Basic Topological Structures of the Theory of Ordinary Differential Equations
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Ordinary Differential Equations
Ordinary Differential Equations for Engineers and Scientists Gregg Waterman Oregon Institute of Technology c 2017 Gregg Waterman This work is licensed under the Creative Commons Attribution 4.0 International license. The essence of the license is that You are free to: Share copy and redistribute the material in any medium or format • Adapt remix, transform, and build upon the material for any purpose, even commercially. • The licensor cannot revoke these freedoms as long as you follow the license terms. Under the following terms: Attribution You must give appropriate credit, provide a link to the license, and indicate if changes • were made. You may do so in any reasonable manner, but not in any way that suggests the licensor endorses you or your use. No additional restrictions You may not apply legal terms or technological measures that legally restrict others from doing anything the license permits. Notices: You do not have to comply with the license for elements of the material in the public domain or where your use is permitted by an applicable exception or limitation. No warranties are given. The license may not give you all of the permissions necessary for your intended use. For example, other rights such as publicity, privacy, or moral rights may limit how you use the material. For any reuse or distribution, you must make clear to others the license terms of this work. The best way to do this is with a link to the web page below. To view a full copy of this license, visit https://creativecommons.org/licenses/by/4.0/legalcode. -
256B Algebraic Geometry
256B Algebraic Geometry David Nadler Notes by Qiaochu Yuan Spring 2013 1 Vector bundles on the projective line This semester we will be focusing on coherent sheaves on smooth projective complex varieties. The organizing framework for this class will be a 2-dimensional topological field theory called the B-model. Topics will include 1. Vector bundles and coherent sheaves 2. Cohomology, derived categories, and derived functors (in the differential graded setting) 3. Grothendieck-Serre duality 4. Reconstruction theorems (Bondal-Orlov, Tannaka, Gabriel) 5. Hochschild homology, Chern classes, Grothendieck-Riemann-Roch For now we'll introduce enough background to talk about vector bundles on P1. We'll regard varieties as subsets of PN for some N. Projective will mean that we look at closed subsets (with respect to the Zariski topology). The reason is that if p : X ! pt is the unique map from such a subset X to a point, then we can (derived) push forward a bounded complex of coherent sheaves M on X to a bounded complex of coherent sheaves on a point Rp∗(M). Smooth will mean the following. If x 2 X is a point, then locally x is cut out by 2 a maximal ideal mx of functions vanishing on x. Smooth means that dim mx=mx = dim X. (In general it may be bigger.) Intuitively it means that locally at x the variety X looks like a manifold, and one way to make this precise is that the completion of the local ring at x is isomorphic to a power series ring C[[x1; :::xn]]; this is the ring where Taylor series expansions live. -
1 Sets and Set Notation. Definition 1 (Naive Definition of a Set)
LINEAR ALGEBRA MATH 2700.006 SPRING 2013 (COHEN) LECTURE NOTES 1 Sets and Set Notation. Definition 1 (Naive Definition of a Set). A set is any collection of objects, called the elements of that set. We will most often name sets using capital letters, like A, B, X, Y , etc., while the elements of a set will usually be given lower-case letters, like x, y, z, v, etc. Two sets X and Y are called equal if X and Y consist of exactly the same elements. In this case we write X = Y . Example 1 (Examples of Sets). (1) Let X be the collection of all integers greater than or equal to 5 and strictly less than 10. Then X is a set, and we may write: X = f5; 6; 7; 8; 9g The above notation is an example of a set being described explicitly, i.e. just by listing out all of its elements. The set brackets {· · ·} indicate that we are talking about a set and not a number, sequence, or other mathematical object. (2) Let E be the set of all even natural numbers. We may write: E = f0; 2; 4; 6; 8; :::g This is an example of an explicity described set with infinitely many elements. The ellipsis (:::) in the above notation is used somewhat informally, but in this case its meaning, that we should \continue counting forever," is clear from the context. (3) Let Y be the collection of all real numbers greater than or equal to 5 and strictly less than 10. Recalling notation from previous math courses, we may write: Y = [5; 10) This is an example of using interval notation to describe a set. -
Introduction to Abstract Algebra (Math 113)
Introduction to Abstract Algebra (Math 113) Alexander Paulin, with edits by David Corwin FOR FALL 2019 MATH 113 002 ONLY Contents 1 Introduction 4 1.1 What is Algebra? . 4 1.2 Sets . 6 1.3 Functions . 9 1.4 Equivalence Relations . 12 2 The Structure of + and × on Z 15 2.1 Basic Observations . 15 2.2 Factorization and the Fundamental Theorem of Arithmetic . 17 2.3 Congruences . 20 3 Groups 23 1 3.1 Basic Definitions . 23 3.1.1 Cayley Tables for Binary Operations and Groups . 28 3.2 Subgroups, Cosets and Lagrange's Theorem . 30 3.3 Generating Sets for Groups . 35 3.4 Permutation Groups and Finite Symmetric Groups . 40 3.4.1 Active vs. Passive Notation for Permutations . 40 3.4.2 The Symmetric Group Sym3 . 43 3.4.3 Symmetric Groups in General . 44 3.5 Group Actions . 52 3.5.1 The Orbit-Stabiliser Theorem . 55 3.5.2 Centralizers and Conjugacy Classes . 59 3.5.3 Sylow's Theorem . 66 3.6 Symmetry of Sets with Extra Structure . 68 3.7 Normal Subgroups and Isomorphism Theorems . 73 3.8 Direct Products and Direct Sums . 83 3.9 Finitely Generated Abelian Groups . 85 3.10 Finite Abelian Groups . 90 3.11 The Classification of Finite Groups (Proofs Omitted) . 95 4 Rings, Ideals, and Homomorphisms 100 2 4.1 Basic Definitions . 100 4.2 Ideals, Quotient Rings and the First Isomorphism Theorem for Rings . 105 4.3 Properties of Elements of Rings . 109 4.4 Polynomial Rings . 112 4.5 Ring Extensions . 115 4.6 Field of Fractions . -
Partial Differential Equations I: Basics and Separable Solutions
18 Partial Differential Equations I: Basics and Separable Solutions We now turn our attention to differential equations in which the “unknown function to be deter- mined” — which we will usually denote by u — depends on two or more variables. Hence the derivatives are partial derivatives with respect to the various variables. (By the way, it may be a good idea to quickly review the A Brief Review of Elementary Ordinary Differential Equations, Appendex A of these notes. We will be using some of the material discussed there.) 18.1 Intro and Examples Simple Examples If we have a horizontally stretched string vibrating up and down, let u(x, t) the vertical position at time t of the bit of string at horizontal position x , = and make some almost reasonable assumptions regarding the string, the universe and the laws of physics, then we can show that u(x, t) satisfies ∂2u ∂2u c2 0 ∂t2 − ∂x2 = where c is some positive constant dependent on the physical properties of the stretched string. This equation is called the one-dimensional wave equation (with no external forces). If, instead, we have a uniform one-dimensional heat conducting rod along the X–axis and let u(x, t) the temperature at time t of the bit of rod at horizontal position x , = then, after applying suitable assumptions about heat flow, etc., we get the one-dimensional heat equation ∂u ∂2u κ f (x, t) . ∂t − ∂x2 = Here, κ is a positive constant dependent on the material properties of the rod, and f (x, t) describes the thermal contributions due to heat sources and/or sinks in the rod. -
Zero and Triviality Andreas Haida1 and Tue Trinh2 1 ELSC, HUJI, Jerusalem, IL 2 Leibniz-ZAS, Berlin, DE Corresponding Author: Tue Trinh ([email protected])
a journal of Haida, Andreas and Tue Trinh. 2020. Zero and general linguistics Glossa triviality. Glossa: a journal of general linguistics 5(1): 116. 1–14. DOI: https://doi.org/10.5334/gjgl.955 RESEARCH Zero and triviality Andreas Haida1 and Tue Trinh2 1 ELSC, HUJI, Jerusalem, IL 2 Leibniz-ZAS, Berlin, DE Corresponding author: Tue Trinh ([email protected]) This paper takes issue with Bylinina & Nouwen’s (2018) hypothesis that the numeral zero has the basic weak meaning of ‘zero or more.’ We argue, on the basis of empirical observation and theoretical consideration, that this hypothesis implies that exhaustification can circum- vent L-triviality, and that exhaustification cannot circumvent L-triviality. We also provide some experimental results to support our argument. Keywords: numerals; modification; exhaustification; L-Triviality 1 Theses and antitheses 1.1 Exhaustification The aim of this squib is to discuss some issues regarding the hypothesis about zero put for- ward by Bylinina & Nouwen (2018). These authors assume that numerals have the weak, ‘at least’ meaning as basic and the strengthened, ‘exactly’ meaning as derived by way of exhaustification, and propose thatzero be considered no different from other numerals in this respect.1 This is illustrated by (1a) and (1b). (1) a. Zero students smoked | ⟦students⟧ ⟦smoked⟧ | ≥ 0 ‘the number of students⟺ who smoked is zero or greater’ ⋂ b. EXH [Zero students smoked] | ⟦students⟧ ⟦smoked⟧ | ≥ 0 | ⟦students⟧ ⟦smoked⟧ | ≥| 1 ‘the number of students who smoked⟺ is zero and not greater’ ⋂ ∧ ⋂ Before we go on, let us be explicit about the notion of exhaustification which we will adopt for the purpose of this discussion. -
Arxiv:1509.06425V4 [Math.AG] 9 Dec 2017 Nipratrl Ntegoercraiaino Conformal of Gen Realization a Geometric the (And in Fact Role This Important Trivial
TRIVIALITY PROPERTIES OF PRINCIPAL BUNDLES ON SINGULAR CURVES PRAKASH BELKALE AND NAJMUDDIN FAKHRUDDIN Abstract. We show that principal bundles for a semisimple group on an arbitrary affine curve over an algebraically closed field are trivial, provided the order of π1 of the group is invertible in the ground field, or if the curve has semi-normal singularities. Several consequences and extensions of this result (and method) are given. As an application, we realize conformal blocks bundles on moduli stacks of stable curves as push forwards of line bundles on (relative) moduli stacks of principal bundles on the universal curve. 1. Introduction It is a consequence of a theorem of Harder [Har67, Satz 3.3] that generically trivial principal G-bundles on a smooth affine curve C over an arbitrary field k are trivial if G is a semisimple and simply connected algebraic group. When k is algebraically closed and G reductive, generic triviality, conjectured by Serre, was proved by Steinberg[Ste65] and Borel–Springer [BS68]. It follows that principal bundles for simply connected semisimple groups over smooth affine curves over algebraically closed fields are trivial. This fact (and a generalization to families of bundles [DS95]) plays an important role in the geometric realization of conformal blocks for smooth curves as global sections of line bundles on moduli-stacks of principal bundles on the curves (see the review [Sor96] and the references therein). An earlier result of Serre [Ser58, Th´eor`eme 1] (also see [Ati57, Theorem 2]) implies that this triviality property is true if G “ SLprq, and C is a possibly singular affine curve over an arbitrary field k. -
Arxiv:1310.3297V1 [Math.AG] 11 Oct 2013 Bertini for Macaulay2
Bertini for Macaulay2 Daniel J. Bates,∗ Elizabeth Gross,† Anton Leykin,‡ Jose Israel Rodriguez§ September 6, 2018 Abstract Numerical algebraic geometry is the field of computational mathematics concerning the numerical solution of polynomial systems of equations. Bertini, a popular software package for computational applications of this field, includes implementations of a variety of algorithms based on polynomial homotopy continuation. The Macaulay2 package Bertini provides an interface to Bertini, making it possible to access the core run modes of Bertini in Macaulay2. With these run modes, users can find approximate solutions to zero-dimensional systems and positive-dimensional systems, test numerically whether a point lies on a variety, sample numerically from a variety, and perform parameter homotopy runs. 1 Numerical algebraic geometry Numerical algebraic geometry (numerical AG) refers to a set of methods for finding and manipulating the solution sets of systems of polynomial equations. Said differently, given f : CN → Cn, numerical algebraic geometry provides facilities for computing numerical approximations to isolated solutions of V (f) = z ∈ CN |f(z)=0 , as well as numerical approximations to generic points on positive-dimensional components. The book [7] provides a good introduction to the field, while the newer book [2] provides a simpler introduction as well as a complete manual for the software package Bertini [1]. arXiv:1310.3297v1 [math.AG] 11 Oct 2013 Bertini is a free, open source software package for computations in numerical alge- braic geometry. The purpose of this article is to present a Macaulay2 [3] package Bertini that provides an interface to Bertini. This package uses basic datatypes and service rou- tines for computations in numerical AG provided by the package NAGtypes. -
Virtual Knot Invariants Arising from Parities
Virtual Knot Invariants Arising From Parities Denis Petrovich Ilyutko Department of Mechanics and Mathematics, Moscow State University, Russia [email protected] Vassily Olegovich Manturov Faculty of Science, People’s Friendship University of Russia, Russia [email protected] Igor Mikhailovich Nikonov Department of Mechanics and Mathematics, Moscow State University, Russia [email protected] Abstract In [12, 15] it was shown that in some knot theories the crucial role is played by parity, i.e. a function on crossings valued in {0, 1} and behaving nicely with respect to Reidemeister moves. Any parity allows one to construct functorial mappings from knots to knots, to refine many invariants and to prove minimality theorems for knots. In the present paper, we generalise the notion of parity and construct parities with coefficients from an abelian group rather than Z2 and investigate them for different knot theories. For some knot theories we arXiv:1102.5081v1 [math.GT] 24 Feb 2011 show that there is the universal parity, i.e. such a parity that any other parity factors through it. We realise that in the case of flat knots all parities originate from homology groups of underlying surfaces and, at the same time, allow one to “localise” the global homological information about the ambient space at crossings. We prove that there is only one non-trivial parity for free knots, the Gaussian parity. At the end of the paper we analyse the behaviour of some invariants constructed for some modifications of parities. 1 Contents 1 Introduction 2 2 Basic definitions 3 2.1 Framed 4-graphs and chord diagrams . -
Triviality Results and the Relationship Between Logical and Natural
Triviality Results and the Relationship between Logical and Natural Languages Justin Khoo Massachusetts Institute of Technology [email protected] Matthew Mandelkern All Souls College, Oxford [email protected] Inquiry into the meaning of logical terms in natural language (‘and’, ‘or’, ‘not’, ‘if’) has generally proceeded along two dimensions. On the one hand, semantic theories aim to predict native speaker intuitions about the natural language sentences involving those logical terms. On the other hand, logical theories explore the formal properties of the translations of those terms into formal languages. Sometimes these two lines of inquiry appear to be in tension: for instance, our best logical investigation into conditional connectives may show that there is no conditional operator that has all the properties native speaker intuitions suggest ‘if’ has. Indicative conditionals have famously been the source of one such tension, ever since the triviality proofs of both Lewis (1976) and Gibbard (1981) established conclusions which are prima facie in tension with ordinary judgements about natural language indicative conditionals. In a recent series of papers, Branden Fitelson (2013, 2015, 2016) has strengthened both triviality results, revealing a common culprit: a logical schema known as IMPORT-EXPORT. Fitelson’s results focus the tension between the logical results and ordinary judgements, since IMPORT-EXPORT seems to be supported by intuitions about natural language. In this paper, we argue that the intuitions which have been taken to support IMPORT-EXPORT are really evidence for a closely related but subtly different principle. We show that the two principles are independent by showing how, given a standard assumption about the conditional operator in the formal language in which IMPORT- EXPORT is stated, many existing theories of indicative conditionals validate one but not the other. -
PARITY of the PARTITION FUNCTION 1. Introduction And
PARITY OF THE PARTITION FUNCTION KEN ONO Abstract. Although much is known about the partition function, little is known about its parity. For the polynomials D(x) := (Dx2 + 1)=24, where D ≡ 23 (mod 24), we show that there are infinitely many m (resp. n) for which p(D(m)) is even (resp. p(D(n)) is odd) if there is at least one such m (resp. n). We bound the first m and n (if any) in terms of the class number h(−D). For prime D we show that there are indeed infinitely many even values. To this end we construct new modular generating functions using generalized Borcherds products, and we employ Galois representations and locally nilpotent Hecke algebras. 1. Introduction and statement of results A partition of a non-negative integer n is a non-increasing sequence of positive integers that sum to n. Ramanujan investigated [43, 44] p(n), the number of partitions of n, and he discovered congruences in certain very special arithmetic progressions such as: p(5n + 4) ≡ 0 (mod 5); (1.1) p(7n + 5) ≡ 0 (mod 7); p(11n + 6) ≡ 0 (mod 11): Ramanujan's congruences have inspired many works (for example, see [2, 3, 4, 5, 6, 7, 8, 9, 15, 19, 20, 24, 26, 28, 31, 32, 39, 51] to name a few). Atkin [6] and Watson [51] notably proved Ramanujan's conjectures concerning congruences mod powers of 5, 7 and 11, while Andrews and Garvan unearthed [5] Dyson's [19] elusive crank, thereby providing a procedure for dividing the partitions into 5, 7, and 11 groups of equal size in (1.1). -
BEYOND CALCULUS Math21a, O
5/7/2004 CALCULUS BEYOND CALCULUS Math21a, O. Knill DISCRETE SPACE CALCULUS. Many ideas in calculus make sense in a discrete setup, where space is a graph, curves are curves in the graph and surfaces are collections of "plaquettes", polygons formed by edges of the graph. One can look at functions on this graph. Scalar functions are functions defined on the vertices of the INTRODUCTION. Topics beyond multi-variable calculus are usually labeled with special names like "linear graphs. Vector fields are functions defined on the edges, other vector fields are defined as functions defined on algebra", "ordinary differential equations", "numerical analysis", "partial differential equations", "functional plaquettes. The gradient is a function defined on an edge as the difference between the values of f at the end analysis" or "complex analysis". Where one would draw the line between calculus and non-calculus topics is points. not clear but if calculus is about learning the basics of limits, differentiation, integration and summation, then Consider a network modeled by a planar graph which forms triangles. A scalar function assigns a value f multi-variable calculus is the "black belt" of calculus. Are there other ways to play this sport? n to each node n. An area function assigns values fT to each triangle T . A vector field assign values Fnm to each edge connecting node n with node m. The gradient of a scalar function is the vector field Fnm = fn fm. HOW WOULD ALIENS COMPUTE? On an other planet, calculus might be taught in a completely different − The curl of a vector field F is attaches to each triangle (k; m; n) the value curl(F )kmn = Fkm + Fmn + Fnk.