Integral Quadratic Forms : Applications to Algebraic Geometry Séminaire N
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3 Bilinear Forms & Euclidean/Hermitian Spaces
3 Bilinear Forms & Euclidean/Hermitian Spaces Bilinear forms are a natural generalisation of linear forms and appear in many areas of mathematics. Just as linear algebra can be considered as the study of `degree one' mathematics, bilinear forms arise when we are considering `degree two' (or quadratic) mathematics. For example, an inner product is an example of a bilinear form and it is through inner products that we define the notion of length in n p 2 2 analytic geometry - recall that the length of a vector x 2 R is defined to be x1 + ... + xn and that this formula holds as a consequence of Pythagoras' Theorem. In addition, the `Hessian' matrix that is introduced in multivariable calculus can be considered as defining a bilinear form on tangent spaces and allows us to give well-defined notions of length and angle in tangent spaces to geometric objects. Through considering the properties of this bilinear form we are able to deduce geometric information - for example, the local nature of critical points of a geometric surface. In this final chapter we will give an introduction to arbitrary bilinear forms on K-vector spaces and then specialise to the case K 2 fR, Cg. By restricting our attention to thse number fields we can deduce some particularly nice classification theorems. We will also give an introduction to Euclidean spaces: these are R-vector spaces that are equipped with an inner product and for which we can `do Euclidean geometry', that is, all of the geometric Theorems of Euclid will hold true in any arbitrary Euclidean space. -
Automorphic Forms for Some Even Unimodular Lattices
AUTOMORPHIC FORMS FOR SOME EVEN UNIMODULAR LATTICES NEIL DUMMIGAN AND DAN FRETWELL Abstract. We lookp at genera of even unimodular lattices of rank 12p over the ring of integers of Q( 5) and of rank 8 over the ring of integers of Q( 3), us- ing Kneser neighbours to diagonalise spaces of scalar-valued algebraic modular forms. We conjecture most of the global Arthur parameters, and prove several of them using theta series, in the manner of Ikeda and Yamana. We find in- stances of congruences for non-parallel weight Hilbert modular forms. Turning to the genus of Hermitian lattices of rank 12 over the Eisenstein integers, even and unimodular over Z, we prove a conjecture of Hentschel, Krieg and Nebe, identifying a certain linear combination of theta series as an Hermitian Ikeda lift, and we prove that another is an Hermitian Miyawaki lift. 1. Introduction Nebe and Venkov [54] looked at formal linear combinations of the 24 Niemeier lattices, which represent classes in the genus of even, unimodular, Euclidean lattices of rank 24. They found a set of 24 eigenvectors for the action of an adjacency oper- ator for Kneser 2-neighbours, with distinct integer eigenvalues. This is equivalent to computing a set of Hecke eigenforms in a space of scalar-valued modular forms for a definite orthogonal group O24. They conjectured the degrees gi in which the (gi) Siegel theta series Θ (vi) of these eigenvectors are first non-vanishing, and proved them in 22 out of the 24 cases. (gi) Ikeda [37, §7] identified Θ (vi) in terms of Ikeda lifts and Miyawaki lifts, in 20 out of the 24 cases, exploiting his integral construction of Miyawaki lifts. -
Notes on Symmetric Bilinear Forms
Symmetric bilinear forms Joel Kamnitzer March 14, 2011 1 Symmetric bilinear forms We will now assume that the characteristic of our field is not 2 (so 1 + 1 6= 0). 1.1 Quadratic forms Let H be a symmetric bilinear form on a vector space V . Then H gives us a function Q : V → F defined by Q(v) = H(v,v). Q is called a quadratic form. We can recover H from Q via the equation 1 H(v, w) = (Q(v + w) − Q(v) − Q(w)) 2 Quadratic forms are actually quite familiar objects. Proposition 1.1. Let V = Fn. Let Q be a quadratic form on Fn. Then Q(x1,...,xn) is a polynomial in n variables where each term has degree 2. Con- versely, every such polynomial is a quadratic form. Proof. Let Q be a quadratic form. Then x1 . Q(x1,...,xn) = [x1 · · · xn]A . x n for some symmetric matrix A. Expanding this out, we see that Q(x1,...,xn) = Aij xixj 1 Xi,j n ≤ ≤ and so it is a polynomial with each term of degree 2. Conversely, any polynomial of degree 2 can be written in this form. Example 1.2. Consider the polynomial x2 + 4xy + 3y2. This the quadratic 1 2 form coming from the bilinear form HA defined by the matrix A = . 2 3 1 We can use this knowledge to understand the graph of solutions to x2 + 2 1 0 4xy + 3y = 1. Note that HA has a diagonal matrix with respect to 0 −1 the basis (1, 0), (−2, 1). -
Embeddings of Integral Quadratic Forms Rick Miranda Colorado State
Embeddings of Integral Quadratic Forms Rick Miranda Colorado State University David R. Morrison University of California, Santa Barbara Copyright c 2009, Rick Miranda and David R. Morrison Preface The authors ran a seminar on Integral Quadratic Forms at the Institute for Advanced Study in the Spring of 1982, and worked on a book-length manuscript reporting on the topic throughout the 1980’s and early 1990’s. Some new results which are proved in the manuscript were announced in two brief papers in the Proceedings of the Japan Academy of Sciences in 1985 and 1986. We are making this preliminary version of the manuscript available at this time in the hope that it will be useful. Still to do before the manuscript is in final form: final editing of some portions, completion of the bibliography, and the addition of a chapter on the application to K3 surfaces. Rick Miranda David R. Morrison Fort Collins and Santa Barbara November, 2009 iii Contents Preface iii Chapter I. Quadratic Forms and Orthogonal Groups 1 1. Symmetric Bilinear Forms 1 2. Quadratic Forms 2 3. Quadratic Modules 4 4. Torsion Forms over Integral Domains 7 5. Orthogonality and Splitting 9 6. Homomorphisms 11 7. Examples 13 8. Change of Rings 22 9. Isometries 25 10. The Spinor Norm 29 11. Sign Structures and Orientations 31 Chapter II. Quadratic Forms over Integral Domains 35 1. Torsion Modules over a Principal Ideal Domain 35 2. The Functors ρk 37 3. The Discriminant of a Torsion Bilinear Form 40 4. The Discriminant of a Torsion Quadratic Form 45 5. -
Genus of Vertex Algebras and Mass Formula
Genus of vertex algebras and mass formula Yuto Moriwaki * Graduate School of Mathematical Science, The University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8914, Japan Abstract. We introduce the notion of a genus and its mass for vertex algebras. For lattice vertex algebras, their genera are the same as those of lattices, which play an important role in the classification of lattices. We derive a formula relating the mass for vertex algebras to that for lattices, and then give a new characterization of some holomorphic vertex operator algebras. Introduction Vertex operator algebras (VOAs) are algebraic structures that play an important role in two-dimensional conformal field theory. The classification of conformal field theories is an extremely interesting problem, of importance in mathematics, statistical mechanics, and string theory; Mathematically, it is related to the classification of vertex operator algebras, which is a main theme of this work. An important class of vertex operator algebras can be constructed from positive-definite even integral lattices, called lattice vertex algebras [Bo1, LL, FLM]. In this paper, we propose a new method to construct and classify vertex algebras by using a method developed in the study of lattices. A lattice is a finite rank free abelian group equipped with a Z-valued symmetric bilinear form. Two such lattices are equivalent (or in the same genus) if they are isomorphic over the ring of p-adic integers Zp for each prime p and also equivalent over the real number arXiv:2004.01441v2 [math.QA] 5 Mar 2021 field R. Lattices in the same genus are not always isomorphic over Z. -
Preliminary Material for M382d: Differential Topology
PRELIMINARY MATERIAL FOR M382D: DIFFERENTIAL TOPOLOGY DAVID BEN-ZVI Differential topology is the application of differential and integral calculus to study smooth curved spaces called manifolds. The course begins with the assumption that you have a solid working knowledge of calculus in flat space. This document sketches some important ideas and given you some problems to jog your memory and help you review the material. Don't panic if some of this material is unfamiliar, as I expect it will be for most of you. Simply try to work through as much as you can. [In the name of intellectual honesty, I mention that this handout, like much of the course, is cribbed from excellent course materials developed in previous semesters by Dan Freed.] Here, first, is a brief list of topics I expect you to know: Linear algebra: abstract vector spaces and linear maps, dual space, direct sum, subspaces and quotient spaces, bases, change of basis, matrix compu- tations, trace and determinant, bilinear forms, diagonalization of symmetric bilinear forms, inner product spaces Calculus: directional derivative, differential, (higher) partial derivatives, chain rule, second derivative as a symmetric bilinear form, Taylor's theo- rem, inverse and implicit function theorem, integration, change of variable formula, Fubini's theorem, vector calculus in 3 dimensions (div, grad, curl, Green and Stokes' theorems), fundamental theorem on ordinary differential equations You may or may not have studied all of these topics in your undergraduate years. Most of the topics listed here will come up at some point in the course. As for references, I suggest first that you review your undergraduate texts. -
Limit Roots of Lorentzian Coxeter Systems
UNIVERSITY OF CALIFORNIA Santa Barbara Limit Roots of Lorentzian Coxeter Systems A Thesis submitted in partial satisfaction of the requirements for the degree of Master of Arts in Mathematics by Nicolas R. Brody Committee in Charge: Professor Jon McCammond, Chair Professor Darren Long Professor Stephen Bigelow June 2016 The Thesis of Nicolas R. Brody is approved: Professor Darren Long Professor Stephen Bigelow Professor Jon McCammond, Committee Chairperson May 2016 Limit Roots of Lorentzian Coxeter Systems Copyright c 2016 by Nicolas R. Brody iii Acknowledgements My time at UC Santa Barbara has been inundated with wonderful friends, teachers, mentors, and mathematicians. I am especially indebted to Jon McCammond, Jordan Schettler, and Maribel Cachadia. A very special thanks to Jean-Phillippe Labb for sharing his code which was used to produce Figures 7.1, 7.3, and 7.4. This thesis is dedicated to my three roommates: Viki, Luna, and Layla. I hope we can all be roommates again soon. iv Abstract Limit Roots of Lorentzian Coxeter Systems Nicolas R. Brody A reflection in a real vector space equipped with a positive definite symmetric bilinear form is any automorphism that sends some nonzero vector v to its negative and pointwise fixes its orthogonal complement, and a finite reflection group is a group generated by such transformations that acts properly on the sphere of unit vectors. We note two important classes of groups which occur as finite reflection groups: for a 2-dimensional vector space, we recover precisely the finite dihedral groups as reflection groups, and permuting basis vectors in an n-dimensional vector space gives a way of viewing a symmetric group as a reflection group. -
Krammer Representations for Complex Braid Groups
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Journal of Algebra 371 (2012) 175–206 Contents lists available at SciVerse ScienceDirect Journal of Algebra www.elsevier.com/locate/jalgebra Krammer representations for complex braid groups Ivan Marin Institut de Mathématiques de Jussieu, Université Paris 7, 175 rue du Chevaleret, F-75013 Paris, France article info abstract Article history: Let B be the generalized braid group associated to some finite Received 5 April 2012 complex reflection group W . We define a representation of B Availableonline30August2012 of dimension the number of reflections of the corresponding Communicated by Michel Broué reflection group, which generalizes the Krammer representation of the classical braid groups, and is thus a good candidate in view MSC: 20C99 of proving the linearity of B. We decompose this representation 20F36 in irreducible components and compute its Zariski closure, as well as its restriction to parabolic subgroups. We prove that it is Keywords: faithful when W is a Coxeter group of type ADE and odd dihedral Braid groups types, and conjecture its faithfulness when W has a single class Complex reflection groups of reflections. If true, this conjecture would imply various group- Linear representations theoretic properties for these groups, that we prove separately to Knizhnik–Zamolodchikov systems be true for the other groups. Krammer representation © 2012 Elsevier Inc. All rights reserved. 1. Introduction Let k be a field of characteristic 0 and E a finite-dimensional k-vector space. A reflection in E is an element s ∈ GL(E) such that s2 = 1 and Ker(s − 1) is a hyperplane of E. -
1 Positive Definite Even Unimodular Lattices
Algebraic automorphic forms and Hilbert-Siegel modular forms Tamotsu Ikeda (Kyoto university) Sep. 17, 2018, at Hakuba 1 Positive definite even unimodular lattices Let F be a totally real number field of degree d. Let n > 0 be an integer such that dn is even. Then, by Minkowski-Hasse theorem, there exists a quadratic space (Vn;Q) of rank 4n with the following properties: (1) (V; Q) is unramified at any non-archimedean place. (2) (V; Q) is positive definite ai any archimedean place. Definition 1. An algebraic automorphic form on the orthogonal group OQ is a locally constant function on OQ(F )nOQ(A). Put 1 (x; y) = (Q(x + y) − Q(x) − Q(y)) x; y 2 V: Q 2 Let L be a o-lattie in V (F ). The dual lattice L∗ is defined by ∗ L = fx 2 Vn(F ) j (x; L)Q ⊂ og: Then L is an integral lattice if and only if L ⊂ L∗. An integral lattice L is called an even lattice if Q(x) ⊂ 2o 8x 2 L: Moreover, an integral lattice L is unimodular if L = L∗. By the assumption (1) and (2), there exists a positive definite even unimodular latice L0 in V (F ). Two integral lattices L1 and L2 are equivalent if there exists an element g 2 OQ(F ) such that g · L1 = L2. Two integral lattices L1 and L2 are in the same genus if there 1 exists an element gv 2 OQ(Fv) such that g · L1;v = L2;v for any finite place v. The set of positive definite even unimodular lattices in V (F ) form a genus. -
On the Classification of Integral Quadratic Forms
15 On the Classification of Integral Quadratic Forms J. H. Conway and N. J. A. Sloane This chapter gives an account of the classification of integral quadratic forms. It is particularly designed for readers who wish to be able to do explicit calculations. Novel features include an elementary system of rational invariants (defined without using the Hilbert norm residue symbol), an improved notation for the genus of a form, an efficient way to compute the number of spinor genera in a genus, and some conditions which imply that there is only one class in a genus. We give tables of the binary forms with - 100 ~ det ~ 50, the indecomposable ternary forms with Idetl ~ 50, the genera of forms with Idetl ~ 11, the genera of p elementary forms for all p, and the positive definite forms with determinant 2 up to dimension 18 and determinant 3 up to dimension 17. 1. Introduction The project of classifying integral quadratic forms has a long history, to which many mathematicians have contributed. The binary (or two dimensional) forms were comprehensively discussed by Gauss. Gauss and later workers also made substantial inroads into the problem of ternary and higher-dimensional forms. The greatest advances since then have been the beautiful development of the theory of rational quadratic forms (Minkowski, Hasse, Witt), and Eichler's complete classification of indefinite forms in dimension 3 or higher in terms of the notion of spinor genus. Definite forms correspond to lattices in Euclidean space. For small dimensions they can be classified using Minkowski's generalization of Gauss's notion of reduced form, but this method rapidly becomes impracticable when the dimension reaches 6 or 7. -
Contents 5 Bilinear and Quadratic Forms
Linear Algebra (part 5): Bilinear and Quadratic Forms (by Evan Dummit, 2020, v. 1.00) Contents 5 Bilinear and Quadratic Forms 1 5.1 Bilinear Forms . 1 5.1.1 Denition, Associated Matrices, Basic Properties . 1 5.1.2 Symmetric Bilinear Forms and Diagonalization . 3 5.2 Quadratic Forms . 5 5.2.1 Denition and Basic Properties . 6 5.2.2 Quadratic Forms Over Rn: Diagonalization of Quadratic Varieties . 7 5.2.3 Quadratic Forms Over Rn: The Second Derivatives Test . 9 5.2.4 Quadratic Forms Over Rn: Sylvester's Law of Inertia . 11 5 Bilinear and Quadratic Forms In this chapter, we will discuss bilinear and quadratic forms. Bilinear forms are simply linear transformations that are linear in more than one variable, and they will allow us to extend our study of linear phenomena. They are closely related to quadratic forms, which are (classically speaking) homogeneous quadratic polynomials in multiple variables. Despite the fact that quadratic forms are not linear, we can (perhaps surprisingly) still use many of the tools of linear algebra to study them. 5.1 Bilinear Forms • We begin by discussing basic properties of bilinear forms on an arbitrary vector space. 5.1.1 Denition, Associated Matrices, Basic Properties • Let V be a vector space over the eld F . • Denition: A function Φ: V × V ! F is a bilinear form on V if it is linear in each variable when the other variable is xed. Explicitly, this means Φ(v1 + αv2; y) = Φ(v1; w) + αΦ(v2; w) and Φ(v; w1 + αw2) = Φ(v; w1) + αΦ(v; w2) for arbitrary vi; wi 2 V and α 2 F . -
Lattice Theory, K3 Surfaces, and the Torelli Theorem
UMass, Reading Seminar in Algebraic Geometry, Lattice theory, K3 surfaces, and the Torelli theorem Luca Schaffler October 4, 2019 1 What is a lattice? Definition 1.1. A lattice is a pair (L; ·), where L is a finitely generated free abelian group and ·: L × L ! Z such that (v; w) 7! v · w is a symmetric bilinear form. • L is even if v2 := v · v is an even number for all v 2 L. • The Gram matrix of L with respect to a basis fe1; : : : ; eng for L is the matrix of intersection (ei · ej)1≤i;j≤n. • The rank of L is defined to be the rank of one of its Gram matrices. • A lattice L is unimodular if the determinant of one of its Gram matrices is ±1. Equivalently, L of maximal rank is unimodular provided the discriminant group ∗ ∗ L =L is trivial (we let L = HomZ(L; Z)). • We can define the signature of L as the signature of one of its Gram matrices. By saying signature (a; b), we mean that a (resp. b) is the number of positive (resp. negative) eigenvalues. If L has signature (a; b), then we say that L is indefinite provided a; b > 0. 2 Example 1.2. U = (Z ; ·) with (v1; v2) · (w1; w2) = v1w2 + v2w1 is called the hyperbolic plane. Check that this is even, unimodular, and of signature (1; 1). 1 8 Example 1.3. E8 = (Z ;B), where 0 −2 1 0 0 0 0 0 0 1 B 1 −2 1 0 0 0 0 0 C B C B 0 1 −2 1 0 0 0 0 C B C B 0 0 1 −2 1 0 0 0 C B = B C : B 0 0 0 1 −2 1 0 1 C B C B 0 0 0 0 1 −2 1 0 C B C @ 0 0 0 0 0 1 −2 0 A 0 0 0 0 1 0 0 −2 This matrix can be reconstructed from the E8 Dynkin diagram.