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Toponogov.V.A.Differential.Geometry
Victor Andreevich Toponogov with the editorial assistance of Vladimir Y. Rovenski Differential Geometry of Curves and Surfaces A Concise Guide Birkhauser¨ Boston • Basel • Berlin Victor A. Toponogov (deceased) With the editorial assistance of: Department of Analysis and Geometry Vladimir Y. Rovenski Sobolev Institute of Mathematics Department of Mathematics Siberian Branch of the Russian Academy University of Haifa of Sciences Haifa, Israel Novosibirsk-90, 630090 Russia Cover design by Alex Gerasev. AMS Subject Classification: 53-01, 53Axx, 53A04, 53A05, 53A55, 53B20, 53B21, 53C20, 53C21 Library of Congress Control Number: 2005048111 ISBN-10 0-8176-4384-2 eISBN 0-8176-4402-4 ISBN-13 978-0-8176-4384-3 Printed on acid-free paper. c 2006 Birkhauser¨ Boston All rights reserved. This work may not be translated or copied in whole or in part without the writ- ten permission of the publisher (Birkhauser¨ Boston, c/o Springer Science+Business Media Inc., 233 Spring Street, New York, NY 10013, USA) and the author, except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and re- trieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed in the United States of America. (TXQ/EB) 987654321 www.birkhauser.com Contents Preface ....................................................... vii About the Author ............................................. -
Differential Geometry
Differential Geometry J.B. Cooper 1995 Inhaltsverzeichnis 1 CURVES AND SURFACES—INFORMAL DISCUSSION 2 1.1 Surfaces ................................ 13 2 CURVES IN THE PLANE 16 3 CURVES IN SPACE 29 4 CONSTRUCTION OF CURVES 35 5 SURFACES IN SPACE 41 6 DIFFERENTIABLEMANIFOLDS 59 6.1 Riemannmanifolds .......................... 69 1 1 CURVES AND SURFACES—INFORMAL DISCUSSION We begin with an informal discussion of curves and surfaces, concentrating on methods of describing them. We shall illustrate these with examples of classical curves and surfaces which, we hope, will give more content to the material of the following chapters. In these, we will bring a more rigorous approach. Curves in R2 are usually specified in one of two ways, the direct or parametric representation and the implicit representation. For example, straight lines have a direct representation as tx + (1 t)y : t R { − ∈ } i.e. as the range of the function φ : t tx + (1 t)y → − (here x and y are distinct points on the line) and an implicit representation: (ξ ,ξ ): aξ + bξ + c =0 { 1 2 1 2 } (where a2 + b2 = 0) as the zero set of the function f(ξ ,ξ )= aξ + bξ c. 1 2 1 2 − Similarly, the unit circle has a direct representation (cos t, sin t): t [0, 2π[ { ∈ } as the range of the function t (cos t, sin t) and an implicit representation x : 2 2 → 2 2 { ξ1 + ξ2 =1 as the set of zeros of the function f(x)= ξ1 + ξ2 1. We see from} these examples that the direct representation− displays the curve as the image of a suitable function from R (or a subset thereof, usually an in- terval) into two dimensional space, R2. -
Differentiable Manifolds
Gerardo F. Torres del Castillo Differentiable Manifolds ATheoreticalPhysicsApproach Gerardo F. Torres del Castillo Instituto de Ciencias Universidad Autónoma de Puebla Ciudad Universitaria 72570 Puebla, Puebla, Mexico [email protected] ISBN 978-0-8176-8270-5 e-ISBN 978-0-8176-8271-2 DOI 10.1007/978-0-8176-8271-2 Springer New York Dordrecht Heidelberg London Library of Congress Control Number: 2011939950 Mathematics Subject Classification (2010): 22E70, 34C14, 53B20, 58A15, 70H05 © Springer Science+Business Media, LLC 2012 All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer Science+Business Media, LLC, 233 Spring Street, New York, NY 10013, USA), except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks, and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed on acid-free paper Springer is part of Springer Science+Business Media (www.birkhauser-science.com) Preface The aim of this book is to present in an elementary manner the basic notions related with differentiable manifolds and some of their applications, especially in physics. The book is aimed at advanced undergraduate and graduate students in physics and mathematics, assuming a working knowledge of calculus in several variables, linear algebra, and differential equations. -
Differential Geometry: Curvature and Holonomy Austin Christian
University of Texas at Tyler Scholar Works at UT Tyler Math Theses Math Spring 5-5-2015 Differential Geometry: Curvature and Holonomy Austin Christian Follow this and additional works at: https://scholarworks.uttyler.edu/math_grad Part of the Mathematics Commons Recommended Citation Christian, Austin, "Differential Geometry: Curvature and Holonomy" (2015). Math Theses. Paper 5. http://hdl.handle.net/10950/266 This Thesis is brought to you for free and open access by the Math at Scholar Works at UT Tyler. It has been accepted for inclusion in Math Theses by an authorized administrator of Scholar Works at UT Tyler. For more information, please contact [email protected]. DIFFERENTIAL GEOMETRY: CURVATURE AND HOLONOMY by AUSTIN CHRISTIAN A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science Department of Mathematics David Milan, Ph.D., Committee Chair College of Arts and Sciences The University of Texas at Tyler May 2015 c Copyright by Austin Christian 2015 All rights reserved Acknowledgments There are a number of people that have contributed to this project, whether or not they were aware of their contribution. For taking me on as a student and learning differential geometry with me, I am deeply indebted to my advisor, David Milan. Without himself being a geometer, he has helped me to develop an invaluable intuition for the field, and the freedom he has afforded me to study things that I find interesting has given me ample room to grow. For introducing me to differential geometry in the first place, I owe a great deal of thanks to my undergraduate advisor, Robert Huff; our many fruitful conversations, mathematical and otherwise, con- tinue to affect my approach to mathematics. -
DISCRETE DIFFERENTIAL GEOMETRY: an APPLIED INTRODUCTION Keenan Crane • CMU 15-458/858 LECTURE 10: INTRODUCTION to CURVES
DISCRETE DIFFERENTIAL GEOMETRY: AN APPLIED INTRODUCTION Keenan Crane • CMU 15-458/858 LECTURE 10: INTRODUCTION TO CURVES DISCRETE DIFFERENTIAL GEOMETRY: AN APPLIED INTRODUCTION Keenan Crane • CMU 15-458/858 Curves & Surfaces •Much of the geometry we encounter in life well-described by curves and surfaces* (Curves) *Or solids… but the boundary of a solid is a surface! (Surfaces) Much Ado About Manifolds • In general, differential geometry studies n-dimensional manifolds; we’ll focus on low dimensions: curves (n=1), surfaces (n=2), and volumes (n=3) • Why? Geometry we encounter in everyday life/applications • Low-dimensional manifolds are not “baby stuff!” • n=1: unknot recognition (open as of 2021) • n=2: Willmore conjecture (2012 for genus 1) • n=3: Geometrization conjecture (2003, $1 million) • Serious intuition gained by studying low-dimensional manifolds • Conversely, problems involving very high-dimensional manifolds (e.g., data analysis/machine learning) involve less “deep” geometry than you might imagine! • fiber bundles, Lie groups, curvature flows, spinors, symplectic structure, ... • Moreover, curves and surfaces are beautiful! (And in some cases, high- dimensional manifolds have less interesting structure…) Smooth Descriptions of Curves & Surfaces •Many ways to express the geometry of a curve or surface: •height function over tangent plane •local parameterization •Christoffel symbols — coordinates/indices •differential forms — “coordinate free” •moving frames — change in adapted frame •Riemann surfaces (local); Quaternionic functions -
The Ricci Curvature of Rotationally Symmetric Metrics
The Ricci curvature of rotationally symmetric metrics Anna Kervison Supervisor: Dr Artem Pulemotov The University of Queensland 1 1 Introduction Riemannian geometry is a branch of differential non-Euclidean geometry developed by Bernhard Riemann, used to describe curved space. In Riemannian geometry, a manifold is a topological space that locally resembles Euclidean space. This means that at any point on the manifold, there exists a neighbourhood around that point that appears ‘flat’and could be mapped into the Euclidean plane. For example, circles are one-dimensional manifolds but a figure eight is not as it cannot be pro- jected into the Euclidean plane at the intersection. Surfaces such as the sphere and the torus are examples of two-dimensional manifolds. The shape of a manifold is defined by the Riemannian metric, which is a measure of the length of tangent vectors and curves in the manifold. It can be thought of as locally a matrix valued function. The Ricci curvature is one of the most sig- nificant geometric characteristics of a Riemannian metric. It provides a measure of the curvature of the manifold in much the same way the second derivative of a single valued function provides a measure of the curvature of a graph. Determining the Ricci curvature of a metric is difficult, as it is computed from a lengthy ex- pression involving the derivatives of components of the metric up to order two. In fact, without additional simplifications, the formula for the Ricci curvature given by this definition is essentially unmanageable. Rn is one of the simplest examples of a manifold. -
INTRODUCTION to MANIFOLDS Contents 1. Differentiable Curves 1
INTRODUCTION TO MANIFOLDS TSOGTGEREL GANTUMUR Abstract. We discuss manifolds embedded in Rn and the implicit function theorem. Contents 1. Differentiable curves 1 2. Manifolds 3 3. The implicit function theorem 6 4. The preimage theorem 10 5. Tangent spaces 12 1. Differentiable curves Intuitively, a differentiable curves is a curve with the property that the tangent line at each of its points can be defined. To motivate our definition, let us look at some examples. Example 1.1. (a) Consider the function γ : (0; π) ! R2 defined by ( ) cos t γ(t) = : (1) sin t As t varies in the interval (0; π), the point γ(t) traces out the curve C = [γ] ≡ fγ(t): t 2 (0; π)g ⊂ R2; (2) which is a semicircle (without its endpoints). We call γ a parameterization of C. If γ(t) represents the coordinates of a particle in the plane at time t, then the \instantaneous velocity vector" of the particle at the time moment t is given by ( ) 0 − sin t γ (t) = : (3) cos t Obviously, γ0(t) =6 0 for all t 2 (0; π), and γ is smooth (i.e., infinitely often differentiable). The direction of the velocity vector γ0(t) defines the direction of the line tangent to C at the point p = γ(t). (b) Under the substitution t = s2, we obtain a different parameterization of C, given by ( ) cos s2 η(s) ≡ γ(s2) = : (4) sin s2 p Note that the parameter s must take values in (0; π). (c) Now consider the function ξ : [0; π] ! R2 defined by ( ) cos t ξ(t) = : (5) sin t Date: 2016/11/12 10:49 (EDT). -
Symbols 1-Form, 10 4-Acceleration, 184 4-Force, 115 4-Momentum, 116
Index Symbols B 1-form, 10 Betti number, 589 4-acceleration, 184 Bianchi type-I models, 448 4-force, 115 Bianchi’s differential identities, 60 4-momentum, 116 complex valued, 532–533 total, 122 consequences of in Newman-Penrose 4-velocity, 114 formalism, 549–551 first contracted, 63 second contracted, 63 A bicharacteristic curves, 620 acceleration big crunch, 441 4-acceleration, 184 big-bang cosmological model, 438, 449 Newtonian, 74 Birkhoff’s theorem, 271 action function or functional bivector space, 486 (see also Lagrangian), 594, 598 black hole, 364–433 ADM action, 606 Bondi-Metzner-Sachs group, 240 affine parameter, 77, 79 boost, 110 alternating operation, antisymmetriza- Born-Infeld (or tachyonic) scalar field, tion, 27 467–471 angle field, 44 Boyer-Lindquist coordinate chart, 334, anisotropic fluid, 218–220, 276 399 collapse, 424–431 Brinkman-Robinson-Trautman met- ric, 514 anti-de Sitter space-time, 195, 644, Buchdahl inequality, 262 663–664 bugle, 69 anti-self-dual, 671 antisymmetric oriented tensor, 49 C antisymmetric tensor, 28 canonical energy-momentum-stress ten- antisymmetrization, 27 sor, 119 arc length parameter, 81 canonical or normal forms, 510 arc separation function, 85 Cartesian chart, 44, 68 arc separation parameter, 77 Casimir effect, 638 Arnowitt-Deser-Misner action integral, Cauchy horizon, 403, 416 606 Cauchy problem, 207 atlas, 3 Cauchy-Kowalewski theorem, 207 complete, 3 causal cone, 108 maximal, 3 causal space-time, 663 698 Index 699 causality violation, 663 contravariant index, 51 characteristic hypersurface, 623 contravariant -
Parsing Images Into Regions, Curves, and Curve Groups
Submitted to Int’l J. of Computer Vision, October 2003. First Review March 2005. Revised June 2005. Parsing Images into Regions, Curves, and Curve Groups Zhuowen Tu1 and Song-Chun Zhu2 Lab of Neuro Imaging, Department of Neurology1, Departments of Statistics and Computer Science2, University of California, Los Angeles, Los Angeles, CA 90095. emails: {ztu,sczhu}@stat.ucla.edu Abstract In this paper, we present an algorithm for parsing natural images into middle level vision representations – regions, curves, and curve groups (parallel curves and trees). This al- gorithm is targeted for an integrated solution to image segmentation and curve grouping through Bayesian inference. The paper makes the following contributions. (1) It adopts a layered (or 2.1D-sketch) representation integrating both region and curve models which compete to explain an input image. The curve layer occludes the region layer and curves observe a partial order occlusion relation. (2) A Markov chain search scheme Metropolized Gibbs Samplers (MGS) is studied. It consists of several pairs of reversible jumps to tra- verse the complex solution space. An MGS proposes the next state within the jump scope of the current state according to a conditional probability like a Gibbs sampler and then accepts the proposal with a Metropolis-Hastings step. This paper discusses systematic de- sign strategies of devising reversible jumps for a complex inference task. (3) The proposal probability ratios in jumps are factorized into ratios of discriminative probabilities. The latter are computed in a bottom-up process, and they drive the Markov chain dynamics in a data-driven Markov chain Monte Carlo framework. -
Geometry of Curves and Surfaces Notes C J M Speight 2011
Geometry of Curves and Surfaces Notes c J M Speight 2011 Contact Details Lecturer: Dr. Lamia Alqahtani E-mail [email protected] This note was made by Prof. Martin Speight, School of Mathematics, The University of Leeds, E-mail: [email protected] 0 Why study geometry? Curves and surfaces are all around us in the natural world, and in the built environ- ment. The first step in understanding these structures is to find a mathematically natural way to describe them. That is the primary aim of this course, which will focus particularly on the concept of curvature. As a side effect, you will develop some very useful transferable skills. Key among these is the ability to translate a mathematical system (a set of equations, or formulae, or inequalities) into a visual picture. Your geometric intuition about the picture can then give you useful insight into the original mathematical system. This trick of visualizing mathematical systems can be very powerful and is, unfortunately, not strongly emphasized in the teaching of maths. Example 0 How does the number of solutions of the pair of simultaneous equations xy = 1 x2 + y2 = a2 depend on the constant a > 0? 0 x2 So for a < a0 (in fact, a0 = √2), the system has 0 solutions, for a = a0 it has 2 and for a > a0 it has 4. One could easily verify this by solving the equations explicitly, but the point is that visualizing x the system gave us a very quick (in fact, 1 almost instantaneous) short cut. The above example featured a pair of curves, each associated with an algebraic equation. -
On Geodesic Behavior of Some Special Curves
S S symmetry Article On Geodesic Behavior of Some Special Curves Savin Trean¸t˘a Department of Applied Mathematics, University Politehnica of Bucharest, 060042 Bucharest, Romania; [email protected] Received: 2 March 2020; Accepted: 17 March 2020; Published: 1 April 2020 Abstract: In this paper, geometric structures on an open subset D ⊆ R2 are investigated such that the graphs associated with the solutions of some special functions to become geodesics. More precisely, we determine the Riemannian metric g such that Bessel (Hermite, harmonic oscillator, Legendre and Chebyshev) ordinary differential equation (ODE) is identified with the geodesic ODEs produced by the Riemannian metric g. The technique is based on the Lagrangian (the energy of the curve) 1 L = k x˙(t) k2, the associated Euler–Lagrange ODEs and their identification with the considered 2 special ODEs. Keywords: auto-parallel curve; geodesic; Euler–Lagrange equations; Lagrangian; special functions MSC: 34A26; 53B15; 53C22 1. Introduction and Preliminaries The concept of connection plays an important role in geometry and, depending on what sort of data one wants to transport along some trajectories, a variety of kinds of connections have been introduced in modern geometry. Crampin et al. [1], in a certain vector bundle, described the construction of a linear connection associated with a second-order differential equation field and, moreover, the corresponding curvature was computed. Ermakov [2] established that linear second-order equations with variable coefficients can be completely integrated only in very rare cases. Further, some aspects of time-dependent second-order differential equations and Berwald-type connections have been studied, with remarkable results, by Sarlet and Mestdag [3]. -
DIFFERENTIAL GEOMETRY of CURVES and SURFACES 7. Geodesics and the Theorem of Gauss-Bonnet 7.1
DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 7. Geodesics and the Theorem of Gauss-Bonnet 7.1. Geodesics on a Surface. The goal of this section is to give an answer to the following question. Question. What kind of curves on a given surface should be the analogues of straight lines in the plane? Let’s understand first what means “straight” line in the plane. If you want to go from a point in a plane “straight” to another one, your trajectory will be such a line. In other words, a straight line has the property that if we fix two points P and Q on it, then the piece of between P Land Q is the shortest curve in the plane which joins the two points. Now, if insteadL of a plane (“flat” surface) you need to go from P to Q in a land with hills and valleys (arbitrary surface), which path will you take? This is how the notion of geodesic line arises: “Definition” 7.1.1. Let S be a surface. A curve α : I S parametrized by arc length → is called a geodesic if for any two points P = α(s1), Q = α(s2) on the curve which are sufficiently close to each other, the piece of the trace of α between P and Q is the shortest of all curves in S which join P and Q. There are at least two inconvenients concerning this definition: first, why did we say that P and Q are “sufficiently close to each other”?; second, this definition will certainly not allow us to do any explicit examples (for instance, find the geodesics on a hyperbolic paraboloid).