Springer. Violations are liable for prosecution under the German Copyright Law. Springer is a part of Springer Science+Business Media springeronline.com © Springer-Verlag Berlin Heidelberg 2005 Printed in Germany The use of general descriptive names, registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. Cover design: Erich Kirchner, Heidelberg Typesetting by the author using a Springer KTjiX macro package Production: LE-TgX Jelonek, Schmidt & Vockler GbR, Leipzig Printed on acid-free paper 46/3142YL -543210 Preface Complex geometry is a highly attractive branch of modern mathematics that has witnessed many years of active and successful research and that has re- cently obtained new impetus from physicists' interest in questions related to mirror symmetry. -
Complex Algebraic Geometry
Complex Algebraic Geometry Jean Gallier∗ and Stephen S. Shatz∗∗ ∗Department of Computer and Information Science University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] ∗∗Department of Mathematics University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] February 25, 2011 2 Contents 1 Complex Algebraic Varieties; Elementary Theory 7 1.1 What is Geometry & What is Complex Algebraic Geometry? . .......... 7 1.2 LocalStructureofComplexVarieties. ............ 14 1.3 LocalStructureofComplexVarieties,II . ............. 28 1.4 Elementary Global Theory of Varieties . ........... 42 2 Cohomologyof(Mostly)ConstantSheavesandHodgeTheory 73 2.1 RealandComplex .................................... ...... 73 2.2 Cohomology,deRham,Dolbeault. ......... 78 2.3 Hodge I, Analytic Preliminaries . ........ 89 2.4 Hodge II, Globalization & Proof of Hodge’s Theorem . ............ 107 2.5 HodgeIII,TheK¨ahlerCase . .......... 131 2.6 Hodge IV: Lefschetz Decomposition & the Hard Lefschetz Theorem............... 147 2.7 ExtensionsofResultstoVectorBundles . ............ 162 3 The Hirzebruch-Riemann-Roch Theorem 165 3.1 Line Bundles, Vector Bundles, Divisors . ........... 165 3.2 ChernClassesandSegreClasses . .......... 179 3.3 The L-GenusandtheToddGenus .............................. 215 3.4 CobordismandtheSignatureTheorem. ........... 227 3.5 The Hirzebruch–Riemann–Roch Theorem (HRR) . ............ 232 3 4 CONTENTS Preface This manuscript is based on lectures given by Steve Shatz for the course Math 622/623–Complex Algebraic Geometry, during Fall 2003 and Spring 2004. The process for producing this manuscript was the following: I (Jean Gallier) took notes and transcribed them in LATEX at the end of every week. A week later or so, Steve reviewed these notes and made changes and corrections. After the course was over, Steve wrote up additional material that I transcribed into LATEX. The following manuscript is thus unfinished and should be considered as work in progress. -
Ishikawa-Oyama.Pdf
Proc. of 15th International Workshop Journal of Singularities on Singularities, Sao˜ Carlos, 2018 Volume 22 (2020), 373-384 DOI: 10.5427/jsing.2020.22v TOPOLOGY OF COMPLEMENTS TO REAL AFFINE SPACE LINE ARRANGEMENTS GOO ISHIKAWA AND MOTOKI OYAMA ABSTRACT. It is shown that the diffeomorphism type of the complement to a real space line arrangement in any dimensional affine ambient space is determined only by the number of lines and the data on multiple points. 1. INTRODUCTION Let A = f`1;`2;:::;`dg be a real space line arrangement, or a configuration, consisting of affine 3 d d-lines in R . The different lines `i;` j(i 6= j) may intersect, so that the union [i=1`i is an affine real algebraic curve of degree d in R3 possibly with multiple points. In this paper we determine the topological 3 d type of the complement M(A ) := R n([i=1`i) of A , which is an open 3-manifold. We observe that the topological type M(A ) is determined only by the number of lines and the data on multiple points of A . Moreover we determine the diffeomorphism type of M(A ). n n i j i j Set D := fx 2 R j kxk ≤ 1g, the n-dimensional closed disk. The pair (D × D ;D × ¶(D )) with i + j = n; 0 ≤ i;0 ≤ j, is called an n-dimensional handle of index j (see [17][1] for instance). Now take one D3 and, for any non-negative integer g, attach to it g-number of 3-dimensional handles 2 1 2 1 (Dk × Dk;Dk × ¶(Dk)) of index 1 (1 ≤ k ≤ g), by an attaching embedding g G 2 1 3 2 j : (Dk × ¶(Dk)) ! ¶(D ) = S k=1 such that the obtained 3-manifold 3 S Fg 2 1 Bg := D j ( k=1(Dk × Dk)) is orientable. -
Geometry in the Age of Enlightenment
Geometry in the Age of Enlightenment Raymond O. Wells, Jr. ∗ July 2, 2015 Contents 1 Introduction 1 2 Algebraic Geometry 3 2.1 Algebraic Curves of Degree Two: Descartes and Fermat . 5 2.2 Algebraic Curves of Degree Three: Newton and Euler . 11 3 Differential Geometry 13 3.1 Curvature of curves in the plane . 17 3.2 Curvature of curves in space . 26 3.3 Curvature of a surface in space: Euler in 1767 . 28 4 Conclusion 30 1 Introduction The Age of Enlightenment is a term that refers to a time of dramatic changes in western society in the arts, in science, in political thinking, and, in particular, in philosophical discourse. It is generally recognized as being the period from the mid 17th century to the latter part of the 18th century. It was a successor to the renaissance and reformation periods and was followed by what is termed the romanticism of the 19th century. In his book A History of Western Philosophy [25] Bertrand Russell (1872{1970) gives a very lucid description of this time arXiv:1507.00060v1 [math.HO] 30 Jun 2015 period in intellectual history, especially in Book III, Chapter VI{Chapter XVII. He singles out Ren´eDescartes as being the founder of the era of new philosophy in 1637 and continues to describe other philosophers who also made significant contributions to mathematics as well, such as Newton and Leibniz. This time of intellectual fervor included literature (e.g. Voltaire), music and the world of visual arts as well. One of the most significant developments was perhaps in the political world: here the absolutism of the church and of the monarchies ∗Jacobs University Bremen; University of Colorado at Boulder; [email protected] 1 were questioned by the political philosophers of this era, ushering in the Glo- rious Revolution in England (1689), the American Revolution (1776), and the bloody French Revolution (1789). -
Linear Algebra I: Vector Spaces A
Linear Algebra I: Vector Spaces A 1 Vector spaces and subspaces 1.1 Let F be a field (in this book, it will always be either the field of reals R or the field of complex numbers C). A vector space V D .V; C; o;˛./.˛2 F// over F is a set V with a binary operation C, a constant o and a collection of unary operations (i.e. maps) ˛ W V ! V labelled by the elements of F, satisfying (V1) .x C y/ C z D x C .y C z/, (V2) x C y D y C x, (V3) 0 x D o, (V4) ˛ .ˇ x/ D .˛ˇ/ x, (V5) 1 x D x, (V6) .˛ C ˇ/ x D ˛ x C ˇ x,and (V7) ˛ .x C y/ D ˛ x C ˛ y. Here, we write ˛ x and we will write also ˛x for the result ˛.x/ of the unary operation ˛ in x. Often, one uses the expression “multiplication of x by ˛”; but it is useful to keep in mind that what we really have is a collection of unary operations (see also 5.1 below). The elements of a vector space are often referred to as vectors. In contrast, the elements of the field F are then often referred to as scalars. In view of this, it is useful to reflect for a moment on the true meaning of the axioms (equalities) above. For instance, (V4), often referred to as the “associative law” in fact states that the composition of the functions V ! V labelled by ˇ; ˛ is labelled by the product ˛ˇ in F, the “distributive law” (V6) states that the (pointwise) sum of the mappings labelled by ˛ and ˇ is labelled by the sum ˛ C ˇ in F, and (V7) states that each of the maps ˛ preserves the sum C.