SINGULARITIES PROCEEDINGS of SYMPOSIA in PURE MATHEMATICS Volume 40, Part 2

Total Page:16

File Type:pdf, Size:1020Kb

SINGULARITIES PROCEEDINGS of SYMPOSIA in PURE MATHEMATICS Volume 40, Part 2 http://dx.doi.org/10.1090/pspum/040.2 SINGULARITIES PROCEEDINGS OF SYMPOSIA IN PURE MATHEMATICS Volume 40, Part 2 SINGULARITIES AMERICAN MATHEMATICAL SOCIETY PROVIDENCE, RHODE ISLAND PROCEEDINGS OF SYMPOSIA IN PURE MATHEMATICS OF THE AMERICAN MATHEMATICAL SOCIETY VOLUME 40 PROCEEDINGS OF THE SUMMER INSTITUTE ON SINGULARITIES HELD AT HUMBOLDT STATE UNIVERSITY ARCATA, CALIFORNIA JULY 20-AUGUST 7, 1981 EDITED BY PETER ORLIK Prepared by the American Mathematical Society with partial support from National Science Foundation grant MCS 80-20208 1980 Mathematics Subject Classification. Primary 14-XX, 16-XX, 32-XX, 53-XX, 55-XX, 57-XX, 58-XX. Library of Congress Cataloging in Publication Data Main entry under title: Singularities. (Proceedings of symposia in pure mathematics; v. 40, pts. 1, 2) Bibliography: p. 1. Singularities (Mathematics)-Addresses, essays, lectures. I. Orlik, Peter, 1938- . II. Series. QA614.58.S55 1983 514'.74 83-2529 ISBN 0-8218-1443-5 (set) ISBN 0^8218-14664 (part 2) ISBN 03218-1450-8 (part 1) ISSN 0082-0717 COPYING AND REPRINTING. Individual readers of this publication, and nonprofit libraries acting for them are permitted to make fair use of the material, such as to copy an article for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews provided the customary acknowledgement of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication (including abstracts) is permitted only under Ucense from the American Mathematical Society. Requests for such permission should be addressed to the Executive Director, American Mathematical Society, Box 6248, Providence, Rhode Island 02940. The appearance of the code on the first page of an article in this journal indicates the copyright owner's consent for copying beyond that permitted by Sections 107 or 108 of the U. S. Copyright Law, provided that the copier pay the stated per copy fee through the Copyright Clearance Center, Inc., 21 Congress Street, Salem, Massachusetts 01970. This consent does not extend to other kinds of copying, such as copying for general distribution, for advertising or promotional purposes, for creating new collective works, or for resale. Copyright © 1983 by the American Mathematical Society. Printed in the United States of America. All rights reserved except those granted to the United States Government. TABLE OF CONTENTS PART 1 Preface xx List of participants Desingularization of plane curves 1 SHREERAM S. ABHYANKAR Zeros of holomorphic vector fields 47 and the Gysin homomorphism E. AKYILDIZ AND J. B. CARRELL On the graded rings associated to 55 holomorphic vector fields with exactly one zero E. AKYILDIZ, J. B. CARRELL, D. I. LIEBERMAN AND A. J. SOMMESE Some open problems in the theory 57 of singularities V. I. ARNOLD Complex surfaces of small homotopy 71 type GOTTFRIED BARTHEL Homeomorphy classification of normal 81 surfaces in P3 with C*-action GOTTFRIED BARTHEL Minimal free resolutions of Gorenstein 105 local rings with small multiplicity KURT BEHNKE Analytic equivalence of isolated hyper- Ill surface singularities defined by homo• geneous polynomials MAX BENSON v VI TABLE OF CONTENTS An application of singularity theory to 119 nonlinear elliptic partial differential equations M. S. BERGER, P. T. CHURCH AND J. G. TIMOURIAN Algebras of composite differentiable 127 functions EDWARD BIERSTONE AND PIERRE D. MILMAN The extension problem and related 137 themes in differential analysis EDWARD BIERSTONE AND GERALD W. SCHWARZ On global extensions of Dynkin diagrams 145 and singular surfaces of the topological type of P2 LAWRENCE BRENTON, DAVID BINDSCHADLER, DANIEL DRUCKER AND GEERT C. E. PRINS Milnor lattices and Dynkin diagrams 153 E. BRIESKORN On the topology of polynomial hyper- 167 surfaces S. A. BROUGHTON Genericity of caustics by reflexion 179 J. W. BRUCE, P. J. GIBLIN AND C. G. GIBSON Envelopes, duality and contact structures 195 J. W. BRUCE Bifurcation involving the hexagonal 203 lattice ERNESTO BUZANO AND MARTIN GOLUBITSKY On saturations of curve singularities 211 (any characteristic) ANTONIO CAMPILLO A note on the classes [£,*(/)] 221 DANIEL S. CHESS Differential maps with small 225 critical set P. T. CHURCH The unfolding and determinacy theorems 233 for subgroups of & and % JAMES DAMON TABLE OF CONTENTS Vll Topological triviality in versal unfoldings 255 JAMES DAMON Newton titrations, monomial algebras 267 and nonisolated and equivariant singu• larities JAMES DAMON Contact germs from the plane to the plane 277 A. DIMCA AND C. G. GIBSON Weyl groups and Cremona transformations 283 IGOR V. DOLGACHEV Genericity and smooth finite determinacy 295 ANDREW DU PLESSIS A naive guide to mixed Hodge theory 313 ALAN H. DURFEE The low-dimensional topology of 321 singularities ALAN H. DURFEE On the monodromy groups of singularities 327 WOLFGANG EBELING Rational curves with cusps 337 DAVID EISENBUD Mixed Hodge structures 345 FOUAD ELZEIN Special polars and curves with one 353 place at infinity ROBERT EPHRAIM Another view of critical point theory 361 ISTVAN FARY Some results on Poincare duality 373 ISTVAN FARY Some essential valuations in the resolution 381 of singularities JONATHAN FINE Derivations and smooth discriminant 385 KLAUS FISCHER Vlll TABLE OF CONTENTS Singularities of period maps and the 391 weak global Torelli problem ROBERT FRIEDMAN AND ROY SMITH The Thorn polynomial of 2TTTT 399 TERENCE GAFFNEY The structure of T&(f), classification 409 and an application to differential geometry TERENCE GAFFNEY Multiple points and associated ramification 429 loci TERENCE GAFFNEY Equivalence theorems in global singularity theory 439 TERENCE GAFFNEY AND LESLIE WILSON Hilbert scheme as flattener 449 A. GALLIGO Differential invariance of multiplicity 453 YIH-NAN GAU AND JOSEPH LIPMAN Classification des singularites isolees 457 simples d'intersections completes MARC GIUSTI Finding the nondegenerate quadratic 495 singularities NORMAN GOLDSTEIN A discussion of symmetry and symmetry 499 breaking MARTIN GOLUBITSKY AND DAVID SCHAEFFER Stratified Morse theory 517 MARK GORESKY AND ROBERT MACPHERSON On the topology of smoothable singularities 535 GERT-MARTIN GREUEL AND JOSEPH STEENBRINK Lefschetz theorems for singular varieties 547 HELMUT A. HAMM Stratification via corank one projections 559 ROBERT M. HARDT An algorithm of construction of the 567 semiuniversal deformation of an isolated singularity HERWIG HAUSER TABLE OF CONTENTS IX Limites de normales, conditions de 575 Whitney et eclatement d'Hironaka J. P. G. HENRY ET M. MERLE Computation of some projective invariants 585 AUDUN HOLME Deforming complete intersection Artin 593 algebras. Appendix: Hilbert function of C[.x, y]/I ANTHONY IARROBINO Duality for Riemannian foliations 609 FRANZ W. KAMBER AND PHILIPPE TONDEUR Normally flat deformations of rational 619 and minimally elliptic singularities ULRICH KARRAS The topology of real algebraic sets 641 H. KING Differential forms and the fundamental 655 group of the complement of hypersurfaces TOSHITAKE KOHNO Questions about the proof of the hard 663 Lefschetz theorem KLAUS LAMOTKE Metric study of the neighbourhood of a 669 singularity REMI LANGEVIN TABLE OF CONTENTS PART 2 Weak simultaneous resolution for deforma- 1 tions of Gorenstein surface singularities HENRY B. LAUFER Introduction to linear differential systems 31 LE DUNG TRANG AND ZOGHMAN MEBKHOUT Cycles evanescents, sections planes et 65 conditions de Whitney. II LE D. T. ET B. TEISSIER Report on the problem session 105 LE D. T. AND B. TEISSIER Extended Artingroups 117 HARM VAN DER LEK Differentiable structures on complete 123 intersections. II ANATOLY S. LIBGOBER AND JOHN W. WOOD Alexander invariants of plane algebraic 135 curves A. LIBGOBER A connection between polar invariants and 145 roots of the Bernstein-Sato polynomial BEN LICHTIN Estimates and formulae 155 for the C° degree of sufficiency of plane curves BEN LICHTIN Quasi-ordinary singularities of 161 surfaces in C3 JOSEPH LIPMAN XI xu TABLE OF CONTENTS The smoothing components of a triangle 173 singularity. I EDUARD LOOIJENGA On the structure of embedded algebroid 185 surfaces IGNACIO LUENGO Some new surfaces of general type 193 RICHARD MANDELBAUM Distance from a submanifold in 199 Euclidean space JOHN N. MATHER On the topology of Deligne's weight 217 filtration CLINT McCRORY Topological types of 227 polynomial map germs ISAO NAKAI Abelian covers of quasihomogeneous 233 surface singularities WALTER D. NEUMANN Geometry of quasihomogeneous surfaces 245 singularities WALTER D. NEUMANN On the stability of the Newton boundary 259 MATSUO OKA Coxeter arrangements 269 PETER ORLIK AND LOUIS SOLOMON Vanishing folds in families of singularities 293 DONAL B. O'SHEA Projective resolutions of Hodge algebras: Some examples 305 JURGEN PESSELHOY AND OSWALD RIEMENSCHNEIDER Vanishing homologies and the n variable 319 saddlepoint method FREDERIC PHAM A note on higher order dual varieties, 335 with an application to scrolls RAGNI PIENE TABLE OF CONTENTS Xlll Factorization of birational maps in 343 dimension 3 HENRY C. PINKHAM Smoothings of the Dpqr singularities, 373 p + q + r = 22 HENRY C. PINKHAM The normal singularities of surfaces in R3 379 IAN R. PORTEOUS Probing singularities 395 IAN. R. PORTEOUS C*-equivariant deformations of germs of 407 coherent sheaves FERNANDO PUERTA The real Jacobian problem 411 JOHN D. RANDALL Milnor fibers and Alexander polynomials 415 of plane curves RICHARD RANDELL Multiple points of real mappings 421 FELICE RONGA A new look at
Recommended publications
  • Ian R. Porteous 9 October 1930 - 30 January 2011
    In Memoriam Ian R. Porteous 9 October 1930 - 30 January 2011 A tribute by Peter Giblin (University of Liverpool) Będlewo, Poland 16 May 2011 Caustics 1998 Bill Bruce, disguised as a Terry Wall, ever a Pro-Vice-Chancellor mathematician Watch out for Bruce@60, Wall@75, Liverpool, June 2012 with Christopher Longuet-Higgins at the Rank Prize Funds symposium on computer vision in Liverpool, summer 1987, jointly organized by Ian, Joachim Rieger and myself After a first degree at Edinburgh and National Service, Ian worked at Trinity College, Cambridge, for a BA then a PhD under first William Hodge, but he was about to become Secretary of the Royal Society and Master of Pembroke College Cambridge so when Michael Atiyah returned from Princeton in January 1957 he took on Ian and also Rolph Schwarzenberger (6 years younger than Ian) as PhD students Ian’s PhD was in algebraic geometry, the effect of blowing up on Chern Classes, published in Proceedings of the Cambridge Philosophical Society in 1960: The behaviour of the Chern classes or of the canonical classes of an algebraic variety under a dilatation has been studied by several authors (Todd, Segre, van de Ven). This problem is of interest since a dilatation is the simplest form of birational transformation which does not preserve the underlying topological structure of the algebraic variety. A relation between the Chern classes of the variety obtained by dilatation of a subvariety and the Chern classes of the original variety has been conjectured by the authors cited above but a complete proof of this relation is not in the literature.
    [Show full text]
  • Evolutes of Curves in the Lorentz-Minkowski Plane
    Evolutes of curves in the Lorentz-Minkowski plane 著者 Izumiya Shuichi, Fuster M. C. Romero, Takahashi Masatomo journal or Advanced Studies in Pure Mathematics publication title volume 78 page range 313-330 year 2018-10-04 URL http://hdl.handle.net/10258/00009702 doi: info:doi/10.2969/aspm/07810313 Evolutes of curves in the Lorentz-Minkowski plane S. Izumiya, M. C. Romero Fuster, M. Takahashi Abstract. We can use a moving frame, as in the case of regular plane curves in the Euclidean plane, in order to define the arc-length parameter and the Frenet formula for non-lightlike regular curves in the Lorentz- Minkowski plane. This leads naturally to a well defined evolute asso- ciated to non-lightlike regular curves without inflection points in the Lorentz-Minkowski plane. However, at a lightlike point the curve shifts between a spacelike and a timelike region and the evolute cannot be defined by using this moving frame. In this paper, we introduce an alternative frame, the lightcone frame, that will allow us to associate an evolute to regular curves without inflection points in the Lorentz- Minkowski plane. Moreover, under appropriate conditions, we shall also be able to obtain globally defined evolutes of regular curves with inflection points. We investigate here the geometric properties of the evolute at lightlike points and inflection points. x1. Introduction The evolute of a regular plane curve is a classical subject of differen- tial geometry on Euclidean plane which is defined to be the locus of the centres of the osculating circles of the curve (cf. [3, 7, 8]).
    [Show full text]
  • The Illinois Mathematics Teacher
    THE ILLINOIS MATHEMATICS TEACHER EDITORS Marilyn Hasty and Tammy Voepel Southern Illinois University Edwardsville Edwardsville, IL 62026 REVIEWERS Kris Adams Chip Day Karen Meyer Jean Smith Edna Bazik Lesley Ebel Jackie Murawska Clare Staudacher Susan Beal Dianna Galante Carol Nenne Joe Stickles, Jr. William Beggs Linda Gilmore Jacqueline Palmquist Mary Thomas Carol Benson Linda Hankey James Pelech Bob Urbain Patty Bruzek Pat Herrington Randy Pippen Darlene Whitkanack Dane Camp Alan Holverson Sue Pippen Sue Younker Bill Carroll John Johnson Anne Marie Sherry Mike Carton Robin Levine-Wissing Aurelia Skiba ICTM GOVERNING BOARD 2012 Don Porzio, President Rich Wyllie, Treasurer Fern Tribbey, Past President Natalie Jakucyn, Board Chair Lannette Jennings, Secretary Ann Hanson, Executive Director Directors: Mary Modene, Catherine Moushon, Early Childhood (2009-2012) Com. College/Univ. (2010-2013) Polly Hill, Marshall Lassak, Early Childhood (2011-2014) Com. College/Univ. (2011-2014) Cathy Kaduk, George Reese, 5-8 (2010-2013) Director-At-Large (2009-2012) Anita Reid, Natalie Jakucyn, 5-8 (2011-2014) Director-At-Large (2010-2013) John Benson, Gwen Zimmermann, 9-12 (2009-2012) Director-At-Large (2011-2014) Jerrine Roderique, 9-12 (2010-2013) The Illinois Mathematics Teacher is devoted to teachers of mathematics at ALL levels. The contents of The Illinois Mathematics Teacher may be quoted or reprinted with formal acknowledgement of the source and a letter to the editor that a quote has been used. The activity pages in this issue may be reprinted for classroom use without written permission from The Illinois Mathematics Teacher. (Note: Occasionally copyrighted material is used with permission. Such material is clearly marked and may not be reprinted.) THE ILLINOIS MATHEMATICS TEACHER Volume 61, No.
    [Show full text]
  • Some Remarks on Duality in S3
    GEOMETRY AND TOPOLOGY OF CAUSTICS — CAUSTICS ’98 BANACH CENTER PUBLICATIONS, VOLUME 50 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 1999 SOME REMARKS ON DUALITY IN S 3 IAN R. PORTEOUS Department of Mathematical Sciences University of Liverpool Liverpool, L69 3BX, UK e-mail: [email protected] Abstract. In this paper we review some of the concepts and results of V. I. Arnol0d [1] for curves in S2 and extend them to curves and surfaces in S3. 1. Introduction. In [1] Arnol0d introduces the concepts of the dual curve and the derivative curve of a smooth (= C1) embedded curve in S2. In particular he shows that the evolute or caustic of such a curve is the dual of the derivative. The dual curve is just the unit normal curve, while the derivative is the unit tangent curve. The definitions extend in an obvious way to curves on S2 with ordinary cusps. Then one proves easily that where a curve has an ordinary geodesic inflection the dual has an ordinary cusp and vice versa. Since the derivative of a curve without cusps clearly has no cusps it follows that the caustic of such a curve has no geodesic inflections. This prompts investigating what kind of singularity a curve must have for its caustic to have a geodesic inflection, by analogy with the classical construction of de l'H^opital,see [2], pages 24{26. In the second and third parts of the paper the definitions of Arnol0d are extended to surfaces in S3 and to curves in S3. The notations are those of Porteous [2], differentiation being indicated by subscripts.
    [Show full text]
  • A Convex, Smooth and Invertible Contact Model for Trajectory Optimization
    A convex, smooth and invertible contact model for trajectory optimization Emanuel Todorov Departments of Applied Mathematics and Computer Science and Engineering University of Washington Abstract— Trajectory optimization is done most efficiently There is however one additional requirement which we when an inverse dynamics model is available. Here we develop believe is essential and requires a qualitatively new approach: the first model of contact dynamics definedinboththeforward iv. The contact model should be defined for both forward and and inverse directions. The contact impulse is the solution to a convex optimization problem: minimize kinetic energy inverse dynamics. Here the forward dynamics in contact space subject to non-penetration and friction-cone w = a (q w u ) (1) constraints. We use a custom interior-point method to make the +1 1 optimization problem unconstrained; this is key to defining the compute the next-step velocity w+1 given the current forward and inverse dynamics in a consistent way. The resulting generalized position q , velocity w and applied force u , model has a parameter which sets the amount of contact smoothing, facilitating continuation methods for optimization. while the inverse dynamics We implemented the proposed contact solver in our new physics u = b (q w w ) (2) engine (MuJoCo). A full Newton step of trajectory optimization +1 for a 3D walking gait takes only 160 msec, on a 12-core PC. compute the applied force that caused the observed change in velocity. Computing the total force that caused the observed I. INTRODUCTION change in velocity is of course straightforward. The hard Optimal control theory provides a powerful set of methods part is decomposing this total force into a contact force and for planning and automatic control.
    [Show full text]
  • Mathematics 1
    Mathematics 1 MATHEMATICS Courses MATH 1483 Mathematical Functions and Their Uses (A) Math is the language of science and a vital part of both cutting-edge Prerequisites: An acceptable placement score - see research and daily life. Contemporary mathematics investigates such placement.okstate.edu. basic concepts as space and number and also the formulation and Description: Analysis of functions and their graphs from the viewpoint analysis of mathematical models arising from applications. Mathematics of rates of change. Linear, exponential, logarithmic and other functions. has always had close relationships to the physical sciences and Applications to the natural sciences, agriculture, business and the social engineering. As the biological, social, and management sciences have sciences. become increasingly quantitative, the mathematical sciences have Credit hours: 3 moved in new directions to support these fields. Contact hours: Lecture: 3 Contact: 3 Levels: Undergraduate Mathematicians teach in high schools and colleges, do research and Schedule types: Lecture teach at universities, and apply mathematics in business, industry, Department/School: Mathematics and government. Outside of education, mathematicians usually work General Education and other Course Attributes: Analytical & Quant in research and analytical positions, although they have become Thought increasingly involved in management. Firms in the aerospace, MATH 1493 Applications of Modern Mathematics (A) communications, computer, defense, electronics, energy, finance, and Prerequisites: An acceptable placement score (see insurance industries employ many mathematicians. In such employment, placement.okstate.edu). a mathematician typically serves either in a consulting capacity, giving Description: Introduction to contemporary applications of discrete advice on mathematical problems to engineers and scientists, or as a mathematics. Topics from management science, statistics, coding and member of a research team composed of specialists in several fields.
    [Show full text]
  • Geometric Differentiation: for the Intelligence of Curves and Surfaces: Second Edition I
    Cambridge University Press 978-0-521-81040-1 - Geometric Differentiation: For the intelligence of Curves and Surfaces: Second Edition I. R. Porteous Frontmatter More information Geometric differentiation © in this web service Cambridge University Press www.cambridge.org Cambridge University Press 978-0-521-81040-1 - Geometric Differentiation: For the intelligence of Curves and Surfaces: Second Edition I. R. Porteous Frontmatter More information © in this web service Cambridge University Press www.cambridge.org Cambridge University Press 978-0-521-81040-1 - Geometric Differentiation: For the intelligence of Curves and Surfaces: Second Edition I. R. Porteous Frontmatter More information Geometric differentiation for the intelligence of curves and surfaces Second edition I. R. Porteous Senior Lecturer, Department of Pure Mathematics University of Liverpool © in this web service Cambridge University Press www.cambridge.org Cambridge University Press 978-0-521-81040-1 - Geometric Differentiation: For the intelligence of Curves and Surfaces: Second Edition I. R. Porteous Frontmatter More information University Printing House, Cambridge CB2 8BS, United Kingdom Cambridge University Press is part of the University of Cambridge. It furthers the University’s mission by disseminating knowledge in the pursuit of education, learning and research at the highest international levels of excellence. www.cambridge.org Information on this title: www.cambridge.org/9780521810401 © Cambridge University Press 1994, 2001 This publication is in copyright. Subject
    [Show full text]
  • Differential Geometry from a Singularity Theory Viewpoint
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Biblioteca Digital da Produção Intelectual da Universidade de São Paulo (BDPI/USP) Universidade de São Paulo Biblioteca Digital da Produção Intelectual - BDPI Departamento de Matemática - ICMC/SMA Livros e Capítulos de Livros - ICMC/SMA 2015-12 Differential geometry from a singularity theory viewpoint IZUMIYA, Shyuichi et al. Differential geometry from a singularity theory viewpoint. Hackensack: World Scientific, 2015. 384 p. http://www.producao.usp.br/handle/BDPI/50103 Downloaded from: Biblioteca Digital da Produção Intelectual - BDPI, Universidade de São Paulo by UNIVERSITY OF SAO PAULO on 03/04/16. For personal use only. Differential Geometry from a Singularity Theory Viewpoint Downloaded www.worldscientific.com 9108_9789814590440_tp.indd 1 22/9/15 9:14 am May 2, 2013 14:6 BC: 8831 - Probability and Statistical Theory PST˙ws This page intentionally left blank by UNIVERSITY OF SAO PAULO on 03/04/16. For personal use only. Differential Geometry from a Singularity Theory Viewpoint Downloaded www.worldscientific.com by UNIVERSITY OF SAO PAULO on 03/04/16. For personal use only. Differential Geometry from a Singularity Theory Viewpoint Downloaded www.worldscientific.com 9108_9789814590440_tp.indd 2 22/9/15 9:14 am Published by World Scientific Publishing Co. Pte. Ltd. 5 Toh Tuck Link, Singapore 596224 USA office: 27 Warren Street, Suite 401-402, Hackensack, NJ 07601 UK office: 57 Shelton Street, Covent Garden, London WC2H 9HE Library of Congress Cataloging-in-Publication Data Differential geometry from a singularity theory viewpoint / by Shyuichi Izumiya (Hokkaido University, Japan) [and three others].
    [Show full text]
  • A Brief Introduction to Singularity Theory (A. Remizov, 2010)
    A. O. Remizov A BRIEF INTRODUCTION TO SINGULARITY THEORY Trieste, 2010 1 Lecture 1. Some useful facts from Singularity Theory. Throughout this course all definitions and statements are local, that is, we always operate with ¾sufficiently small¿ neighborhoods of the considered point. In other words, we deal with germs of functioms, maps, vector fields, etc. 1.1 Multiplicity of smooth functions and maps One of the key notions of Singularity Theory is ¾multiplicity¿. Definition 1: Let f(x): R ! R be a smooth (¾smooth¿ means C1) function, and x∗ is its critical point, i.e., f 0(x∗) = 0. Multiplicity of the function f(x) at the critical point x∗ is the order of tangency of the graphs y = f(x) and y = f(x∗) at x∗, i.e., the natural number µ is defined by the condition df dµf dµ+1f (x∗) = 0;:::; (x∗) = 0; (x∗) 6= 0: (1.1) dx dxµ dxµ+1 If such natural number µ does not exist, then we put µ = 1 and the function f(x) − f(x∗) is called ¾1-flat¿ or simply ¾flat¿ at the point x∗. We also put µ = 0 for non-critical points. Critical points with infinite multiplicity can occur, but we will deal only with finite multiplicities. If µ = 1, then the critical point x∗ is called ¾non-degenerated¿. Exercise 1. Prove that any function f with µ < 1 can be simplified to the form f(x) = f(x∗) ± (x − x∗)µ+1 by means of a smooth change of the variable x (the sign ± coincides with the sign of the non-zero derivative in (1.1)).
    [Show full text]
  • In Particular, Line and Sphere Complexes – with Applications to the Theory of Partial Differential Equations
    “Ueber Complexe, insbesondere Linien- und Kugel-complexe, mit Anwendung auf die Theorie partieller Differentialgleichungen,” Math. Ann. 5 (1872), 145-208. On complexes −−− in particular, line and sphere complexes – with applications to the theory of partial differential equations By Sophus Lie in CHRISTIANIA Translated by D. H. Delphenich _______ I. The rapid development of geometry in our century is, as is well-known, intimately linked with philosophical arguments about the essence of Cartesian geometry, arguments that were set down in their most general form by Plücker in his early papers. For anyone who proceeds in the spirit of Plücker’s work, the thought that one can employ every curve that depends on three parameters as a space element will convey nothing that is essentially new, so if no one, as far as I know, has pursued this idea then I believe that the reason for this is that no one has ascribed any practical utility to that fact. I was led to study the aforementioned theory when I discovered a remarkable transformation that represented a precise connection between lines of curvature and principal tangent curves, and it is my intention to summarize the results that I obtained in this way in the following treatise. In the first section, I concern myself with curve complexes – that is, manifolds that are composed of a three-fold infinitude of curves. All surfaces that are composed of a single infinitude of curves from a given complex satisfy a partial differential equation of second order that admits a partial differential equation of first order as its singular first integral.
    [Show full text]
  • Frictional Contact on Smooth Elastic Solids
    Frictional Contact on Smooth Elastic Solids EGOR LARIONOV, University of British Columbia, Canada YE FAN, Vital Mechanics, Canada DINESH K. PAI, University of British Columbia and Vital Mechanics Research, Canada Fig. 1. A rigid whiskey glass is pinched between the index finger and thumb of an animated hand model and lifted up. The first frame shows the internal geometry of the distal phalanges whose vertices drive the finger tips of the tetrahedral simulation mesh of the hand. The remaining hand bones and tendons (not shown) are used to determine other interior animated vertices. The following frames show a selection of frames from the resulting simulation showing the grasp, lift and hold of the glass. The last image shows a photo of a similar scenario for reference. The collision surface of the hand is represented byanimplicit function approximating a smoothed distance potential, while the glass surface is sampled using discrete points. Our method produces realistic deformation at the point of contact between the fingers and the rigid object. Frictional contact between deformable elastic objects remains a difficult ACM Reference Format: simulation problem in computer graphics. Traditionally, contact has been Egor Larionov, Ye Fan, and Dinesh K. Pai. 2021. Frictional Contact on Smooth resolved using sophisticated collision detection schemes and methods that Elastic Solids. ACM Trans. Graph. 40, 2, Article 15 (April 2021), 17 pages. build on the assumption that contact happens between polygons. While https://doi.org/10.1145/3446663 polygonal surfaces are an efficient representation for solids, they lack some intrinsic properties that are important for contact resolution. Generally, polygonal surfaces are not equipped with an intrinsic inside and outside 1 INTRODUCTION partitioning or a smooth distance field close to the surface.
    [Show full text]
  • Contact Singularities in Nonstandard Slow-Fast Dynamical Systems
    Contact singularities in nonstandard slow-fast dynamical systems Ian Lizarraga, Robby Marangell, and Martin Wechselberger School of Mathematics and Statistics, University of Sydney, Camperdown 2006, Australia Abstract We develop the contact singularity theory for singularly-perturbed (or ‘slow-fast’) vector fields of the general form z′ = H(z, ε), z Rn and ε 1. Our main result ∈ ≪ is the derivation of computable, coordinate-independent defining equations for contact singularities under an assumption that the leading-order term of the vector field admits a suitable factorization. This factorization can in turn be computed explicitly in a wide variety of applications. We demonstrate these computable criteria by locating contact folds and, for the first time, contact cusps in some nonstandard models of biochemical oscillators. 1 Introduction Classifying the loss of normal hyperbolicity of the critical manifold is a fundamental step in the analysis of slow-fast dynamical systems. For systems in the so-called standard form1 x′ = εg(x,y,ε) y′ = f(x,y,ε), (1) the k-dimensional critical manifold lies inside the zero set of a smooth mapping f(x, y, 0) : Rn Rn−k. Loss of normal hyperbolicity occurs along points where the critical manifold becomes→ tangent to the layer problem of (1), formally defined by the ε 0 limit: → x′ = 0 y′ = f(x, y, 0). (2) In the planar case x, y R, the solutions of the layer flow consist of trajectories lying within vertical lines x = c (also∈ known as fast fibers). In general, solutions of the layer flow lie in arXiv:2004.01825v1 [math.DS] 4 Apr 2020 hyperplanes orthogonal to the coordinate axes of the slow variable x Rk.
    [Show full text]