Analytic Function Theory Basic Analysis in One Complex Variable Lecture Notes
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Class 1/28 1 Zeros of an Analytic Function
Math 752 Spring 2011 Class 1/28 1 Zeros of an analytic function Towards the fundamental theorem of algebra and its statement for analytic functions. Definition 1. Let f : G → C be analytic and f(a) = 0. a is said to have multiplicity m ≥ 1 if there exists an analytic function g : G → C with g(a) 6= 0 so that f(z) = (z − a)mg(z). Definition 2. If f is analytic in C it is called entire. An entire function has a power series expansion with infinite radius of convergence. Theorem 1 (Liouville’s Theorem). If f is a bounded entire function then f is constant. 0 Proof. Assume |f(z)| ≤ M for all z ∈ C. Use Cauchy’s estimate for f to obtain that |f 0(z)| ≤ M/R for every R > 0 and hence equal to 0. Theorem 2 (Fundamental theorem of algebra). For every non-constant polynomial there exists a ∈ C with p(a) = 0. Proof. Two facts: If p has degree ≥ 1 then lim p(z) = ∞ z→∞ where the limit is taken along any path to ∞ in C∞. (Sometimes also written as |z| → ∞.) If p has no zero, its reciprocal is therefore entire and bounded. Invoke Liouville’s theorem. Corollary 1. If p is a polynomial with zeros aj (multiplicity kj) then p(z) = k k km c(z − a1) 1 (z − a2) 2 ...(z − am) . Proof. Induction, and the fact that p(z)/(z − a) is a polynomial of degree n − 1 if p(a) = 0. 1 The zero function is the only analytic function that has a zero of infinite order. -
Lecture Notes in Mathematics
Lecture Notes in Mathematics Edited by A. Dold and B. Eckmann Subseries: Mathematisches Institut der Universit~it und Max-Planck-lnstitut for Mathematik, Bonn - voL 5 Adviser: E Hirzebruch 1111 Arbeitstagung Bonn 1984 Proceedings of the meeting held by the Max-Planck-lnstitut fur Mathematik, Bonn June 15-22, 1984 Edited by E Hirzebruch, J. Schwermer and S. Suter I IIII Springer-Verlag Berlin Heidelberg New York Tokyo Herausgeber Friedrich Hirzebruch Joachim Schwermer Silke Suter Max-Planck-lnstitut fLir Mathematik Gottfried-Claren-Str. 26 5300 Bonn 3, Federal Republic of Germany AMS-Subject Classification (1980): 10D15, 10D21, 10F99, 12D30, 14H10, 14H40, 14K22, 17B65, 20G35, 22E47, 22E65, 32G15, 53C20, 57 N13, 58F19 ISBN 3-54045195-8 Springer-Verlag Berlin Heidelberg New York Tokyo ISBN 0-387-15195-8 Springer-Verlag New York Heidelberg Berlin Tokyo CIP-Kurztitelaufnahme der Deutschen Bibliothek. Mathematische Arbeitstagung <25. 1984. Bonn>: Arbeitstagung Bonn: 1984; proceedings of the meeting, held in Bonn, June 15-22, 1984 / [25. Math. Arbeitstagung]. Ed. by E Hirzebruch ... - Berlin; Heidelberg; NewYork; Tokyo: Springer, 1985. (Lecture notes in mathematics; Vol. 1t11: Subseries: Mathematisches I nstitut der U niversit~it und Max-Planck-lnstitut for Mathematik Bonn; VoL 5) ISBN 3-540-t5195-8 (Berlin...) ISBN 0-387q5195-8 (NewYork ...) NE: Hirzebruch, Friedrich [Hrsg.]; Lecture notes in mathematics / Subseries: Mathematischee Institut der UniversitAt und Max-Planck-lnstitut fur Mathematik Bonn; HST This work ts subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically those of translation, reprinting, re~use of illustrations, broadcasting, reproduction by photocopying machine or similar means, and storage in data banks. -
Topic 7 Notes 7 Taylor and Laurent Series
Topic 7 Notes Jeremy Orloff 7 Taylor and Laurent series 7.1 Introduction We originally defined an analytic function as one where the derivative, defined as a limit of ratios, existed. We went on to prove Cauchy's theorem and Cauchy's integral formula. These revealed some deep properties of analytic functions, e.g. the existence of derivatives of all orders. Our goal in this topic is to express analytic functions as infinite power series. This will lead us to Taylor series. When a complex function has an isolated singularity at a point we will replace Taylor series by Laurent series. Not surprisingly we will derive these series from Cauchy's integral formula. Although we come to power series representations after exploring other properties of analytic functions, they will be one of our main tools in understanding and computing with analytic functions. 7.2 Geometric series Having a detailed understanding of geometric series will enable us to use Cauchy's integral formula to understand power series representations of analytic functions. We start with the definition: Definition. A finite geometric series has one of the following (all equivalent) forms. 2 3 n Sn = a(1 + r + r + r + ::: + r ) = a + ar + ar2 + ar3 + ::: + arn n X = arj j=0 n X = a rj j=0 The number r is called the ratio of the geometric series because it is the ratio of consecutive terms of the series. Theorem. The sum of a finite geometric series is given by a(1 − rn+1) S = a(1 + r + r2 + r3 + ::: + rn) = : (1) n 1 − r Proof. -
Complex Analysis Qual Sheet
Complex Analysis Qual Sheet Robert Won \Tricks and traps. Basically all complex analysis qualifying exams are collections of tricks and traps." - Jim Agler 1 Useful facts 1 X zn 1. ez = n! n=0 1 X z2n+1 1 2. sin z = (−1)n = (eiz − e−iz) (2n + 1)! 2i n=0 1 X z2n 1 3. cos z = (−1)n = (eiz + e−iz) 2n! 2 n=0 1 4. If g is a branch of f −1 on G, then for a 2 G, g0(a) = f 0(g(a)) 5. jz ± aj2 = jzj2 ± 2Reaz + jaj2 6. If f has a pole of order m at z = a and g(z) = (z − a)mf(z), then 1 Res(f; a) = g(m−1)(a): (m − 1)! 7. The elementary factors are defined as z2 zp E (z) = (1 − z) exp z + + ··· + : p 2 p Note that elementary factors are entire and Ep(z=a) has a simple zero at z = a. 8. The factorization of sin is given by 1 Y z2 sin πz = πz 1 − : n2 n=1 9. If f(z) = (z − a)mg(z) where g(a) 6= 0, then f 0(z) m g0(z) = + : f(z) z − a g(z) 1 2 Tricks 1. If f(z) nonzero, try dividing by f(z). Otherwise, if the region is simply connected, try writing f(z) = eg(z). 2. Remember that jezj = eRez and argez = Imz. If you see a Rez anywhere, try manipulating to get ez. 3. On a similar note, for a branch of the log, log reiθ = log jrj + iθ. -
Smooth Versus Analytic Functions
Smooth versus Analytic functions Henry Jacobs December 6, 2009 Functions of the form X i f(x) = aix i≥0 that converge everywhere are called analytic. We see that analytic functions are equal to there Taylor expansions. Obviously all analytic functions are smooth or C∞ but not all smooth functions are analytic. For example 2 g(x) = e−1/x Has derivatives of all orders, so g ∈ C∞. This function also has a Taylor series expansion about any point. In particular the Taylor expansion about 0 is g(x) ≈ 0 + 0x + 0x2 + ... So that the Taylor series expansion does in fact converge to the function g˜(x) = 0 We see that g andg ˜ are competely different and only equal each other at a single point. So we’ve shown that g is not analytic. This is relevent in this class when finding approximations of invariant man- ifolds. Generally when we ask you to find a 2nd order approximation of the center manifold we just want you to express it as the graph of some function on an affine subspace of Rn. For example say we’re in R2 with an equilibrium point at the origin, and a center subspace along the y-axis. Than if you’re asked to find the center manifold to 2nd order you assume the manifold is locally (i.e. near (0,0)) defined by the graph (h(y), y). Where h(y) = 0, h0(y) = 0. Thus the taylor approximation is h(y) = ay2 + hot. and you must solve for a using the invariance of the manifold and the dynamics. -
Sample Questions for Preliminary Complex Analysis Exam
SAMPLE QUESTIONS FOR PRELIMINARY COMPLEX ANALYSIS EXAM VERSION 2.0 Contents 1. Complex numbers and functions 1 2. Definition of holomorphic function 1 3. Complex Integrals and the Cauchy Integral Formula 2 4. Sequences and series, Taylor series, and series of analytic functions 2 5. Identity Theorem 3 6. Schwarz Lemma and Cauchy Inequalities 4 7. Liouville's Theorem 4 8. Laurent series and singularities 4 9. Residue Theorem 5 10. Contour Integrals 5 11. Argument Principle 6 12. Rouch´e'sTheorem 6 13. Conformal maps 7 14. Analytic Continuation 7 15. Suggested Practice Exams 8 1. Complex numbers and functions (1.1) Write all values of ii in the form a + bi. 2 (1.2) Prove thatp sin z = z has infinitely many complex solutions. (1.3) Find log 3 + i, using the principal branch. 2. Definition of holomorphic function (2.1) Find all v : R2 ! R2 such that for z = x + iy, f(z) = (x3 − 3xy2) + iv(x; y) is analytic. (2.2) Prove that if g : C ! C is a C1 function, the following two definitions of \holomor- phic" are the same: @g (a) @z = 0 0 2 2 (b) the derivative transformation g (z0): R ! R is C-linear, for all z0 2 C. That 0 0 is, g (z0)mw = mwg (z0) for all w 2 C, where mw is the linear transformation given by complex multiplication by w. @h (2.3) True or false: If h is an entire function such that @z 6= 0 everywhere, then h is injective. 1 2 VERSION 2.0 (2.4) Find all possible a; b 2 R such that f (x; y) = x2 +iaxy +by2, x; y 2 R is holomorphic as a function of z = x + iy. -
Chapter 2 Complex Analysis
Chapter 2 Complex Analysis In this part of the course we will study some basic complex analysis. This is an extremely useful and beautiful part of mathematics and forms the basis of many techniques employed in many branches of mathematics and physics. We will extend the notions of derivatives and integrals, familiar from calculus, to the case of complex functions of a complex variable. In so doing we will come across analytic functions, which form the centerpiece of this part of the course. In fact, to a large extent complex analysis is the study of analytic functions. After a brief review of complex numbers as points in the complex plane, we will ¯rst discuss analyticity and give plenty of examples of analytic functions. We will then discuss complex integration, culminating with the generalised Cauchy Integral Formula, and some of its applications. We then go on to discuss the power series representations of analytic functions and the residue calculus, which will allow us to compute many real integrals and in¯nite sums very easily via complex integration. 2.1 Analytic functions In this section we will study complex functions of a complex variable. We will see that di®erentiability of such a function is a non-trivial property, giving rise to the concept of an analytic function. We will then study many examples of analytic functions. In fact, the construction of analytic functions will form a basic leitmotif for this part of the course. 2.1.1 The complex plane We already discussed complex numbers briefly in Section 1.3.5. -
Lecture Note for Math 220A Complex Analysis of One Variable
Lecture Note for Math 220A Complex Analysis of One Variable Song-Ying Li University of California, Irvine Contents 1 Complex numbers and geometry 2 1.1 Complex number field . 2 1.2 Geometry of the complex numbers . 3 1.2.1 Euler's Formula . 3 1.3 Holomorphic linear factional maps . 6 1.3.1 Self-maps of unit circle and the unit disc. 6 1.3.2 Maps from line to circle and upper half plane to disc. 7 2 Smooth functions on domains in C 8 2.1 Notation and definitions . 8 2.2 Polynomial of degree n ...................... 9 2.3 Rules of differentiations . 11 3 Holomorphic, harmonic functions 14 3.1 Holomorphic functions and C-R equations . 14 3.2 Harmonic functions . 15 3.3 Translation formula for Laplacian . 17 4 Line integral and cohomology group 18 4.1 Line integrals . 18 4.2 Cohomology group . 19 4.3 Harmonic conjugate . 21 1 5 Complex line integrals 23 5.1 Definition and examples . 23 5.2 Green's theorem for complex line integral . 25 6 Complex differentiation 26 6.1 Definition of complex differentiation . 26 6.2 Properties of complex derivatives . 26 6.3 Complex anti-derivative . 27 7 Cauchy's theorem and Morera's theorem 31 7.1 Cauchy's theorems . 31 7.2 Morera's theorem . 33 8 Cauchy integral formula 34 8.1 Integral formula for C1 and holomorphic functions . 34 8.2 Examples of evaluating line integrals . 35 8.3 Cauchy integral for kth derivative f (k)(z) . 36 9 Application of the Cauchy integral formula 36 9.1 Mean value properties . -
Notes on Analytic Functions
Notes on Analytic Functions In these notes we define the notion of an analytic function. While this is not something we will spend a lot of time on, it becomes much more important in some other classes, in particular complex analysis. First we recall the following facts, which are useful in their own right: Theorem 1. Let (fn) be a sequence of functions on (a; b) and suppose that each fn is differentiable. 0 If (fn) converges to a function f uniformly and the sequence of derivatives (fn) converges uniformly to a function g, then f is differentiable and f 0 = g. So, the uniform limit of differentiable functions is itself differentiable as long as the sequence of derivatives also converges uniformly, in which case the derivative of the uniform limit is the uniform limit of the derivatives. We will not prove this here as the proof is not easy; however, note that the proof of Theorem 26.5 in the book can be modified to give a proof of the above theorem in the 0 special case that each derivative fn is continuous. Note that we need the extra assumption that the sequence of derivatives converges uniformly, as the following example shows: q 2 1 Example 1. For each n, let fn :(−1; 1) be the function fn(x) = x + n . We have seen before that (fn) converges uniformly to f(x) = jxj on (−1; 1). Each fn is differentiable at 0 but f is not, so the uniform limit of differentiable functions need not be differentiable. We shouldn't expect that the uniform limit of differentiable functions be differentiable for the fol- lowing reason: differentiability is a local condition which measures how rapidly a function changes, while uniform convergence is a global condition which measures how close functions are to one another. -
Vector-Valued Holomorphic Functions
Appendix A Vector-valued Holomorphic Functions Let X be a Banach space and let Ω ⊂ C be an open set. A function f :Ω→ X is holomorphic if f(z0 + h) − f(z0) f (z0) := lim (A.1) h→0 h h∈C\{0} exists for all z0 ∈ Ω. If f is holomorphic, then f is continuous and weakly holomorphic (i.e. x∗ ◦ f ∗ ∗ is holomorphic for all x ∈ X ). If Γ := {γ(t):t ∈ [a,b]} is a finite, piecewise smooth contour in Ω, we can form the contour integral f(z) dz. This coincides Γ b with the Bochner integral a f(γ(t))γ (t) dt (see Section 1.1). Similarly we can define integrals over infinite contours when the corresponding Bochner integral is absolutely convergent. Since 1 2 f(z) dz, x∗ = f(z),x∗ dz, Γ Γ many properties of holomorphic functions and contour integrals may be extended from the scalar to the vector-valued case, by applying the Hahn-Banach theorem. For example, Cauchy’s theorem is valid, and also Cauchy’s integral formula: 1 f(z) f(w)= dz (A.2) − 2πi |z−z0|=r z w whenever f is holomorphic in Ω, the closed ball B(z0,r) is contained in Ω and w ∈ B(z0,r). As in the scalar case one deduces Taylor’s theorem from this. Proposition A.1. Let f :Ω→ X be holomorphic, where Ω ⊂ C is open. Let z0 ∈ Ω,r>0 such that B(z0,r) ⊂ Ω.Then W. Arendt et al., Vector-valued Laplace Transforms and Cauchy Problems: Second Edition, 461 Monographs in Mathematics 96, DOI 10.1007/978-3-0348-0087-7, © Springer Basel AG 2011 462 A. -
Cauchy's Theorem
® Cauchy’s Theorem 26.5 Introduction In this Section we introduce Cauchy’s theorem which allows us to simplify the calculation of certain contour integrals. A second result, known as Cauchy’s integral formula, allows us to evaluate some I f(z) integrals of the form dz where z0 lies inside C. C z − z0 • be familiar with the basic ideas of functions Prerequisites of a complex variable Before starting this Section you should ... • be familiar with line integrals Learning Outcomes • state and use Cauchy’s theorem • state and use Cauchy’s integral formula On completion you should be able to ... HELM (2008): 39 Section 26.5: Cauchy’s Theorem 1. Cauchy’s theorem Simply-connected regions A region is said to be simply-connected if any closed curve in that region can be shrunk to a point without any part of it leaving a region. The interior of a square or a circle are examples of simply connected regions. In Figure 11 (a) and (b) the shaded grey area is the region and a typical closed curve is shown inside the region. In Figure 11 (c) the region contains a hole (the white area inside). The shaded region between the two circles is not simply-connected; curve C1 can shrink to a point but curve C2 cannot shrink to a point without leaving the region, due to the hole inside it. C2 C1 (a) (b) (c) Figure 11 Key Point 2 Cauchy’s Theorem The theorem states that if f(z) is analytic everywhere within a simply-connected region then: I f(z) dz = 0 C for every simple closed path C lying in the region. -
18.04 S18 Topic 2: Analytic Functions
Topic 2 Notes Jeremy Orloff 2 Analytic functions 2.1 Introduction The main goal of this topic is to define and give some of the important properties of complex analytic functions. A function f .z/ is analytic if it has a complex derivative f ¨.z/. In general, the rules for computing derivatives will be familiar to you from single variable calculus. However, a much richer set of conclusions can be drawn about a complex analytic function than is generally true about real differentiable functions. 2.2 The derivative: preliminaries In calculus we defined the derivative as a limit. In complex analysis we will do the same. Δf f .z + Δz/* f .z/ f ¨.z/ = lim = lim : Δz→0 Δz Δz→0 Δz Before giving the derivative our full attention we are going to have to spend some time exploring and understanding limits. To motivate this we’ll first look at two simple examples – one positive and one negative. Example 2.1. Find the derivative of f .z/ = z2. Solution: We compute using the definition of the derivative as a limit. .z + Δz/2 * z2 z2 + 2zΔz + (Δz/2 * z2 lim = lim = lim 2z + Δz = 2z: Δz→0 Δz Δz→0 Δz Δz→0 That was a positive example. Here’s a negative one which shows that we need a careful understanding of limits. Example 2.2. Let f .z/ = z. Show that the limit for f ¨.0/ does not converge. Solution: Let’s try to compute f ¨.0/ using a limit: f (Δz/* f .0/ Δz Δx * iΔy f ¨.0/ = lim = lim = : Δz→0 Δz Δz→0 Δz Δx + iΔy Here we used Δz = Δx + iΔy.