Algebraic Geometry Notes Richard Borcherds
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THE CUBIC THREEFOLD and FRIENDS 1. Background On
THE CUBIC THREEFOLD AND FRIENDS 1. Background on Threefolds Fano, around the 1910s, proved that any smooth quartic threefold • is not rational. Later on, in the 1950s, Roth criticised the proof as incomplete. In 1971, Iskovskikh and Manin provide a complete proof. In 1972, Artin and Mumford gave an example of another unirational, • but not rational Fano threefold. This is a certain double cover X of P3 ramified over a singular quartic surface. They showed that H3(X; Z) is a birational invariant and obtained that H3(X; Z) = Z2, from which they concluded that X cannot be rational. At the same time, Clemens and Griffiths showed that any smooth • cubic threefold V over a field of characteristic zero is unirational, but not rational. In the same year, Murre proved the result in char- acteristic p. The idea of Clemens and Griffiths was to consider two auxiliary varieties of a smooth cubic threefold V: The intermediate Jacobian J(V) - a principally polarised abelian variety • playing a role similar to that of the Jacobian for studying divisors on curves. the Fano variety of lines F(V) - a smooth projective surface parametris- • ing lines on V. In order to arrive at the result, they represented J(V) as the Albanese variety of F(V), and studied its theta divisors. 2. The Cohomology of the Cubic Threefold As before, let V be a cubic threefold, i.e. a hypersurface of degree three in P4. A first idea is to compare the cohomology of V with that of P3 and hope that we shall thus find a birational invariant that has different values for V and P3, respectively. -
The Many Lives of the Twisted Cubic
Mathematical Assoc. of America American Mathematical Monthly 121:1 February 10, 2018 11:32 a.m. TwistedMonthly.tex page 1 The many lives of the twisted cubic Abstract. We trace some of the history of the twisted cubic curves in three-dimensional affine and projective spaces. These curves have reappeared many times in many different guises and at different times they have served as primary objects of study, as motivating examples, and as hidden underlying structures for objects considered in mathematics and its applications. 1. INTRODUCTION Because of its simple coordinate functions, the humble (affine) 3 twisted cubic curve in R , given in the parametric form ~x(t) = (t; t2; t3) (1.1) is staple of computational problems in many multivariable calculus courses. (See Fig- ure 1.) We and our students compute its intersections with planes, find its tangent vectors and lines, approximate the arclength of segments of the curve, derive its cur- vature and torsion functions, and so forth. But in many calculus books, the curve is not even identified by name and no indication of its protean nature and rich history is given. This essay is (semi-humorously) in part an attempt to remedy that situation, and (more seriously) in part a meditation on the ways that the things mathematicians study often seem to have existences of their own. Basic structures can reappear at many times in many different contexts and under different names. According to the current consensus view of mathematical historiography, historians of mathematics do well to keep these different avatars of the underlying structure separate because it is almost never correct to attribute our understanding of the sorts of connections we will be con- sidering to the thinkers of the past. -
Chapter 11. Three Dimensional Analytic Geometry and Vectors
Chapter 11. Three dimensional analytic geometry and vectors. Section 11.5 Quadric surfaces. Curves in R2 : x2 y2 ellipse + =1 a2 b2 x2 y2 hyperbola − =1 a2 b2 parabola y = ax2 or x = by2 A quadric surface is the graph of a second degree equation in three variables. The most general such equation is Ax2 + By2 + Cz2 + Dxy + Exz + F yz + Gx + Hy + Iz + J =0, where A, B, C, ..., J are constants. By translation and rotation the equation can be brought into one of two standard forms Ax2 + By2 + Cz2 + J =0 or Ax2 + By2 + Iz =0 In order to sketch the graph of a quadric surface, it is useful to determine the curves of intersection of the surface with planes parallel to the coordinate planes. These curves are called traces of the surface. Ellipsoids The quadric surface with equation x2 y2 z2 + + =1 a2 b2 c2 is called an ellipsoid because all of its traces are ellipses. 2 1 x y 3 2 1 z ±1 ±2 ±3 ±1 ±2 The six intercepts of the ellipsoid are (±a, 0, 0), (0, ±b, 0), and (0, 0, ±c) and the ellipsoid lies in the box |x| ≤ a, |y| ≤ b, |z| ≤ c Since the ellipsoid involves only even powers of x, y, and z, the ellipsoid is symmetric with respect to each coordinate plane. Example 1. Find the traces of the surface 4x2 +9y2 + 36z2 = 36 1 in the planes x = k, y = k, and z = k. Identify the surface and sketch it. Hyperboloids Hyperboloid of one sheet. The quadric surface with equations x2 y2 z2 1. -
Moduli Spaces of Quadratic Rational Maps with a Marked Periodic Point
J. Blanc et al. (2015) “Quadratic Maps with a Marked Periodic Point of Small Order,” International Mathematics Research Notices, Vol. 2015, No. 23, pp. 12459–12489 Advance Access Publication March 10, 2015 doi:10.1093/imrn/rnv063 Moduli Spaces of Quadratic Rational Maps with a Marked Periodic Point of Small Order Downloaded from https://academic.oup.com/imrn/article/2015/23/12459/672405 by guest on 27 September 2021 Jer´ emy´ Blanc1, Jung Kyu Canci1, and Noam D. Elkies2 1Mathematisches Institut, Universitat¨ Basel, Spiegelgasse 1, CH-4051 Basel, Switzerland and 2Department of Mathematics, Harvard University, Cambridge, MA 02138, USA Correspondence to be sent to: [email protected] The surface corresponding to the moduli space of quadratic endomorphisms of P1 with a marked periodic point of order nis studied. It is shown that the surface is rational over Q when n≤ 5 and is of general type for n= 6. An explicit description of the n= 6 surface lets us find several infinite families of quadratic endomorphisms f : P1 → P1 defined over Q with a rational periodic point of order 6. In one of these families, f also has a rational fixed point, for a total of at least 7 periodic and 7 preperiodic points. This is in contrast with the polynomial case, where it is conjectured that no polynomial endomorphism defined over Q admits rational periodic points of order n> 3. 1 Introduction A classical question in arithmetic dynamics concerns periodic, and more generally preperiodic, points of a rational map (endomorphism) f : P1(Q) → P1(Q).Apointp is said to be periodic of order n if f n(p) = p and if f i(p) = p for 0 < i < n.Apointp is said to be preperiodic if there exists a non-negative integer m such that the point f m(p) is periodic. -
A Three-Dimensional Laguerre Geometry and Its Visualization
A Three-Dimensional Laguerre Geometry and Its Visualization Hans Havlicek and Klaus List, Institut fur¨ Geometrie, TU Wien 3 We describe and visualize the chains of the 3-dimensional chain geometry over the ring R("), " = 0. MSC 2000: 51C05, 53A20. Keywords: chain geometry, Laguerre geometry, affine space, twisted cubic. 1 Introduction The aim of the present paper is to discuss in some detail the Laguerre geometry (cf. [1], [6]) which arises from the 3-dimensional real algebra L := R("), where "3 = 0. This algebra generalizes the algebra of real dual numbers D = R("), where "2 = 0. The Laguerre geometry over D is the geometry on the so-called Blaschke cylinder (Figure 1); the non-degenerate conics on this cylinder are called chains (or cycles, circles). If one generator of the cylinder is removed then the remaining points of the cylinder are in one-one correspon- dence (via a stereographic projection) with the points of the plane of dual numbers, which is an isotropic plane; the chains go over R" to circles and non-isotropic lines. So the point space of the chain geometry over the real dual numbers can be considered as an affine plane with an extra “improper line”. The Laguerre geometry based on L has as point set the projective line P(L) over L. It can be seen as the real affine 3-space on L together with an “improper affine plane”. There is a point model R for this geometry, like the Blaschke cylinder, but it is more compli- cated, and belongs to a 7-dimensional projective space ([6, p. -
A Quick Algebra Review
A Quick Algebra Review 1. Simplifying Expressions 2. Solving Equations 3. Problem Solving 4. Inequalities 5. Absolute Values 6. Linear Equations 7. Systems of Equations 8. Laws of Exponents 9. Quadratics 10. Rationals 11. Radicals Simplifying Expressions An expression is a mathematical “phrase.” Expressions contain numbers and variables, but not an equal sign. An equation has an “equal” sign. For example: Expression: Equation: 5 + 3 5 + 3 = 8 x + 3 x + 3 = 8 (x + 4)(x – 2) (x + 4)(x – 2) = 10 x² + 5x + 6 x² + 5x + 6 = 0 x – 8 x – 8 > 3 When we simplify an expression, we work until there are as few terms as possible. This process makes the expression easier to use, (that’s why it’s called “simplify”). The first thing we want to do when simplifying an expression is to combine like terms. For example: There are many terms to look at! Let’s start with x². There Simplify: are no other terms with x² in them, so we move on. 10x x² + 10x – 6 – 5x + 4 and 5x are like terms, so we add their coefficients = x² + 5x – 6 + 4 together. 10 + (-5) = 5, so we write 5x. -6 and 4 are also = x² + 5x – 2 like terms, so we can combine them to get -2. Isn’t the simplified expression much nicer? Now you try: x² + 5x + 3x² + x³ - 5 + 3 [You should get x³ + 4x² + 5x – 2] Order of Operations PEMDAS – Please Excuse My Dear Aunt Sally, remember that from Algebra class? It tells the order in which we can complete operations when solving an equation. -
Real Rank Two Geometry Arxiv:1609.09245V3 [Math.AG] 5
Real Rank Two Geometry Anna Seigal and Bernd Sturmfels Abstract The real rank two locus of an algebraic variety is the closure of the union of all secant lines spanned by real points. We seek a semi-algebraic description of this set. Its algebraic boundary consists of the tangential variety and the edge variety. Our study of Segre and Veronese varieties yields a characterization of tensors of real rank two. 1 Introduction Low-rank approximation of tensors is a fundamental problem in applied mathematics [3, 6]. We here approach this problem from the perspective of real algebraic geometry. Our goal is to give an exact semi-algebraic description of the set of tensors of real rank two and to characterize its boundary. This complements the results on tensors of non-negative rank two presented in [1], and it offers a generalization to the setting of arbitrary varieties, following [2]. A familiar example is that of 2 × 2 × 2-tensors (xijk) with real entries. Such a tensor lies in the closure of the real rank two tensors if and only if the hyperdeterminant is non-negative: 2 2 2 2 2 2 2 2 x000x111 + x001x110 + x010x101 + x011x100 + 4x000x011x101x110 + 4x001x010x100x111 −2x000x001x110x111 − 2x000x010x101x111 − 2x000x011x100x111 (1) −2x001x010x101x110 − 2x001x011x100x110 − 2x010x011x100x101 ≥ 0: If this inequality does not hold then the tensor has rank two over C but rank three over R. To understand this example geometrically, consider the Segre variety X = Seg(P1 × P1 × P1), i.e. the set of rank one tensors, regarded as points in the projective space P7 = 2 2 2 7 arXiv:1609.09245v3 [math.AG] 5 Apr 2017 P(C ⊗ C ⊗ C ). -
Algebraic Geometry Michael Stoll
Introductory Geometry Course No. 100 351 Fall 2005 Second Part: Algebraic Geometry Michael Stoll Contents 1. What Is Algebraic Geometry? 2 2. Affine Spaces and Algebraic Sets 3 3. Projective Spaces and Algebraic Sets 6 4. Projective Closure and Affine Patches 9 5. Morphisms and Rational Maps 11 6. Curves — Local Properties 14 7. B´ezout’sTheorem 18 2 1. What Is Algebraic Geometry? Linear Algebra can be seen (in parts at least) as the study of systems of linear equations. In geometric terms, this can be interpreted as the study of linear (or affine) subspaces of Cn (say). Algebraic Geometry generalizes this in a natural way be looking at systems of polynomial equations. Their geometric realizations (their solution sets in Cn, say) are called algebraic varieties. Many questions one can study in various parts of mathematics lead in a natural way to (systems of) polynomial equations, to which the methods of Algebraic Geometry can be applied. Algebraic Geometry provides a translation between algebra (solutions of equations) and geometry (points on algebraic varieties). The methods are mostly algebraic, but the geometry provides the intuition. Compared to Differential Geometry, in Algebraic Geometry we consider a rather restricted class of “manifolds” — those given by polynomial equations (we can allow “singularities”, however). For example, y = cos x defines a perfectly nice differentiable curve in the plane, but not an algebraic curve. In return, we can get stronger results, for example a criterion for the existence of solutions (in the complex numbers), or statements on the number of solutions (for example when intersecting two curves), or classification results. -
Writing the Equation of a Line
Name______________________________ Writing the Equation of a Line When you find the equation of a line it will be because you are trying to draw scientific information from it. In math, you write equations like y = 5x + 2 This equation is useless to us. You will never graph y vs. x. You will be graphing actual data like velocity vs. time. Your equation should therefore be written as v = (5 m/s2) t + 2 m/s. See the difference? You need to use proper variables and units in order to compare it to theory or make actual conclusions about physical principles. The second equation tells me that when the data collection began (t = 0), the velocity of the object was 2 m/s. It also tells me that the velocity was changing at 5 m/s every second (m/s/s = m/s2). Let’s practice this a little, shall we? Force vs. mass F (N) y = 6.4x + 0.3 m (kg) You’ve just done a lab to see how much force was necessary to get a mass moving along a rough surface. Excel spat out the graph above. You labeled each axis with the variable and units (well done!). You titled the graph starting with the variable on the y-axis (nice job!). Now we turn to the equation. First we replace x and y with the variables we actually graphed: F = 6.4m + 0.3 Then we add units to our slope and intercept. The slope is found by dividing the rise by the run so the units will be the units from the y-axis divided by the units from the x-axis. -
Hyperbolic Monopoles and Rational Normal Curves
HYPERBOLIC MONOPOLES AND RATIONAL NORMAL CURVES Nigel Hitchin (Oxford) Edinburgh April 20th 2009 204 Research Notes A NOTE ON THE TANGENTS OF A TWISTED CUBIC B Y M. F. ATIYAH Communicated by J. A. TODD Received 8 May 1951 1. Consider a rational normal cubic C3. In the Klein representation of the lines of $3 by points of a quadric Q in Ss, the tangents of C3 are represented by the points of a rational normal quartic O4. It is the object of this note to examine some of the consequences of this correspondence, in terms of the geometry associated with the two curves. 2. C4 lies on a Veronese surface V, which represents the congruence of chords of O3(l). Also C4 determines a 4-space 2 meeting D. in Qx, say; and since the surface of tangents of O3 is a developable, consecutive tangents intersect, and therefore the tangents to C4 lie on Q, and so on £lv Hence Qx, containing the sextic surface of tangents to C4, must be the quadric threefold / associated with C4, i.e. the quadric determining the same polarity as C4 (2). We note also that the tangents to C4 correspond in #3 to the plane pencils with vertices on O3, and lying in the corresponding osculating planes. 3. We shall prove that the surface U, which is the locus of points of intersection of pairs of osculating planes of C4, is the projection of the Veronese surface V from L, the pole of 2, on to 2. Let P denote a point of C3, and t, n the tangent line and osculating plane at P, and let T, T, w denote the same for the corresponding point of C4. -
The Geometry of the Phase Diffusion Equation
J. Nonlinear Sci. Vol. 10: pp. 223–274 (2000) DOI: 10.1007/s003329910010 © 2000 Springer-Verlag New York Inc. The Geometry of the Phase Diffusion Equation N. M. Ercolani,1 R. Indik,1 A. C. Newell,1,2 and T. Passot3 1 Department of Mathematics, University of Arizona, Tucson, AZ 85719, USA 2 Mathematical Institute, University of Warwick, Coventry CV4 7AL, UK 3 CNRS UMR 6529, Observatoire de la Cˆote d’Azur, 06304 Nice Cedex 4, France Received on October 30, 1998; final revision received July 6, 1999 Communicated by Robert Kohn E E Summary. The Cross-Newell phase diffusion equation, (|k|)2T =∇(B(|k|) kE), kE =∇2, and its regularization describes natural patterns and defects far from onset in large aspect ratio systems with rotational symmetry. In this paper we construct explicit solutions of the unregularized equation and suggest candidates for its weak solutions. We confirm these ideas by examining a fourth-order regularized equation in the limit of infinite aspect ratio. The stationary solutions of this equation include the minimizers of a free energy, and we show these minimizers are remarkably well-approximated by a second-order “self-dual” equation. Moreover, the self-dual solutions give upper bounds for the free energy which imply the existence of weak limits for the asymptotic minimizers. In certain cases, some recent results of Jin and Kohn [28] combined with these upper bounds enable us to demonstrate that the energy of the asymptotic minimizers converges to that of the self-dual solutions in a viscosity limit. 1. Introduction The mathematical models discussed in this paper are motivated by physical systems, far from equilibrium, which spontaneously form patterns. -
RATIONAL HOMOGENEOUS VARIETIES Giorgio Ottaviani
RATIONAL HOMOGENEOUS VARIETIES Giorgio Ottaviani Dipartimento di Matematica, Universit`adell'Aquila Current address: Dipartimento di Matematica, Universit`adi Firenze viale Morgagni 67/A 50134 FIRENZE [email protected]fi.it x1. Introduction page 1 x2. Grassmannians and flag varieties 5 x3. Lie algebras and Lie groups 9 x4. The Borel fixed point theorem 18 x5. SL(2) 22 x6. The Cartan decomposition 26 x7. Borel and parabolic subgroups 37 x8. ABC about bundles 40 x9. Homogeneous bundles 47 x10. The theorem of Borel-Weil 51 x11. The theorem of Bott 61 x12. Stability of homogeneous bundles 65 References 69 These notes have been written for distribution to the participants to the summer school in Algebraic Geometry organized by the Scuola Matematica Universitaria in Cortona in the period 13-26 August 1995. The aim was to describe the classification of rational homogeneous varieties and to provide the theorems of Borel-Weil and Bott. Lie algebras are introduced starting from the definition and they are studied as far as it is necessary for the aim. At the other side, the knowledge of basic techniques of algebraic geometry (as sheaf cohomology) and algebraic topology was assumed. I learned most of the material of these notes from many lectures and discussions with Vincenzo Ancona and Alan Huckleberry. I am sincerely grateful to both of them and also to all the participants to the course in Cortona, especially to Raffaella Paoletti and Anke Simon for careful proofreading and for their suggestions. x1. Introduction An algebraic variety is a quasiprojective variety over the field C of complex numbers.