Linear and Complex Analysis for Applications John P. D'angelo
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The Integral Geometry of Line Complexes and a Theorem of Gelfand-Graev Astérisque, Tome S131 (1985), P
Astérisque VICTOR GUILLEMIN The integral geometry of line complexes and a theorem of Gelfand-Graev Astérisque, tome S131 (1985), p. 135-149 <http://www.numdam.org/item?id=AST_1985__S131__135_0> © Société mathématique de France, 1985, tous droits réservés. L’accès aux archives de la collection « Astérisque » (http://smf4.emath.fr/ Publications/Asterisque/) implique l’accord avec les conditions générales d’uti- lisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Société Mathématique de France Astérisque, hors série, 1985, p. 135-149 THE INTEGRAL GEOMETRY OF LINE COMPLEXES AND A THEOREM OF GELFAND-GRAEV BY Victor GUILLEMIN 1. Introduction Let P = CP3 be the complex three-dimensional projective space and let G = CG(2,4) be the Grassmannian of complex two-dimensional subspaces of C4. To each point p E G corresponds a complex line lp in P. Given a smooth function, /, on P we will show in § 2 how to define properly the line integral, (1.1) f(\)d\ d\. = f(p). d A complex hypersurface, 5, in G is called admissible if there exists no smooth function, /, which is not identically zero but for which the line integrals, (1,1) are zero for all p G 5. In other words if S is admissible, then, in principle, / can be determined by its integrals over the lines, Zp, p G 5. In the 60's GELFAND and GRAEV settled the problem of characterizing which subvarieties, 5, of G have this property. -
CR Singular Immersions of Complex Projective Spaces
Beitr¨agezur Algebra und Geometrie Contributions to Algebra and Geometry Volume 43 (2002), No. 2, 451-477. CR Singular Immersions of Complex Projective Spaces Adam Coffman∗ Department of Mathematical Sciences Indiana University Purdue University Fort Wayne Fort Wayne, IN 46805-1499 e-mail: Coff[email protected] Abstract. Quadratically parametrized smooth maps from one complex projective space to another are constructed as projections of the Segre map of the complexifi- cation. A classification theorem relates equivalence classes of projections to congru- ence classes of matrix pencils. Maps from the 2-sphere to the complex projective plane, which generalize stereographic projection, and immersions of the complex projective plane in four and five complex dimensions, are considered in detail. Of particular interest are the CR singular points in the image. MSC 2000: 14E05, 14P05, 15A22, 32S20, 32V40 1. Introduction It was shown by [23] that the complex projective plane CP 2 can be embedded in R7. An example of such an embedding, where R7 is considered as a subspace of C4, and CP 2 has complex homogeneous coordinates [z1 : z2 : z3], was given by the following parametric map: 1 2 2 [z1 : z2 : z3] 7→ 2 2 2 (z2z¯3, z3z¯1, z1z¯2, |z1| − |z2| ). |z1| + |z2| + |z3| Another parametric map of a similar form embeds the complex projective line CP 1 in R3 ⊆ C2: 1 2 2 [z0 : z1] 7→ 2 2 (2¯z0z1, |z1| − |z0| ). |z0| + |z1| ∗The author’s research was supported in part by a 1999 IPFW Summer Faculty Research Grant. 0138-4821/93 $ 2.50 c 2002 Heldermann Verlag 452 Adam Coffman: CR Singular Immersions of Complex Projective Spaces This may look more familiar when restricted to an affine neighborhood, [z0 : z1] = (1, z) = (1, x + iy), so the set of complex numbers is mapped to the unit sphere: 2x 2y |z|2 − 1 z 7→ ( , , ), 1 + |z|2 1 + |z|2 1 + |z|2 and the “point at infinity”, [0 : 1], is mapped to the point (0, 0, 1) ∈ R3. -
An Introduction to Complex Analysis and Geometry John P. D'angelo
An Introduction to Complex Analysis and Geometry John P. D'Angelo Dept. of Mathematics, Univ. of Illinois, 1409 W. Green St., Urbana IL 61801 [email protected] 1 2 c 2009 by John P. D'Angelo Contents Chapter 1. From the real numbers to the complex numbers 11 1. Introduction 11 2. Number systems 11 3. Inequalities and ordered fields 16 4. The complex numbers 24 5. Alternative definitions of C 26 6. A glimpse at metric spaces 30 Chapter 2. Complex numbers 35 1. Complex conjugation 35 2. Existence of square roots 37 3. Limits 39 4. Convergent infinite series 41 5. Uniform convergence and consequences 44 6. The unit circle and trigonometry 50 7. The geometry of addition and multiplication 53 8. Logarithms 54 Chapter 3. Complex numbers and geometry 59 1. Lines, circles, and balls 59 2. Analytic geometry 62 3. Quadratic polynomials 63 4. Linear fractional transformations 69 5. The Riemann sphere 73 Chapter 4. Power series expansions 75 1. Geometric series 75 2. The radius of convergence 78 3. Generating functions 80 4. Fibonacci numbers 82 5. An application of power series 85 6. Rationality 87 Chapter 5. Complex differentiation 91 1. Definitions of complex analytic function 91 2. Complex differentiation 92 3. The Cauchy-Riemann equations 94 4. Orthogonal trajectories and harmonic functions 97 5. A glimpse at harmonic functions 98 6. What is a differential form? 103 3 4 CONTENTS Chapter 6. Complex integration 107 1. Complex-valued functions 107 2. Line integrals 109 3. Goursat's proof 116 4. The Cauchy integral formula 119 5. -
Math 311 - Introduction to Proof and Abstract Mathematics Group Assignment # 15 Name: Due: at the End of Class on Tuesday, March 26Th
Math 311 - Introduction to Proof and Abstract Mathematics Group Assignment # 15 Name: Due: At the end of class on Tuesday, March 26th More on Functions: Definition 5.1.7: Let A, B, C, and D be sets. Let f : A B and g : C D be functions. Then f = g if: → → A = C and B = D • For all x A, f(x)= g(x). • ∈ Intuitively speaking, this definition tells us that a function is determined by its underlying correspondence, not its specific formula or rule. Another way to think of this is that a function is determined by the set of points that occur on its graph. 1. Give a specific example of two functions that are defined by different rules (or formulas) but that are equal as functions. 2. Consider the functions f(x)= x and g(x)= √x2. Find: (a) A domain for which these functions are equal. (b) A domain for which these functions are not equal. Definition 5.1.9 Let X be a set. The identity function on X is the function IX : X X defined by, for all x X, → ∈ IX (x)= x. 3. Let f(x)= x cos(2πx). Prove that f(x) is the identity function when X = Z but not when X = R. Definition 5.1.10 Let n Z with n 0, and let a0,a1, ,an R such that an = 0. The function p : R R is a ∈ ≥ ··· ∈ 6 n n−1 → polynomial of degree n with real coefficients a0,a1, ,an if for all x R, p(x)= anx +an−1x + +a1x+a0. -
Complex Algebraic Geometry
Complex Algebraic Geometry Jean Gallier∗ and Stephen S. Shatz∗∗ ∗Department of Computer and Information Science University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] ∗∗Department of Mathematics University of Pennsylvania Philadelphia, PA 19104, USA e-mail: [email protected] February 25, 2011 2 Contents 1 Complex Algebraic Varieties; Elementary Theory 7 1.1 What is Geometry & What is Complex Algebraic Geometry? . .......... 7 1.2 LocalStructureofComplexVarieties. ............ 14 1.3 LocalStructureofComplexVarieties,II . ............. 28 1.4 Elementary Global Theory of Varieties . ........... 42 2 Cohomologyof(Mostly)ConstantSheavesandHodgeTheory 73 2.1 RealandComplex .................................... ...... 73 2.2 Cohomology,deRham,Dolbeault. ......... 78 2.3 Hodge I, Analytic Preliminaries . ........ 89 2.4 Hodge II, Globalization & Proof of Hodge’s Theorem . ............ 107 2.5 HodgeIII,TheK¨ahlerCase . .......... 131 2.6 Hodge IV: Lefschetz Decomposition & the Hard Lefschetz Theorem............... 147 2.7 ExtensionsofResultstoVectorBundles . ............ 162 3 The Hirzebruch-Riemann-Roch Theorem 165 3.1 Line Bundles, Vector Bundles, Divisors . ........... 165 3.2 ChernClassesandSegreClasses . .......... 179 3.3 The L-GenusandtheToddGenus .............................. 215 3.4 CobordismandtheSignatureTheorem. ........... 227 3.5 The Hirzebruch–Riemann–Roch Theorem (HRR) . ............ 232 3 4 CONTENTS Preface This manuscript is based on lectures given by Steve Shatz for the course Math 622/623–Complex Algebraic Geometry, during Fall 2003 and Spring 2004. The process for producing this manuscript was the following: I (Jean Gallier) took notes and transcribed them in LATEX at the end of every week. A week later or so, Steve reviewed these notes and made changes and corrections. After the course was over, Steve wrote up additional material that I transcribed into LATEX. The following manuscript is thus unfinished and should be considered as work in progress. -
1 Monoids and Groups
1 Monoids and groups 1.1 Definition. A monoid is a set M together with a map M × M ! M; (x; y) 7! x · y such that (i) (x · y) · z = x · (y · z) 8x; y; z 2 M (associativity); (ii) 9e 2 M such that x · e = e · x = x for all x 2 M (e = the identity element of M). 1.2 Examples. 1) Z with addition of integers (e = 0) 2) Z with multiplication of integers (e = 1) 3) Mn(R) = fthe set of all n × n matrices with coefficients in Rg with ma- trix multiplication (e = I = the identity matrix) 4) U = any set P (U) := fthe set of all subsets of Ug P (U) is a monoid with A · B := A [ B and e = ?. 5) Let U = any set F (U) := fthe set of all functions f : U ! Ug F (U) is a monoid with multiplication given by composition of functions (e = idU = the identity function). 1.3 Definition. A monoid is commutative if x · y = y · x for all x; y 2 M. 1.4 Example. Monoids 1), 2), 4) in 1.2 are commutative; 3), 5) are not. 1 1.5 Note. Associativity implies that for x1; : : : ; xk 2 M the expression x1 · x2 ····· xk has the same value regardless how we place parentheses within it; e.g.: (x1 · x2) · (x3 · x4) = ((x1 · x2) · x3) · x4 = x1 · ((x2 · x3) · x4) etc. 1.6 Note. A monoid has only one identity element: if e; e0 2 M are identity elements then e = e · e0 = e0 1.7 Definition. -
Ishikawa-Oyama.Pdf
Proc. of 15th International Workshop Journal of Singularities on Singularities, Sao˜ Carlos, 2018 Volume 22 (2020), 373-384 DOI: 10.5427/jsing.2020.22v TOPOLOGY OF COMPLEMENTS TO REAL AFFINE SPACE LINE ARRANGEMENTS GOO ISHIKAWA AND MOTOKI OYAMA ABSTRACT. It is shown that the diffeomorphism type of the complement to a real space line arrangement in any dimensional affine ambient space is determined only by the number of lines and the data on multiple points. 1. INTRODUCTION Let A = f`1;`2;:::;`dg be a real space line arrangement, or a configuration, consisting of affine 3 d d-lines in R . The different lines `i;` j(i 6= j) may intersect, so that the union [i=1`i is an affine real algebraic curve of degree d in R3 possibly with multiple points. In this paper we determine the topological 3 d type of the complement M(A ) := R n([i=1`i) of A , which is an open 3-manifold. We observe that the topological type M(A ) is determined only by the number of lines and the data on multiple points of A . Moreover we determine the diffeomorphism type of M(A ). n n i j i j Set D := fx 2 R j kxk ≤ 1g, the n-dimensional closed disk. The pair (D × D ;D × ¶(D )) with i + j = n; 0 ≤ i;0 ≤ j, is called an n-dimensional handle of index j (see [17][1] for instance). Now take one D3 and, for any non-negative integer g, attach to it g-number of 3-dimensional handles 2 1 2 1 (Dk × Dk;Dk × ¶(Dk)) of index 1 (1 ≤ k ≤ g), by an attaching embedding g G 2 1 3 2 j : (Dk × ¶(Dk)) ! ¶(D ) = S k=1 such that the obtained 3-manifold 3 S Fg 2 1 Bg := D j ( k=1(Dk × Dk)) is orientable. -
Lecture 3 Partially Ordered Sets
Lecture 3 Partially ordered sets Now for something totally different. In life, useful sets are rarely “just” sets. They often come with additional structure. For example, R isn’t useful just because it’s some set. It’s useful because we can add its elements, multiply its elements, and even compare its elements. If A is, for example, the set of all bananas and apples on earth, it’s not as natural to do any of these things with elements of A. Today, we’ll talk about a structure called a partial order. 3.1 Preliminaries First, let me remind you of something called the Cartesian product, or direct product of sets. Definition 3.1.1. Let A and B be sets. Then the Cartesian product of A and B is defined to be the set consisting of all pairs (a, b) where a A and œ b B. We denote the Cartesian product by œ A B. ◊ Example 3.1.2. R2 is the Cartesian product R R. ◊ Example 3.1.3. Let T be the set of all t-shirts in Hiro’s closet, and S the set of all shorts in Hiro’s closet. Then S T represents the collection of all ◊ possible outfits Hiro is willing to consider in August. (I.e., Hiro is willing to consider putting on any of his shorts together with any of his t-shirts.) 23 24 LECTURE 3. PARTIALLY ORDERED SETS Note that we can “repeat” the Cartesian product operation, or apply it many times at once. Example 3.1.4. -
Lecture 19: Alternating Group
MATH 433 Applied Algebra Lecture 19: Alternating group. Abstract groups. Sign of a permutation Theorem 1 For any n ≥ 2 there exists a unique function sgn : S(n) → {−1, 1} such that • sgn(πσ)= sgn(π) sgn(σ) for all π, σ ∈ S(n), • sgn(τ)= −1 for any transposition τ in S(n). A permutation π is called even if it is a product of an even number of transpositions, and odd if it is a product of an odd number of transpositions. It turns out that π is even if sgn(π)=1 and odd if sgn(π)= −1. Theorem 2 (i) sgn(πσ)= sgn(π) sgn(σ) for any π, σ ∈ S(n). (ii) sgn(π−1)= sgn(π) for any π ∈ S(n). (iii) sgn(id) = 1. (iv) sgn(τ)= −1 for any transposition τ. (v) sgn(σ)=(−1)r−1 for any cycle σ of length r. Alternating group Given an integer n ≥ 2, the alternating group on n symbols, denoted An or A(n), is the set of all even permutations in the symmetric group S(n). Theorem (i) For any two permutations π, σ ∈ A(n), the product πσ is also in A(n). (ii) The identity function id is in A(n). (iii) For any permutation π ∈ A(n), the inverse π−1 is in A(n). In other words, the product of even permutations is even, the identity function is an even permutation, and the inverse of an even permutation is even. Theorem The alternating group A(n) has n!/2 elements. -
Theoretical Probability and Statistics
Theoretical Probability and Statistics Charles J. Geyer Copyright 1998, 1999, 2000, 2001, 2008 by Charles J. Geyer September 5, 2008 Contents 1 Finite Probability Models 1 1.1 Probability Mass Functions . 1 1.2 Events and Measures . 5 1.3 Random Variables and Expectation . 6 A Greek Letters 9 B Sets and Functions 11 B.1 Sets . 11 B.2 Intervals . 12 B.3 Functions . 12 C Summary of Brand-Name Distributions 14 C.1 The Discrete Uniform Distribution . 14 C.2 The Bernoulli Distribution . 14 i Chapter 1 Finite Probability Models The fundamental idea in probability theory is a probability model, also called a probability distribution. Probability models can be specified in several differ- ent ways • probability mass function (PMF), • probability density function (PDF), • distribution function (DF), • probability measure, and • function mapping from one probability model to another. We will meet probability mass functions and probability measures in this chap- ter, and will meet others later. The terms “probability model” and “probability distribution” don’t indicate how the model is specified, just that it is specified somehow. 1.1 Probability Mass Functions A probability mass function (PMF) is a function pr Ω −−−−→ R which satisfies the following conditions: its values are nonnegative pr(ω) ≥ 0, ω ∈ Ω (1.1a) and sum to one X pr(ω) = 1. (1.1b) ω∈Ω The domain Ω of the PMF is called the sample space of the probability model. The sample space is required to be nonempty in order that (1.1b) make sense. 1 CHAPTER 1. FINITE PROBABILITY MODELS 2 In this chapter we require all sample spaces to be finite sets. -
Linear Algebra I: Vector Spaces A
Linear Algebra I: Vector Spaces A 1 Vector spaces and subspaces 1.1 Let F be a field (in this book, it will always be either the field of reals R or the field of complex numbers C). A vector space V D .V; C; o;˛./.˛2 F// over F is a set V with a binary operation C, a constant o and a collection of unary operations (i.e. maps) ˛ W V ! V labelled by the elements of F, satisfying (V1) .x C y/ C z D x C .y C z/, (V2) x C y D y C x, (V3) 0 x D o, (V4) ˛ .ˇ x/ D .˛ˇ/ x, (V5) 1 x D x, (V6) .˛ C ˇ/ x D ˛ x C ˇ x,and (V7) ˛ .x C y/ D ˛ x C ˛ y. Here, we write ˛ x and we will write also ˛x for the result ˛.x/ of the unary operation ˛ in x. Often, one uses the expression “multiplication of x by ˛”; but it is useful to keep in mind that what we really have is a collection of unary operations (see also 5.1 below). The elements of a vector space are often referred to as vectors. In contrast, the elements of the field F are then often referred to as scalars. In view of this, it is useful to reflect for a moment on the true meaning of the axioms (equalities) above. For instance, (V4), often referred to as the “associative law” in fact states that the composition of the functions V ! V labelled by ˇ; ˛ is labelled by the product ˛ˇ in F, the “distributive law” (V6) states that the (pointwise) sum of the mappings labelled by ˛ and ˇ is labelled by the sum ˛ C ˇ in F, and (V7) states that each of the maps ˛ preserves the sum C. -
Inverse Monoids Associated with the Complexity Class NP
Inverse monoids associated with the complexity class NP J.C. Birget 6 March 2017 Abstract We study the P versus NP problem through properties of functions and monoids, continuing the work of [3]. Here we consider inverse monoids whose properties and relationships determine whether P is different from NP, or whether injective one-way functions (with respect to worst-case complexity) exist. 1 Introduction We give a few definitions before motivating the monoid approach to the P versus NP problem. Some of these notions appeared already in [3]. By function we mean a partial function A∗ → A∗, where A is a finite alphabet (usually, A = {0, 1}), and A∗ denotes the set of all finite strings over A. Let Dom(f) (⊆ A∗) denote the domain of f, i.e., {x ∈ A∗ : f(x) is defined}; and let Im(f) (⊆ A∗) denote the image (or range) of f, i.e., {f(x) : x ∈ ∗ ∗ Dom(f)}. The length of x ∈ A is denoted by |x|. The restriction of f to X ⊆ A is denoted by f|X , and the identity function on X is denoted by idX or id|X . Definition 1.1 (inverse, co-inverse, mutual inverse) A function f ′ is an inverse of a function f iff f ◦ f ′ ◦ f = f. In that case we also say that f is a co-inverse of f ′. If f ′ is both an inverse and a co-inverse of f, we say that f ′ is a mutual inverse of f, or that f ′ and f are mutual inverses (of each other).1 It is easy to see that f ′ is an inverse of f iff for every y ∈ Im(f): f ′(y) is defined and f ′(y) ∈ f −1(y).