Lecture Note for Math 220B Complex Analysis of One Variable

Lecture Note for Math 220B Complex Analysis of One Variable

Lecture Note for Math 220B Complex Analysis of One Variable Song-Ying Li University of California, Irvine Contents 1 The Residue theorem applied to real integrals 3 1.1 Several types of real integrals . 3 1.2 The Logarithm function . 11 1.3 Real integrals involving ln x ................... 13 1.4 Homework 1 . 17 2 The Zero Set of Holomorphic Functions 18 2.1 The Argument Principle and its Applications . 18 2.2 The Open Mapping theorem . 20 2.3 Rouch´eTheorems . 20 2.4 Applications and Examples . 21 2.5 Hurwitz's Theorem and Applications . 23 2.6 Examples/Applications . 24 2.7 Homework 2 . 25 3 The Geometry of Holomorphic Mappings 27 3.1 The Maximum Modulus Theorem . 27 3.2 Schwarz Lemma . 29 3.2.1 Schwarz-Pick Lemma . 29 3.3 Homework 3 . 32 3.4 Conformal and proper holomorphic function maps . 33 3.5 Automorphism groups . 35 3.6 M¨obiustransformations . 37 1 3.7 Cross ratio . 38 3.8 Properties of the Cross Ratio . 39 3.8.1 Symmetric points . 39 3.9 Construction of conformal maps . 41 3.10 Homework 4 . 44 3.11 Midterm Review . 46 3.12 Normal families . 48 3.12.1 Examples for normal families . 50 3.13 The Riemann Mapping Theorem . 52 3.13.1 Existence of the Riemann map . 52 3.13.2 Proof of Riemann mapping theorem . 54 3.14 Homework 5 . 55 3.15 The Reflection Principle . 57 3.16 Homework 6 . 58 3.17 Singular Points and Regular Points . 59 4 Infinite Products 60 4.1 Basic properties of infinite products . 61 4.2 Examples . 63 4.3 Infinite Products and Factorization Factors . 64 4.4 Weierstrass Factorization Theorem . 66 4.5 Application to Singular Points . 68 4.6 Mittag-Leffler’s Theorem . 69 4.7 Homework 7 . 71 List of Figures 1 The nice contour . 5 2 The semi-circular contour with a bump . 8 3 Another common contour . 9 4 The contour that works well with ln(x) . 14 5 Conformal Map 1 . 42 6 Upper half disc to unit disc . 43 7 Region between two circles to unit disc . 44 8 conformal map 4 . 45 Acknowledgement: I would like to thank J. N. Treuer for reading through the first draft and making some revisions. 2 1 The Residue theorem applied to real inte- grals We are going to apply the Residue theorem to evaluate integrals of real- valued functions over subsets of IR. We will call such integrals real integrals. 1.1 Several types of real integrals I) Let R(x; y) be a rational function in x and y. How does one evaluate Z 2π R(cos t; sin t)dt? 0 Solution. Let z = eit; t 2 [0; 2π): Then z + 1 z2 + 1 z − 1 z2 − 1 dz cos t = z = ; sin t = z = and dt = : 2 2z 2i 2iz iz Therefore, Z 2π Z z2 + 1 z2 − 1 1 R(cos t; sin t)dt = R( ; ) dz: 0 jzj=1 2z 2iz iz We can apply the Residue theorem to evaluate the right hand side. EXAMPLE 1 For a > 1, evaluate the integral Z 2π 1 dt 0 a + cos t Solution. Let z =: eit Then 1 1 cos t = (z + ); dz = izdt 2 z 3 Therefore, Z 2π 1 Z 1 1 dt = 1 dz 0 a + cos t jzj=1 a + 2 (z + 1=z) iz 2 Z 1 = dz i jzj=1 2az + z2 + 1 1 p = 4πRes ; −a + a2 − 1 z2 + 2az + 1 4π = p 2(−a + a2 − 1) + 2a 2π = p : a2 − 1 II) How does one evaluate Z 1 R(x)dx? −∞ THEOREM 1.1 Let Pm(x) and Qn(x) be polynomials of degree m and n respectively and (P ;Q ) = 1. Let R(x) = Pm(x) . Suppose also that Q (x) 6= m n Qn(x) n 0 for all x 2 IR and n − m ≥ 2. Then ` Z 1 X R(x)dx = 2πi( Res(R; zk)) −∞ k=1 where z1; ··· ; z` are the zeros of Qn not counting multiplicity in the upper 2 half plane IR+. Proof. Let fz1; :::; z`g be the zeros stated in the theorem's hypothesis and choose r >> 1 such that fz1; ··· ; z`g ⊂ D(0; r). Apply the Residue theorem 2 to R(z) on Dr = fz 2 IR+ : jzj < rg. Then ` Z r Z X R(x) = − R(z)dz + 2πi Res(R; zk) −r Cr k=1 iθ where Cr = fz = re : 0 ≤ θ ≤ πg. Since n ≥ m + 2, we have Z lim R(z)dz = 0: r!1 Cr The theorem is proved. 4 Cr Dr −r r Figure 1: The nice contour EXAMPLE 2 Evaluate the integral Z 1 1 dx: 0 (1 + x2)2 Solution. Let f(z) = 1=(z2 + 1)2. Then Z 1 1 1 Z 1 1 dx = dt 0 (1 + x2)2 2 −∞ (1 + x2)2 −2 = πiRes(f; i) = πi 3 (z + i) z=i 2πi π = − = (2i)3 4 III) How does one evaluate Z 1 f(x)eixdx? −∞ 2 Lemma 1.2 Let f(z) be meromorphic in IR+ such that lim f(reiθ) = 0 r!1 2 uniformly for θ 2 (0; π). Let fzk : 1 ≤ k ≤ mg be zero set of f in IR+. Then Z lim f(z)eizdz = 0 R!1 CR where CR = fz = x + iy 2 C: jzj = R; y > 0g 5 iθ Proof. Let MR = maxfjf(Re )j : θ 2 [0; π]g. Then Z Z π iz iθ −R sin θ f(z)e dz ≤ jf(Re )je Rdθ CR 0 Z π −R sin θ ≤ MR e Rdθ 0 Z π=2 −R sin θ = 2MR e Rdθ 0 Z π=2 −2Rθ/π ≤ 2MR e Rdθ 0 Z 1 −t ≤ πMR e dt 0 = πMR ! 0 as R ! 1 π where the third inequality follows because sin(θ) is concave on [0; 2 ]; hence 2θ π sin(θ) > π on [0; 2 ]: 2 THEOREM 1.3 Let f(z) be meromorphic in IR+ such that lim f(reiθ) = 0 r!1 2 uniformly for θ 2 (0; π). Let fzk : 1 ≤ k ≤ mg be zero set of f in IR+.Then Z 1 m ix X iz f(x)e dx = 2πi Res(fe ; zk) −∞ k=1 2 Proof. Let DR = fz 2 IR+ : jzj < Rg. By the Residue theorem, one has Z R Z Z ix iz iz X iz f(x)e + f(z)e dz = f(z)e dz = 2πi Res(f(z)e ; zk) −R CR @DR zk2DR Let R ! 1. By the previous lemma, Z 1 m ix X iz f(x)e = 2πi Res(f(z)e ; zk) −∞ k=1 The proof is complete. EXAMPLE 3 Evaluate the following integral: Z 1 cos x dx 0 1 + x2 6 Solution. Since Z 1 cos x 1 Z 1 cos x dx = dx 0 1 + x2 2 −∞ 1 + x2 1 Z 1 eix = Re dx 2 −∞ 1 + x2 eiz = Re πiRes( ; i) 1 + z2 π = : 2e EXAMPLE 4 Evaluate the following integral: Z 1 sin x dx 0 x Solution.We would like to write Z 1 sin x 1 Z 1 sin x 1 Z 1 eix dx = dx = Im dx: 0 x 2 −∞ x 2 −∞ x However, the last equality may cause trouble because the last integral does not converge. So, instead, we write Z 1 sin x h Z −r sin(x) Z R sin x i dx = lim dx + dx −∞ x R!1;r!0 −R x r x Let 2 Dr;R = fz 2 IR+ : jzj < R; jzj > rg and @Dr;R = CR [ [−R; −r] [ (−Cr) [ [r; R]: Thus Z 1 sin x h Z −r eix Z R eix i dx = lim Im dx + dx −∞ x R!1;r!0 −R x r x h Z eiz Z eiz Z eiz i = lim Im dz − dz + dz R!1;r!0 @Dr;R z CR z Cr z Z eiz = 0 + 0 + lim Im dz r!0 Cr z Z π eri cos θ−r sin θ = lim Im ireiθdθ r!0 0 reiθ = π 7 CR Dr;R −Cr -R -r r R Figure 2: The semi-circular contour with a bump eiz where the third equality follows because z is holomorphic in a neighborhood of Dr;R and lemma 1.2. Therefore, Z 1 sin x π dx = : 0 x 2 EXAMPLE 5 Evaluate the following integral: Z 1 sin2 x dx: 0 x2 Solution. 2 2 Z 1 sin x sin x 1 Z 1 2 sin x cos x dx = − + dx 0 x2 x 0 0 x Z 1 sin(2x) = dx 0 x Z 1 sin(2x) = d(2x) 0 2x π = : 2 EXAMPLE 6 Evaluate the following integral: Z 1 1 − cos x dx 0 x2 8 Solution. Z 1 1 − cos x 1 − cos x 1 Z 1 sin x π dx = − + = : 0 x2 x 0 0 x 2 IV) Choosing special integral path. EXAMPLE 7 Evaluate the following integral: Z 1 1 dx: 0 1 + x3 Solution. We know that (e2πi=3)3 = 1. Choose iθ DR = fz = jzje : 0 < θ < 2π=3; jzj < Rg Then for R > 2; Re2πi=3 2π 3 R Figure 3: Another common contour Z 1 1 iπ=3 2πi 3 dz = 2πiRes( 3 ; e ) = 2πi=3 @DR 1 + z 1 + z 3e On the other hand, Z Z R Z Z 0 1 1 1 1 2πi=3 3 dz = 3 dx + 3 dz + 3 e dx @DR 1 + z 0 1 + x CR 1 + z R 1 + x Z 1 1 ! (1 − e2πi=3) dx 0 1 + x3 9 as R ! 1.

View Full Text

Details

  • File Type
    pdf
  • Upload Time
    -
  • Content Languages
    English
  • Upload User
    Anonymous/Not logged-in
  • File Pages
    76 Page
  • File Size
    -

Download

Channel Download Status
Express Download Enable

Copyright

We respect the copyrights and intellectual property rights of all users. All uploaded documents are either original works of the uploader or authorized works of the rightful owners.

  • Not to be reproduced or distributed without explicit permission.
  • Not used for commercial purposes outside of approved use cases.
  • Not used to infringe on the rights of the original creators.
  • If you believe any content infringes your copyright, please contact us immediately.

Support

For help with questions, suggestions, or problems, please contact us