Baire Categories, Continuous Functions, and Approximations

Total Page:16

File Type:pdf, Size:1020Kb

Baire Categories, Continuous Functions, and Approximations BAIRE CATEGORIES, CONTINUOUS FUNCTIONS, AND APPROXIMATIONS ANDREW CHEN Abstract. This paper is an exploration into continuous functions and how they can be approximated. We first gain insight into the nature of continuous functions and demonstrate why most continuous functions are nowhere differentiable using the Baire Category Theorem. We then discuss two methods of approximating continuous functions: the first of which is using polynomials via the Weierstrass Approximation Theorem, and the second of which is using neural networks via the Universal Approximation Theorem. Contents 1. Introduction 1 2. Continuous Functions and Differentiability 1 2.1. Introducing the Baire Category Theorem 2 2.2. Applying the Baire Category Theorem to the Set of Continuous Functions 4 3. Weierstrass Approximation Theorem 6 4. The Universal Approximation Theorem 9 Acknowledgments 14 References 15 1. Introduction For many years, it was widely thought by mathematicians that most (if not all) continuous functions are differentiable, due to intuitive notions of continuity and differentiability. While calculus was invented in the late 1600s, the first known example of a non-differentiable continuous function was not discovered until around year 1830, by Bernard Bolzano, and the first published example was not presented until 1872, by Karl Weierstrass [9]. Due to later advances in the field of topology, we now know that most continuous functions are in fact nowhere differentiable. Section 2 will explore a proof of this, which utilizes an important theorem in topology called the Baire Category Theorem. We will then explore methods of approximating continuous functions, even those that are nowhere differentiable. Section 3 will explore a probabilistic proof of the Weierstrass Approximation Theorem, which will show that all continuous functions f : [0; 1] ! R can be approximated arbitrarily well using polynomials. The fourth and final section will then explore the ability of machine learning to approximate continuous functions. The main result is the Universal Approximation Theorem, which states that a feedforward neural network used in machine learning can approximate continuous functions arbitrarily well. 2. Continuous Functions and Differentiability The goal of this section is to use analysis to explore the nature of continuous functions. In particular, we will apply the Baire Category Theorem to the space of real-valued continuous functions C(K) on a compact 1 set K to show that most continuous functions are nowhere differentiable. The definitions in this section can be found in most real analysis textbooks such as [8], and the specific proof presented here was inspired by [5]. 2.1. Introducing the Baire Category Theorem. This section will assume that the reader has a general understanding of metric spaces and their usual topology. As a reminder, a metric space is a set X with some notion of distance between any two elements of the set, given by a distance function d : X × X ! [0; 1) that is symmetric, satisfies the triangle inequality, and has the property that d(x; y) = 0 () x = y. Definition 2.1. For an element p in a metric space X, and a real number r > 0, we define the open ball B(p; r) as B(p; r) = fq 2 X j d(p; q) < rg: Similarly, we define the closed ball B(p; r) as B(p; r) = fq 2 X j d(p; q) ≤ rg: Definition 2.2. A set D is dense in a metric space X if and only if for every element p 2 X and > 0, D \ B(p; ) 6= ?. Alternatively, D is dense in X iff its closure D = X. Example 2.3. The rational numbers Q are dense in the real numbers R. Proof. Between any two real numbers a and b with a < b, there exists a rational number q such that a < q < b. Thus the intersection of the rationals with any open ball in the reals will always be nonempty. ◦ Definition 2.4. A set E is nowhere dense in a metric space X if E = ?. Example 2.5. The integers Z are nowhere dense in the real numbers R. Proof. Z has no limit points, so we know that Z = Z. Then assume for contradiction that the interior of Z is not empty; in other words, assume there exists some nonempty open ball U ⊂ R such that U ⊂ Z. Since Z is countable, U must also be countable. However, this is a contradiction because all open subsets of R are uncountable. Therefore U does not exist, so the interior of Z is empty. Remark 2.6. A set can be not dense, but also not nowhere dense. For example, consider the interval (0; 1) ⊂ R. (0; 1) = [0; 1] 6= R, so (0; 1) is not dense in R. However, [0; 1]◦ is also nonempty in R since it contains (0; 1), so the interval is also not nowhere dense in R. We can see that nowhere dense is a much stronger property than simply being not dense; in a sense, it means a set is not dense everywhere. Lemma 2.7. The complement of a closed nowhere dense set is an open dense set. Proof. Let A be a closed nowhere dense set. X n (A◦) = X n A, but A has empty interior, so X = X n A. Therefore X n A is open and dense. We are ready to state the major result of this section. 1 Theorem 2.8 (Baire Category Theorem). If X is a nonempty complete metric space, and (Gn)n=1 is a T1 countable collection of dense open subsets of X, then n=1 Gn is dense in X. Proof. Let U be an arbitrary open ball in X. Since G1 is dense in X, we know it has nonempty intersection with U. Pick x1 2 G1 \ U and 0 < r1 < 1 such that B(x1; r1) ⊆ G1 \ U. This is possible since both 2 G1 and U are open. Since G2 is dense in X, we know that G2 \ B(x1; r1) is nonempty. We repeat the 1 same process, picking x2 2 G2 \ B(x1; r1) and 0 < r2 < 2 such that B(x2; r2) ⊆ G2 \ B(x1; r1). Since every Gn is dense, we continue repeating the process to get a nested sequence of closed balls, such that 1 B(xn; rn) ⊆ Gn \ B(xn−1; rn−1), and 0 < rn < n . Note that xn 2 B(xm; rn) for all n > m, or in other 1 1 words, jxm − xnj < rn < n . Thus, for any > 0, there exists N 2 N such that N < , and for n; m ≥ N, jxm − xnj < rn < . Since X is a complete metric space, xn ! x 2 X as n ! 1, for some x. By definition of closure, we know that x 2 B(xn; rn). Since our sequence of balls is nested, and B(xn; rn) ⊆ Gn, we know that x 2 Gn for all n. Additionally, since B(x1; r1) ⊆ U, we know that x 2 U. Therefore, we have shown T T that ( Gn) \ U contains x and is thus nonempty. Since U is arbitrary, we have shown that Gn is dense in X. To understand why this is called the Baire Category Theorem, we introduce the following definition. Definition 2.9. In a metric space X, a set E ⊆ X is called meager if E can be written as a countable union of nowhere dense sets: 1 [ E = En; n=1 where each En is nowhere dense. Meager sets are also known as first category. E is called non-meager, or second category, if it is not first category. Two important properties of meager sets are that a subset of a meager set is also meager, and the union of meager sets is also meager. Remark 2.10. The usage of the word \category" in this context is unrelated to category theory. Corollary 2.11. If X is a nonempty complete metric space, then X is non-meager in itself. Proof. Let fEig be an arbitrary countable collection of closed nowhere dense subsets of X. Then by Lemma T 2.7, Vi = X nEi is an open dense subset of X for every i. By Theorem 2.8, i Vi is dense in X and nonempty. T S S T Since i Vi is disjoint with i Ei, we know that X 6= i Ei since there are elements in i Vi ⊂ X that are S not in i Ei. If fEig is instead an arbitrary countable collection of open nowhere dense subsets of X, then S each Ei must be the empty set, and thus i Ei = ? 6= X. Therefore, X cannot be written as a countable union of nowhere dense subsets. Example 2.12. Z and Q are meager in R, but the set of irrationals R n Q is non-meager in R. Proof. Z and Q are both countable, so they can be expressed as the countable union of singleton sets. Singleton sets are nowhere dense in R, so Z and Q are meager in R. Assume for contradiction R n Q is also meager in R. Then Q [ (R n Q) = R is meager in R, but R is non-meager by Corollary 2.11, so our assumption is false and R n Q is non-meager. Remark 2.13. This example helps show why we can think of meager sets as being small relative to non- meager sets in the same topological space. However, it is important to note that not all non-meager sets are of the same \size", and that meagerness and non-meagerness have nothing to do with the \absolute" or \objective" size of a set.
Recommended publications
  • The Linear Algebra Version of the Chain Rule 1
    Ralph M Kaufmann The Linear Algebra Version of the Chain Rule 1 Idea The differential of a differentiable function at a point gives a good linear approximation of the function – by definition. This means that locally one can just regard linear functions. The algebra of linear functions is best described in terms of linear algebra, i.e. vectors and matrices. Now, in terms of matrices the concatenation of linear functions is the matrix product. Putting these observations together gives the formulation of the chain rule as the Theorem that the linearization of the concatenations of two functions at a point is given by the concatenation of the respective linearizations. Or in other words that matrix describing the linearization of the concatenation is the product of the two matrices describing the linearizations of the two functions. 1. Linear Maps Let V n be the space of n–dimensional vectors. 1.1. Definition. A linear map F : V n → V m is a rule that associates to each n–dimensional vector ~x = hx1, . xni an m–dimensional vector F (~x) = ~y = hy1, . , yni = hf1(~x),..., (fm(~x))i in such a way that: 1) For c ∈ R : F (c~x) = cF (~x) 2) For any two n–dimensional vectors ~x and ~x0: F (~x + ~x0) = F (~x) + F (~x0) If m = 1 such a map is called a linear function. Note that the component functions f1, . , fm are all linear functions. 1.2. Examples. 1) m=1, n=3: all linear functions are of the form y = ax1 + bx2 + cx3 for some a, b, c ∈ R.
    [Show full text]
  • Characterization of Non-Differentiable Points in a Function by Fractional Derivative of Jumarrie Type
    Characterization of non-differentiable points in a function by Fractional derivative of Jumarrie type Uttam Ghosh (1), Srijan Sengupta(2), Susmita Sarkar (2), Shantanu Das (3) (1): Department of Mathematics, Nabadwip Vidyasagar College, Nabadwip, Nadia, West Bengal, India; Email: [email protected] (2):Department of Applied Mathematics, Calcutta University, Kolkata, India Email: [email protected] (3)Scientist H+, RCSDS, BARC Mumbai India Senior Research Professor, Dept. of Physics, Jadavpur University Kolkata Adjunct Professor. DIAT-Pune Ex-UGC Visiting Fellow Dept. of Applied Mathematics, Calcutta University, Kolkata India Email (3): [email protected] The Birth of fractional calculus from the question raised in the year 1695 by Marquis de L'Hopital to Gottfried Wilhelm Leibniz, which sought the meaning of Leibniz's notation for the derivative of order N when N = 1/2. Leibnitz responses it is an apparent paradox from which one day useful consequences will be drown. Abstract There are many functions which are continuous everywhere but not differentiable at some points, like in physical systems of ECG, EEG plots, and cracks pattern and for several other phenomena. Using classical calculus those functions cannot be characterized-especially at the non- differentiable points. To characterize those functions the concept of Fractional Derivative is used. From the analysis it is established that though those functions are unreachable at the non- differentiable points, in classical sense but can be characterized using Fractional derivative. In this paper we demonstrate use of modified Riemann-Liouvelli derivative by Jumarrie to calculate the fractional derivatives of the non-differentiable points of a function, which may be one step to characterize and distinguish and compare several non-differentiable points in a system or across the systems.
    [Show full text]
  • 1 Think About a Linear Function and Its First and Second Derivative The
    Think about a linear function and its first and second derivative The second derivative of a linear function always equals 0 Anytime you are trying to find the limit of a piecewise function, find the limit approaching from the left and right ­ if they are equal then the limit exists Remember you can't differentiate at a vertical tangent line Differentiabilty implies continuity ­ the graph isn't continuous at x = 0 1 To find the velocity, take the first derivative of the position function. To find where the velocity equals zero, set the first derivative equal to zero 2 From the graph, we know that f (1) = 0; Since the graph is increasing, we know that f '(1) is positive; since the graph is concave down, we know that f ''(1) is negative Possible points of inflection ­ need to set up a table to see where concavity changes (that verifies points of inflection) (­∞, ­1) (­1, 0) (0, 2) (2, ∞) + ­ + + concave up concave down concave up concave up Since the concavity changes when x = ­1 and when x = 0, they are points of inflection. x = 2 is not a point of inflection 3 We need to find the derivative, find the critical numbers and use them in the first derivative test to find where f (x) is increasing and decreasing (­∞, 0) (0, ∞) ­ + Decreasing Increasing 4 This is the graph of y = cos x, shifted right (A) and (C) are the only graphs of sin x, and (A) is the graph of ­sin x, which reflects across the x­axis 5 Take the derivative of the velocity function to find the acceleration function There are no critical numbers, because v '(t) doesn't ever equal zero (you can verify this by graphing v '(t) ­ there are no x­intercepts).
    [Show full text]
  • Algebra Vocabulary List (Definitions for Middle School Teachers)
    Algebra Vocabulary List (Definitions for Middle School Teachers) A Absolute Value Function – The absolute value of a real number x, x is ⎧ xifx≥ 0 x = ⎨ ⎩−<xifx 0 http://www.math.tamu.edu/~stecher/171/F02/absoluteValueFunction.pdf Algebra Lab Gear – a set of manipulatives that are designed to represent polynomial expressions. The set includes representations for positive/negative 1, 5, 25, x, 5x, y, 5y, xy, x2, y2, x3, y3, x2y, xy2. The manipulatives can be used to model addition, subtraction, multiplication, division, and factoring of polynomials. They can also be used to model how to solve linear equations. o For more info: http://www.stlcc.cc.mo.us/mcdocs/dept/math/homl/manip.htm http://www.awl.ca/school/math/mr/alg/ss/series/algsrtxt.html http://www.picciotto.org/math-ed/manipulatives/lab-gear.html Algebra Tiles – a set of manipulatives that are designed for modeling algebraic expressions visually. Each tile is a geometric model of a term. The set includes representations for positive/negative 1, x, and x2. The manipulatives can be used to model addition, subtraction, multiplication, division, and factoring of polynomials. They can also be used to model how to solve linear equations. o For more info: http://math.buffalostate.edu/~it/Materials/MatLinks/tilelinks.html http://plato.acadiau.ca/courses/educ/reid/Virtual-manipulatives/tiles/tiles.html Algebraic Expression – a number, variable, or combination of the two connected by some mathematical operation like addition, subtraction, multiplication, division, exponents and/or roots. o For more info: http://www.wtamu.edu/academic/anns/mps/math/mathlab/beg_algebra/beg_alg_tut11 _simp.htm http://www.math.com/school/subject2/lessons/S2U1L1DP.html Area Under the Curve – suppose the curve y=f(x) lies above the x axis for all x in [a, b].
    [Show full text]
  • Generic Continuous Functions and Other Strange Functions in Classical Real Analysis
    Georgia State University ScholarWorks @ Georgia State University Mathematics Theses Department of Mathematics and Statistics 4-17-2008 Generic Continuous Functions and other Strange Functions in Classical Real Analysis Douglas Albert Woolley Follow this and additional works at: https://scholarworks.gsu.edu/math_theses Part of the Mathematics Commons Recommended Citation Woolley, Douglas Albert, "Generic Continuous Functions and other Strange Functions in Classical Real Analysis." Thesis, Georgia State University, 2008. https://scholarworks.gsu.edu/math_theses/44 This Thesis is brought to you for free and open access by the Department of Mathematics and Statistics at ScholarWorks @ Georgia State University. It has been accepted for inclusion in Mathematics Theses by an authorized administrator of ScholarWorks @ Georgia State University. For more information, please contact [email protected]. GENERIC CONTINUOUS FUNCTIONS AND OTHER STRANGE FUNCTIONS IN CLASSICAL REAL ANALYSIS by Douglas A. Woolley Under the direction of Mihaly Bakonyi ABSTRACT In this paper we examine continuous functions which on the surface seem to defy well-known mathematical principles. Before describing these functions, we introduce the Baire Cate- gory theorem and the Cantor set, which are critical in describing some of the functions and counterexamples. We then describe generic continuous functions, which are nowhere differ- entiable and monotone on no interval, and we include an example of such a function. We then construct a more conceptually challenging function, one which is everywhere differen- tiable but monotone on no interval. We also examine the Cantor function, a nonconstant continuous function with a zero derivative almost everywhere. The final section deals with products of derivatives. INDEX WORDS: Baire, Cantor, Generic Functions, Nowhere Differentiable GENERIC CONTINUOUS FUNCTIONS AND OTHER STRANGE FUNCTIONS IN CLASSICAL REAL ANALYSIS by Douglas A.
    [Show full text]
  • Chapter 3. Linearization and Gradient Equation Fx(X, Y) = Fxx(X, Y)
    Oliver Knill, Harvard Summer School, 2010 An equation for an unknown function f(x, y) which involves partial derivatives with respect to at least two variables is called a partial differential equation. If only the derivative with respect to one variable appears, it is called an ordinary differential equation. Examples of partial differential equations are the wave equation fxx(x, y) = fyy(x, y) and the heat Chapter 3. Linearization and Gradient equation fx(x, y) = fxx(x, y). An other example is the Laplace equation fxx + fyy = 0 or the advection equation ft = fx. Paul Dirac once said: ”A great deal of my work is just playing with equations and see- Section 3.1: Partial derivatives and partial differential equations ing what they give. I don’t suppose that applies so much to other physicists; I think it’s a peculiarity of myself that I like to play about with equations, just looking for beautiful ∂ mathematical relations If f(x, y) is a function of two variables, then ∂x f(x, y) is defined as the derivative of the function which maybe don’t have any physical meaning at all. Sometimes g(x) = f(x, y), where y is considered a constant. It is called partial derivative of f with they do.” Dirac discovered a PDE describing the electron which is consistent both with quan- respect to x. The partial derivative with respect to y is defined similarly. tum theory and special relativity. This won him the Nobel Prize in 1933. Dirac’s equation could have two solutions, one for an electron with positive energy, and one for an electron with ∂ antiparticle One also uses the short hand notation fx(x, y)= ∂x f(x, y).
    [Show full text]
  • 1 Uniform Continuity
    Math 0450 Honors intro to analysis Spring, 2009 Notes 17 1 Uniform continuity Read rst: 5.4 Here are some examples of continuous functions, some of which we have done before. 1. A = (0; 1]; f : A R given by f (x) = 1 . ! x Proof. To prove that f is continuous at c (0; 1], suppose that " > 0, and 2 2 let = min c ; c " : If x c < , then rst of all, x > c and so 0 < 1 < 2 . 2 2 j j 2 x c Hence, n o 1 1 c x 1 1 2 1 c2" = = c x < = ": x c xc x c j j c c 2 2. f : R R given by f (x) = x2: ! Proof. Observe that x2 c2 = x c (x + c) : j j j j " If c = 0; let = p": If c = 0; let = min c ; 2 c If c = 0 and x c < , 6 j j j j j j then x < p" and x2 c2 = x2 < ", Ifnc = 0; theno j j j j j j 6 " x2 c2 = x + c x c < 2 c = ": j j j j j j 2 c j j 3. A = [1; ); f (x) = 1 . 1 x Proof. This makes use of item 1 above. Suppose that c A. From item 1, 2 2 we see that if " > 0, and x c < min c ; c " , then 1 1 < ". Hence, j j 2 2 x c 2 let = " : If x c < , and x and c aren in A, theno x c < min c ; c " ; so 2 j j j j 2 2 1 1 < ": n o x c 1 1 4.
    [Show full text]
  • Section 14.4 Tangent Planes and Linear Approximations
    Section 14.4 Tangent planes and linear approximations. Tangent planes. • Suppose a surface S has equation z = f(x, y), where f has continuous first partial derivatives, and let P (x0,y0,z0) be a point on S. • Let C1 and C2 be the curves obtained by intersecting the vertical planes y = y0 and x = x0 with the surface S. P lies on both C1 and C2. • Let T1 and T2 be the tangent lines to the curves C1 and C2 at the point P . • The tangent plane to the surface S at the point P is defined to be the plane that containts both of the tangent lines T1 and T2. An equation on the tangent plane to the surface z = f(x, y) at the point P (x0,y0,z0) is z − z0 = fx(x0,y0)(x − x0)+ fy(x0,y0)(y − y0) Example 1. Find the equation of the tangent plane to the surface z = ln(2x + y) at the point (−1, 3, 0). 1 Linear Approximations. An equation of a tangent plane to the graph of the function f of two variables at the point (a,b,f(a,b)) is z = f(a,b)+ fx(a,b)(x − a)+ fy(a,b)(y − b) The linear function L(x, y)= f(a,b)+ fx(a,b)(x − a)+ fy(a,b)(y − b) is called the linearization of f(a,b) and the approximation f(x, y) ≈ f(a,b)+ fx(a,b)(x − a)+ fy(a,b)(y − b) is called the linear approximation ot the tangent line approximation of f at (a,b).
    [Show full text]
  • Multivariate Approximation and Matrix Calculus
    Multivariate Approximation and Matrix Calculus Introduction Taylor series is a representation of a function as an infinite sum of terms that are calculated from the values of the function's derivatives at a single point. Any finite number of initial terms of the Taylor series of a function is called a Taylor polynomial. In single variable calculus, Taylor polynomial of n degrees is used to approximate an (n+1)-order differentiable function and the error of the approximation can be estimated by the (n+1)-th term of the Taylor series. By introducing vector and matrix calculus notations, we can express the same idea for multivariate functions and vector functions. Applications Because all numbers that can be represented by finite digits are rational numbers, the numerical computation of an irrational function at a particular point is almost always approximated. The first order and second order of Taylor polynomials are most frequently selected as the proper rational function to approximate irrational functions. This idea is called linear and quadratic approximation in calculus, respectively. In addition, the quadratic approximation is also used to in optimization because local maximum or minimum occurs at the critical points where the second term (first derivatives) of the Taylor polynomial is zero and the third term (second derivatives) are definitely positive or negative. In order to obtain the first or second order Taylor polynomial, we compute the coefficients of Taylor series by calculating the first and second derivatives of the original function. When we move towards the advanced mathematical applications (temperature in 4 dimensional temporal-spatial space and vector field of moving hurricane centers), we need to use multivariate (vector) functions, instead of single variable functions.
    [Show full text]
  • Convergent Factorial Series Solutions of Linear Difference Equations*
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF DIFFERENTIAL EQUATIONS 29, 345-361 (1978) Convergent Factorial Series Solutions of Linear Difference Equations* W. J. FITZPATRICK+ AND L. J. GRIMM Depal-tment of Mathematics, University of Missowi-Rolla, Rolh, Missotwi 65801 Received July 27, 1977 1. IPU’TRODUCTION Although the analytic theory of linear difference equations dates back to an 1885 memoir of Poincare, continuing work essentially began around 1910 with publication of several papers of G. D. Birkhoff, R. D. Carmichael, J. Horn, and N. E. Norlund; see, for instance, [l, 2, 4, 51. Since that time, C. R. Adams, M7. J. Trjitzinsky, and others have carried on the development of the theory; numerous contributions have been made in recent years by TV. A. Harris, Jr., P. Sibuya, and H. L. Turrittin; see, for instance, [7-9, 16-171. The monographs of Norlund [14] and L. M. Milne-Thomson [13] give a comprehensive account of earlier work, and references to more recent literature are given in the surrey paper of Harris [S]. The similarity between difference equations and differential equations has been noted by many investigators; for instance, Birkhoff [3] pointed out that the analytic theory of linear difference equations provides a “methodological pattern” for the “essentially simpler but analogous” theory of linear differential equations. In this paper, we apply a projection method which has been useful in the treat- ment of analytic differential equations [6, 101 to obtain existence theorems for convergent factorial series solutions of analytic difference equations.
    [Show full text]
  • Elementary Real Analysis
    Elementary Real Analysis MAT 2125 Winter 2017 Alistair Savage Department of Mathematics and Statistics University of Ottawa This work is licensed under a Creative Commons Attribution-ShareAlike 4.0 International License Contents Preface iii 1 The real numbers1 1.1 Algebraic structure: the field axioms......................1 1.2 Order structure..................................3 1.3 Bounds and the completeness axiom......................4 1.4 Natural numbers and induction.........................7 1.5 Rational numbers................................. 10 1.6 Absolute value: the metric structure on R ................... 11 1.7 Constructing the real numbers.......................... 12 2 Sequences 13 2.1 Limits....................................... 13 2.2 Properties of limits................................ 17 2.3 Monotonic convergence criterion......................... 20 2.4 Subsequences................................... 22 2.5 Cauchy sequences................................. 25 2.6 Limit inferior and limit superior......................... 27 3 Series 31 3.1 Definition and basic properties.......................... 31 3.2 Convergence tests................................. 35 3.3 Absolute convergence............................... 40 4 Topology of Rd 42 4.1 Norms....................................... 42 4.2 Convergence in Rd ................................ 45 4.3 Open and closed sets............................... 48 4.4 Compact sets................................... 54 5 Continuity 59 5.1 Limits......................................
    [Show full text]
  • Complex Analysis
    University of Cambridge Mathematics Tripos Part IB Complex Analysis Lent, 2018 Lectures by G. P. Paternain Notes by Qiangru Kuang Contents Contents 1 Basic notions 2 1.1 Complex differentiation ....................... 2 1.2 Power series .............................. 4 1.3 Conformal maps ........................... 8 2 Complex Integration I 10 2.1 Integration along curves ....................... 10 2.2 Cauchy’s Theorem, weak version .................. 15 2.3 Cauchy Integral Formula, weak version ............... 17 2.4 Application of Cauchy Integration Formula ............ 18 2.5 Uniform limits of holomorphic functions .............. 20 2.6 Zeros of holomorphic functions ................... 22 2.7 Analytic continuation ........................ 22 3 Complex Integration II 24 3.1 Winding number ........................... 24 3.2 General form of Cauchy’s theorem ................. 26 4 Laurent expansion, Singularities and the Residue theorem 29 4.1 Laurent expansion .......................... 29 4.2 Isolated singularities ......................... 30 4.3 Application and techniques of integration ............. 34 5 The Argument principle, Local degree, Open mapping theorem & Rouché’s theorem 38 Index 41 1 1 Basic notions 1 Basic notions Some preliminary notations/definitions: Notation. • 퐷(푎, 푟) is the open disc of radius 푟 > 0 and centred at 푎 ∈ C. • 푈 ⊆ C is open if for any 푎 ∈ 푈, there exists 휀 > 0 such that 퐷(푎, 휀) ⊆ 푈. • A curve is a continuous map from a closed interval 휑 ∶ [푎, 푏] → C. It is continuously differentiable, i.e. 퐶1, if 휑′ exists and is continuous on [푎, 푏]. • An open set 푈 ⊆ C is path-connected if for every 푧, 푤 ∈ 푈 there exists a curve 휑 ∶ [0, 1] → 푈 with endpoints 푧, 푤.
    [Show full text]