RETURN of the PLANE EVOLUTE 1. Short Historical Account As We
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Bézout's Theorem
Bézout's theorem Toni Annala Contents 1 Introduction 2 2 Bézout's theorem 4 2.1 Ane plane curves . .4 2.2 Projective plane curves . .6 2.3 An elementary proof for the upper bound . 10 2.4 Intersection numbers . 12 2.5 Proof of Bézout's theorem . 16 3 Intersections in Pn 20 3.1 The Hilbert series and the Hilbert polynomial . 20 3.2 A brief overview of the modern theory . 24 3.3 Intersections of hypersurfaces in Pn ...................... 26 3.4 Intersections of subvarieties in Pn ....................... 32 3.5 Serre's Tor-formula . 36 4 Appendix 42 4.1 Homogeneous Noether normalization . 42 4.2 Primes associated to a graded module . 43 1 Chapter 1 Introduction The topic of this thesis is Bézout's theorem. The classical version considers the number of points in the intersection of two algebraic plane curves. It states that if we have two algebraic plane curves, dened over an algebraically closed eld and cut out by multi- variate polynomials of degrees n and m, then the number of points where these curves intersect is exactly nm if we count multiple intersections and intersections at innity. In Chapter 2 we dene the necessary terminology to state this theorem rigorously, give an elementary proof for the upper bound using resultants, and later prove the full Bézout's theorem. A very modest background should suce for understanding this chapter, for example the course Algebra II given at the University of Helsinki should cover most, if not all, of the prerequisites. In Chapter 3, we generalize Bézout's theorem to higher dimensional projective spaces. -
Chapter 1 Geometry of Plane Curves
Chapter 1 Geometry of Plane Curves Definition 1 A (parametrized) curve in Rn is a piece-wise differentiable func- tion α :(a, b) Rn. If I is any other subset of R, α : I Rn is a curve provided that α→extends to a piece-wise differentiable function→ on some open interval (a, b) I. The trace of a curve α is the set of points α ((a, b)) Rn. ⊃ ⊂ AsubsetS Rn is parametrized by α if and only if there exists set I R ⊂ ⊆ such that α : I Rn is a curve for which α (I)=S. A one-to-one parame- trization α assigns→ and orientation toacurveC thought of as the direction of increasing parameter, i.e., if s<t,the direction of increasing parameter runs from α (s) to α (t) . AsubsetS Rn may be parametrized in many ways. ⊂ Example 2 Consider the circle C : x2 + y2 =1and let ω>0. The curve 2π α : 0, R2 given by ω → ¡ ¤ α(t)=(cosωt, sin ωt) . is a parametrization of C for each choice of ω R. Recall that the velocity and acceleration are respectively given by ∈ α0 (t)=( ω sin ωt, ω cos ωt) − and α00 (t)= ω2 cos 2πωt, ω2 sin 2πωt = ω2α(t). − − − The speed is given by ¡ ¢ 2 2 v(t)= α0(t) = ( ω sin ωt) +(ω cos ωt) = ω. (1.1) k k − q 1 2 CHAPTER 1. GEOMETRY OF PLANE CURVES The various parametrizations obtained by varying ω change the velocity, ac- 2π celeration and speed but have the same trace, i.e., α 0, ω = C for each ω. -
The Geometry of Resonance Tongues: a Singularity Theory Approach
INSTITUTE OF PHYSICS PUBLISHING NONLINEARITY Nonlinearity 16 (2003) 1511–1538 PII: S0951-7715(03)55769-3 The geometry of resonance tongues: a singularity theory approach Henk W Broer1, Martin Golubitsky2 and Gert Vegter3 1 Department of Mathematics, University of Groningen, PO Box 800, 9700 AV Groningen, The Netherlands 2 Department of Mathematics, University of Houston, Houston, TX 77204-3476, USA 3 Department of Computing Science, University of Groningen, PO Box 800, 9700 AV Groningen, The Netherlands Received 7 November 2002, in final form 20 May 2003 Published 6 June 2003 Online at stacks.iop.org/Non/16/1511 Recommended by A Chenciner Abstract Resonance tongues and their boundaries are studied for nondegenerate and (certain) degenerate Hopf bifurcations of maps using singularity theory methods of equivariant contact equivalence and universal unfoldings. We recover the standard theory of tongues (the nondegenerate case) in a straightforward way and we find certain surprises in the tongue boundary structure when degeneracies are present. For example, the tongue boundaries at degenerate singularities in weak resonance are much blunter than expected from the nondegenerate theory. Also at a semi-global level we find ‘pockets’ or ‘flames’ that can be understood in terms of the swallowtail catastrophe. Mathematics Subject Classification: 37G15, 37G40, 34C25 1. Introduction This paper focuses on resonance tongues obtained by Hopf bifurcation from a fixed point of a map. More precisely, Hopf bifurcations of maps occur at parameter values where the Jacobian of the map has a critical eigenvalue that is a root of unity e2πpi/q , where p and q are coprime integers with q 3 and |p| <q.Resonance tongues themselves are regions in parameter space near the point of Hopf bifurcation where periodic points of period q exist and tongue boundaries consist of critical points in parameter space where the q-periodic points disappear, typically in a saddle-node bifurcation. -
The Witten Equation, Mirror Symmetry, and Quantum Singularity Theory
Annals of Mathematics 178 (2013), 1{106 http://dx.doi.org/10.4007/annals.2013.178.1.1 The Witten equation, mirror symmetry, and quantum singularity theory By Huijun Fan, Tyler Jarvis, and Yongbin Ruan Abstract For any nondegenerate, quasi-homogeneous hypersurface singularity, we describe a family of moduli spaces, a virtual cycle, and a corresponding cohomological field theory associated to the singularity. This theory is analogous to Gromov-Witten theory and generalizes the theory of r-spin curves, which corresponds to the simple singularity Ar−1. We also resolve two outstanding conjectures of Witten. The first con- jecture is that ADE-singularities are self-dual, and the second conjecture is that the total potential functions of ADE-singularities satisfy correspond- ing ADE-integrable hierarchies. Other cases of integrable hierarchies are also discussed. Contents 1. Introduction2 1.1. Organization of the paper9 1.2. Acknowledgments9 2. W -curves and their moduli 10 2.1. W -structures on orbicurves 10 2.2. Moduli of stable W -orbicurves 20 2.3. Admissible groups G and W g;k;G 30 2.4. The tautological ring of W g;k 32 3. The state space associated to a singularity 35 3.1. Lefschetz thimble 35 3.2. Orbifolding and state space 37 H. F. was partially Supported by NSFC 10401001, NSFC 10321001, and NSFC 10631050. T. J. was partially supported by National Science Foundation grants DMS-0605155 and DMS-0105788 and the Institut Mittag-Leffler (Djursholm, Sweden). Y. R. was partially supported by the National Science Foundation and the Yangtze Center of Mathematics at Sichuan University. -
Vanishing Cycles, Plane Curve Singularities, and Framed Mapping Class Groups
VANISHING CYCLES, PLANE CURVE SINGULARITIES, AND FRAMED MAPPING CLASS GROUPS PABLO PORTILLA CUADRADO AND NICK SALTER Abstract. Let f be an isolated plane curve singularity with Milnor fiber of genus at least 5. For all such f, we give (a) an intrinsic description of the geometric monodromy group that does not invoke the notion of the versal deformation space, and (b) an easy criterion to decide if a given simple closed curve in the Milnor fiber is a vanishing cycle or not. With the lone exception of singularities of type An and Dn, we find that both are determined completely by a canonical framing of the Milnor fiber induced by the Hamiltonian vector field associated to f. As a corollary we answer a question of Sullivan concerning the injectivity of monodromy groups for all singularities having Milnor fiber of genus at least 7. 1. Introduction Let f : C2 ! C denote an isolated plane curve singularity and Σ(f) the Milnor fiber over some point. A basic principle in singularity theory is to study f by way of its versal deformation space ∼ µ Vf = C , the parameter space of all deformations of f up to topological equivalence (see Section 2.2). From this point of view, two of the most basic invariants of f are the set of vanishing cycles and the geometric monodromy group. A simple closed curve c ⊂ Σ(f) is a vanishing cycle if there is some deformation fe of f with fe−1(0) a nodal curve such that c is contracted to a point when transported to −1 fe (0). -
Combination of Cubic and Quartic Plane Curve
IOSR Journal of Mathematics (IOSR-JM) e-ISSN: 2278-5728,p-ISSN: 2319-765X, Volume 6, Issue 2 (Mar. - Apr. 2013), PP 43-53 www.iosrjournals.org Combination of Cubic and Quartic Plane Curve C.Dayanithi Research Scholar, Cmj University, Megalaya Abstract The set of complex eigenvalues of unistochastic matrices of order three forms a deltoid. A cross-section of the set of unistochastic matrices of order three forms a deltoid. The set of possible traces of unitary matrices belonging to the group SU(3) forms a deltoid. The intersection of two deltoids parametrizes a family of Complex Hadamard matrices of order six. The set of all Simson lines of given triangle, form an envelope in the shape of a deltoid. This is known as the Steiner deltoid or Steiner's hypocycloid after Jakob Steiner who described the shape and symmetry of the curve in 1856. The envelope of the area bisectors of a triangle is a deltoid (in the broader sense defined above) with vertices at the midpoints of the medians. The sides of the deltoid are arcs of hyperbolas that are asymptotic to the triangle's sides. I. Introduction Various combinations of coefficients in the above equation give rise to various important families of curves as listed below. 1. Bicorn curve 2. Klein quartic 3. Bullet-nose curve 4. Lemniscate of Bernoulli 5. Cartesian oval 6. Lemniscate of Gerono 7. Cassini oval 8. Lüroth quartic 9. Deltoid curve 10. Spiric section 11. Hippopede 12. Toric section 13. Kampyle of Eudoxus 14. Trott curve II. Bicorn curve In geometry, the bicorn, also known as a cocked hat curve due to its resemblance to a bicorne, is a rational quartic curve defined by the equation It has two cusps and is symmetric about the y-axis. -
Singularities Bifurcations and Catastrophes
Singularities Bifurcations and Catastrophes James Montaldi University of Manchester ©James Montaldi, 2020 © James Montaldi, 2020 Contents Preface xi 1 What’sitallabout? 1 1.1 The fold or saddle-nodebifurcation 2 1.2 Bifurcationsof contours 4 1.3 Zeeman catastrophemachine 5 1.4 Theevolute 6 1.5 Pitchfork bifurcation 11 1.6 Conclusions 13 Problems 14 I Catastrophe theory 17 2 Familiesof functions 19 2.1 Criticalpoints 19 2.2 Degeneracyin onevariable 22 2.3 Familiesoffunctions 23 2.4 Cuspcatastrophe 26 2.5 Why‘catastrophes’ 29 Problems 30 3 The ring of germs of smooth functions 33 3.1 Germs: making everythinglocal 33 3.2 Theringofgerms 35 3.3 Newtondiagram 39 3.4 Nakayama’s lemma 41 3.5 Idealsof finite codimension 43 3.6 Geometric criterion for finite codimension 45 Problems 45 4 Rightequivalence 49 4.1 Rightequivalence 49 4.2 Jacobianideal 51 4.3 Codimension 52 4.4 Nondegeneratecritical points 52 4.5 SplittingLemma 55 Problems 59 vi Contents 5 Finitedeterminacy 63 5.1 Trivial familiesofgerms 64 5.2 Finitedeterminacy 67 5.3 Apartialconverse 70 5.4 Arefinementofthefinitedeterminacytheorem 71 5.5 Thehomotopymethod 72 5.6 Proof of finite determinacy theorems 74 5.7 Geometriccriterion 77 Problems 78 6 Classificationoftheelementarycatastrophes 81 6.1 Classification of corank 1 singularities 82 6.2 Classification of corank 2 critical points 84 6.3 Thom’s 7 elementarysingularities 86 6.4 Furtherclassification 87 Problems 89 7 Unfoldingsand catastrophes 91 7.1 Geometry of families of functions 92 7.2 Changeofparameterandinducedunfoldings 94 7.3 Equivalenceof -
Arxiv:Math/0507171V1 [Math.AG] 8 Jul 2005 Monodromy
Monodromy Wolfgang Ebeling Dedicated to Gert-Martin Greuel on the occasion of his 60th birthday. Abstract Let (X,x) be an isolated complete intersection singularity and let f : (X,x) → (C, 0) be the germ of an analytic function with an isolated singularity at x. An important topological invariant in this situation is the Picard-Lefschetz monodromy operator associated to f. We give a survey on what is known about this operator. In particular, we re- view methods of computation of the monodromy and its eigenvalues (zeta function), results on the Jordan normal form of it, definition and properties of the spectrum, and the relation between the monodromy and the topology of the singularity. Introduction The word ’monodromy’ comes from the greek word µoνo − δρoµψ and means something like ’uniformly running’ or ’uniquely running’. According to [99, 3.4.4], it was first used by B. Riemann [135]. It arose in keeping track of the solutions of the hypergeometric differential equation going once around arXiv:math/0507171v1 [math.AG] 8 Jul 2005 a singular point on a closed path (cf. [30]). The group of linear substitutions which the solutions are subject to after this process is called the monodromy group. Since then, monodromy groups have played a substantial rˆole in many areas of mathematics. As is indicated on the webside ’www.monodromy.com’ of N. M. Katz, there are several incarnations, classical and l-adic, local and global, arithmetic and geometric. Here we concentrate on the classical lo- cal geometric monodromy in singularity theory. More precisely we focus on the monodromy operator of an isolated hypersurface or complete intersection singularity. -
1 Functions, Derivatives, and Notation 2 Remarks on Leibniz Notation
ORDINARY DIFFERENTIAL EQUATIONS MATH 241 SPRING 2019 LECTURE NOTES M. P. COHEN CARLETON COLLEGE 1 Functions, Derivatives, and Notation A function, informally, is an input-output correspondence between values in a domain or input space, and values in a codomain or output space. When studying a particular function in this course, our domain will always be either a subset of the set of all real numbers, always denoted R, or a subset of n-dimensional Euclidean space, always denoted Rn. Formally, Rn is the set of all ordered n-tuples (x1; x2; :::; xn) where each of x1; x2; :::; xn is a real number. Our codomain will always be R, i.e. our functions under consideration will be real-valued. We will typically functions in two ways. If we wish to highlight the variable or input parameter, we will write a function using first a letter which represents the function, followed by one or more letters in parentheses which represent input variables. For example, we write f(x) or y(t) or F (x; y). In the first two examples above, we implicitly assume that the variables x and t vary over all possible inputs in the domain R, while in the third example we assume (x; y)p varies over all possible inputs in the domain R2. For some specific examples of functions, e.g. f(x) = x − 5, we assume that the domain includesp only real numbers x for which it makes sense to plug x into the formula, i.e., the domain of f(x) = x − 5 is just the interval [5; 1). -
Diophantine Problems in Polynomial Theory
Diophantine Problems in Polynomial Theory by Paul David Lee B.Sc. Mathematics, The University of British Columbia, 2009 A THESIS SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF MASTER OF SCIENCE in The College of Graduate Studies (Mathematics) THE UNIVERSITY OF BRITISH COLUMBIA (Okanagan) August 2011 c Paul David Lee 2011 Abstract Algebraic curves and surfaces are playing an increasing role in mod- ern mathematics. From the well known applications to cryptography, to computer vision and manufacturing, studying these curves is a prevalent problem that is appearing more often. With the advancement of computers, dramatic progress has been made in all branches of algebraic computation. In particular, computer algebra software has made it much easier to find rational or integral points on algebraic curves. Computers have also made it easier to obtain rational parametrizations of certain curves and surfaces. Each algebraic curve has an associated genus, essentially a classification, that determines its topological structure. Advancements on methods and theory on curves of genus 0, 1 and 2 have been made in recent years. Curves of genus 0 are the only algebraic curves that you can obtain a rational parametrization for. Curves of genus 1 (also known as elliptic curves) have the property that their rational points have a group structure and thus one can call upon the massive field of group theory to help with their study. Curves of higher genus (such as genus 2) do not have the background and theory that genus 0 and 1 do but recent advancements in theory have rapidly expanded advancements on the topic. -
TWO FAMILIES of STABLE BUNDLES with the SAME SPECTRUM Nonreduced [M]
proceedings of the american mathematical society Volume 109, Number 3, July 1990 TWO FAMILIES OF STABLE BUNDLES WITH THE SAME SPECTRUM A. P. RAO (Communicated by Louis J. Ratliff, Jr.) Abstract. We study stable rank two algebraic vector bundles on P and show that the family of bundles with fixed Chern classes and spectrum may have more than one irreducible component. We also produce a component where the generic bundle has a monad with ghost terms which cannot be deformed away. In the last century, Halphen and M. Noether attempted to classify smooth algebraic curves in P . They proceeded with the invariants d , g , the degree and genus, and worked their way up to d = 20. As the invariants grew larger, the number of components of the parameter space grew as well. Recent work of Gruson and Peskine has settled the question of which invariant pairs (d, g) are admissible. For a fixed pair (d, g), the question of determining the number of components of the parameter space is still intractable. For some values of (d, g) (for example [E-l], if d > g + 3) there is only one component. For other values, one may find many components including components which are nonreduced [M]. More recently, similar questions have been asked about algebraic vector bun- dles of rank two on P . We will restrict our attention to stable bundles a? with first Chern class c, = 0 (and second Chern class c2 = n, so that « is a positive integer and i? has no global sections). To study these, we have the invariants n, the a-invariant (which is equal to dim//"'(P , f(-2)) mod 2) and the spectrum. -
Geometry of Algebraic Curves
Geometry of Algebraic Curves Fall 2011 Course taught by Joe Harris Notes by Atanas Atanasov One Oxford Street, Cambridge, MA 02138 E-mail address: [email protected] Contents Lecture 1. September 2, 2011 6 Lecture 2. September 7, 2011 10 2.1. Riemann surfaces associated to a polynomial 10 2.2. The degree of KX and Riemann-Hurwitz 13 2.3. Maps into projective space 15 2.4. An amusing fact 16 Lecture 3. September 9, 2011 17 3.1. Embedding Riemann surfaces in projective space 17 3.2. Geometric Riemann-Roch 17 3.3. Adjunction 18 Lecture 4. September 12, 2011 21 4.1. A change of viewpoint 21 4.2. The Brill-Noether problem 21 Lecture 5. September 16, 2011 25 5.1. Remark on a homework problem 25 5.2. Abel's Theorem 25 5.3. Examples and applications 27 Lecture 6. September 21, 2011 30 6.1. The canonical divisor on a smooth plane curve 30 6.2. More general divisors on smooth plane curves 31 6.3. The canonical divisor on a nodal plane curve 32 6.4. More general divisors on nodal plane curves 33 Lecture 7. September 23, 2011 35 7.1. More on divisors 35 7.2. Riemann-Roch, finally 36 7.3. Fun applications 37 7.4. Sheaf cohomology 37 Lecture 8. September 28, 2011 40 8.1. Examples of low genus 40 8.2. Hyperelliptic curves 40 8.3. Low genus examples 42 Lecture 9. September 30, 2011 44 9.1. Automorphisms of genus 0 an 1 curves 44 9.2.