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A guide to complex variables by steven g krantz

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Tiêu đề A Guide to Complex Variables
Tác giả Steven G. Krantz
Thể loại book
Năm xuất bản 2007
Định dạng
Số trang 185
Dung lượng 1,27 MB

Cấu trúc

  • 1.1 Complex Arithmetic (17)
    • 1.1.1 The Real Numbers (17)
    • 1.1.2 The Complex Numbers (17)
    • 1.1.3 Complex Conjugate (19)
    • 1.1.4 Modulus of a Complex Number (19)
    • 1.1.5 The Topology of the Complex Plane (19)
    • 1.1.6 The Complex Numbers as a Field (23)
    • 1.1.7 The Fundamental Theorem of Algebra (24)
  • 1.2 The Exponential and Applications (24)
    • 1.2.1 The Exponential Function (24)
    • 1.2.2 The Exponential Using Power Series (25)
    • 1.2.3 Laws of Exponentiation (25)
    • 1.2.4 Polar Form of a Complex Number (25)
    • 1.2.5 Roots of Complex Numbers (27)
    • 1.2.6 The Argument of a Complex Number (29)
    • 1.2.7 Fundamental Inequalities (30)
  • 1.3 Holomorphic Functions (31)
    • 1.3.1 Continuously Differentiable and C k Functions (31)
    • 1.3.2 The Cauchy-Riemann Equations (31)
    • 1.3.3 Derivatives (32)
    • 1.3.4 Definition of Holomorphic Function (33)
    • 1.3.5 The Complex Derivative (34)
    • 1.3.6 Alternative Terminology for Holomorphic Functions (35)
  • 1.4 Holomorphic and Harmonic Functions (37)
    • 1.4.1 Harmonic Functions (37)
    • 1.4.2 How They are Related (37)
  • 2.1 Real and Complex Line Integrals (39)
    • 2.1.1 Curves (39)
    • 2.1.2 Closed Curves (40)
    • 2.1.3 Differentiable and C k Curves (40)
    • 2.1.4 Integrals on Curves (41)
    • 2.1.5 The Fundamental Theorem of Calculus along Curves . 24 (42)
    • 2.1.6 The Complex Line Integral (42)
    • 2.1.7 Properties of Integrals (43)
  • 2.2 Complex Differentiability and Conformality (44)
    • 2.2.1 Limits (44)
    • 2.2.2 Continuity (0)
    • 2.2.3 The Complex Derivative (0)
    • 2.2.4 Holomorphicity and the Complex Derivative (0)
    • 2.2.5 Conformality (0)
  • 2.3 The Cauchy Integral Formula and Theorem (48)
    • 2.3.1 The Cauchy Integral Theorem, Basic Form (48)
    • 2.3.2 The Cauchy Integral Formula (49)
    • 2.3.3 More General Forms of the Cauchy Theorems (49)
    • 2.3.4 Deformability of Curves (50)
  • 2.4 The Limitations of the Cauchy Formula (51)
  • 3.1 The Derivatives of a Holomorphic Function (55)
    • 3.1.1 A Formula for the Derivative (55)
    • 3.1.2 The Cauchy Estimates (55)
    • 3.1.3 Entire Functions and Liouville’s Theorem (56)
    • 3.1.4 The Fundamental Theorem of Algebra (57)
    • 3.1.5 Sequences of Holomorphic Functions and their Deriva- (58)
    • 3.1.6 The Power Series Representation of a Holomorphic Func- (59)
  • 3.2 The Zeros of a Holomorphic Function (61)
    • 3.2.1 The Zero Set of a Holomorphic Function (61)
    • 3.2.2 Discreteness of the Zeros of a Holomorphic Function (62)
    • 3.2.3 Discrete Sets and Zero Sets (62)
    • 3.2.4 Uniqueness of Analytic Continuation (64)
  • 4.1 The Behavior of a Holomorphic Function near an Isolated Sin- (67)
    • 4.1.1 Isolated Singularities (67)
    • 4.1.2 A Holomorphic Function on a Punctured Domain (67)
    • 4.1.3 Classification of Singularities (68)
    • 4.1.4 Removable Singularities, Poles, and Essential Singu- (69)
    • 4.1.5 The Riemann Removable Singularities Theorem (69)
    • 4.1.6 The Casorati-Weierstrass Theorem (69)
  • 4.2 Expansion around Singular Points (70)
    • 4.2.1 Laurent Series (70)
    • 4.2.2 Convergence of a Doubly Infinite Series (70)
    • 4.2.3 Annulus of Convergence (71)
    • 4.2.4 Uniqueness of the Laurent Expansion (72)
    • 4.2.5 The Cauchy Integral Formula for an Annulus (72)
    • 4.2.6 Existence of Laurent Expansions (72)
    • 4.2.7 Holomorphic Functions with Isolated Singularities (73)
    • 4.2.8 Classification of Singularities in Terms of Laurent Series 52 (74)
  • 4.3 Examples of Laurent Expansions (75)
    • 4.3.1 Principal Part of a Function (75)
    • 4.3.2 Algorithm for Calculating the Coefficients of the Lau- (76)
  • 4.4 The Calculus of Residues (77)
    • 4.4.1 Functions with Multiple Singularities (77)
    • 4.4.2 The Residue Theorem (77)
    • 4.4.3 Residues (78)
    • 4.4.4 The Index or Winding Number of a Curve about a Point 56 (78)
    • 4.4.5 Restatement of the Residue Theorem (79)
    • 4.4.6 Method for Calculating Residues (80)
    • 4.4.7 Summary Charts of Laurent Series and Residues (81)
  • 4.5 Applications to the Calculation of Definite Integrals and Sums 58 (81)
    • 4.5.1 The Evaluation of Definite Integrals (81)
    • 4.5.2 A Basic Example (82)
    • 4.5.3 Complexification of the Integrand (85)
    • 4.5.4 An Example with a More Subtle Choice of Contour (86)
    • 4.5.5 Making the Spurious Part of the Integral Disappear (89)
    • 4.5.6 The Use of the Logarithm (91)
    • 4.5.7 Summing a Series Using Residues (94)
  • 4.6 Singularities at Infinity (95)
    • 4.6.1 Meromorphic Functions (95)
    • 4.6.2 Discrete Sets and Isolated Points (0)
    • 4.6.3 Definition of Meromorphic Function (0)
    • 4.6.4 Examples of Meromorphic Functions (0)
    • 4.6.5 Meromorphic Functions with Infinitely Many Poles (0)
    • 4.6.6 Singularities at Infinity (0)
    • 4.6.7 The Laurent Expansion at Infinity (0)
    • 4.6.8 Meromorphic at Infinity (0)
    • 4.6.9 Meromorphic Functions in the Extended Plane (0)
  • 5.1 Counting Zeros and Poles (101)
    • 5.1.1 Local Geometric Behavior of a Holomorphic Function . 77 (101)
    • 5.1.2 Locating the Zeros of a Holomorphic Function (101)
    • 5.1.3 Zero of Order n (102)
    • 5.1.4 Counting the Zeros of a Holomorphic Function (102)
    • 5.1.5 The Argument Principle (103)
    • 5.1.6 Location of Poles (105)
    • 5.1.7 The Argument Principle for Meromorphic Functions . 81 (105)
  • 5.2 The Local Geometry of Holomorphic Functions (105)
    • 5.2.1 The Open Mapping Theorem (105)
  • 5.3 Further Results on the Zeros of Holomorphic Functions (107)
    • 5.3.1 Rouch´e’s Theorem (107)
    • 5.3.2 Typical Application of Rouch´e’s Theorem (108)
    • 5.3.3 Rouch´e’s Theorem and the Fundamental Theorem of (108)
    • 5.3.4 Hurwitz’s Theorem (109)
  • 5.4 The Maximum Principle (109)
    • 5.4.1 The Maximum Modulus Principle (109)
    • 5.4.2 Boundary Maximum Modulus Theorem (111)
    • 5.4.3 The Minimum Principle (111)
    • 5.4.4 The Maximum Principle on an Unbounded Domain (112)
  • 5.5 The Schwarz Lemma (112)
    • 5.5.1 Schwarz’s Lemma (112)
    • 5.5.2 The Schwarz-Pick Lemma (113)
  • 6.1 The Idea of a Conformal Mapping (117)
    • 6.1.1 Conformal Mappings (117)
    • 6.1.2 Conformal Self-Maps of the Plane (118)
  • 6.2 Conformal Mappings of the Unit Disc (0)
  • 6.3 Linear Fractional Transformations (121)
    • 6.3.1 Linear Fractional Mappings (0)
    • 6.3.2 The Topology of the Extended Plane (0)
    • 6.3.3 The Riemann Sphere (0)
    • 6.3.4 Conformal Self-Maps of the Riemann Sphere (0)
    • 6.3.5 The Cayley Transform (0)
    • 6.3.6 Generalized Circles and Lines (0)
    • 6.3.7 The Cayley Transform Revisited (0)
    • 6.3.8 Summary Chart of Linear Fractional Transformations . 101 (0)
  • 6.4 The Riemann Mapping Theorem (0)
    • 6.4.1 The Concept of Homeomorphism (0)
    • 6.4.2 The Riemann Mapping Theorem (0)
    • 6.4.3 The Riemann Mapping Theorem: Second Formulation 102 (0)
  • 6.5 Conformal Mappings of Annuli (0)
    • 6.5.1 A Riemann Mapping Theorem for Annuli (0)
    • 6.5.2 Conformal Equivalence of Annuli (0)
    • 6.5.3 Classification of Planar Domains (0)
  • 7.1 Basic Properties of Harmonic Functions (129)
    • 7.1.1 The Laplace Equation (129)
    • 7.1.2 Definition of Harmonic Function (129)
    • 7.1.3 Real- and Complex-Valued Harmonic Functions (130)
    • 7.1.4 Harmonic Functions as the Real Parts of Holomorphic (130)
    • 7.1.5 Smoothness of Harmonic Functions (131)
  • 7.2 The Maximum Principle and the Mean Value Property (131)
    • 7.2.1 The Maximum Principle for Harmonic Functions (131)
    • 7.2.2 The Minimum Principle for Harmonic Functions (131)
    • 7.2.3 The Boundary Maximum and Minimum Principles (132)
    • 7.2.4 The Mean Value Property (132)
    • 7.2.5 Boundary Uniqueness for Harmonic Functions (133)
  • 7.3 The Poisson Integral Formula (133)
    • 7.3.1 The Poisson Integral (133)
    • 7.3.2 The Poisson Kernel (134)
    • 7.3.3 The Dirichlet Problem (134)
    • 7.3.4 The Solution of the Dirichlet Problem on the Disc (135)
    • 7.3.5 The Dirichlet Problem on a General Disc (135)
  • 7.4 Regularity of Harmonic Functions (136)
    • 7.4.1 The Mean Value Property on Circles (136)
    • 7.4.2 The Limit of a Sequence of Harmonic Functions (136)
  • 7.5 The Schwarz Reflection Principle (136)
    • 7.5.1 Reflection of Harmonic Functions (136)
    • 7.5.2 Schwarz Reflection Principle for Harmonic Functions . 112 (137)
    • 7.5.3 The Schwarz Reflection Principle for Holomorphic Func- (137)
    • 7.5.4 More General Versions of the Schwarz Reflection Prin- (138)
  • 7.6 Harnack’s Principle (139)
    • 7.6.1 The Harnack Inequality (139)
    • 7.6.2 Harnack’s Principle (139)
  • 7.7 The Dirichlet Problem and Subharmonic Functions (140)
    • 7.7.1 The Dirichlet Problem (140)
    • 7.7.2 Conditions for Solving the Dirichlet Problem (140)
    • 7.7.3 Motivation for Subharmonic Functions (141)
    • 7.7.4 Definition of Subharmonic Function (142)
    • 7.7.5 Other Characterizations of Subharmonic Functions (142)
    • 7.7.6 The Maximum Principle (142)
    • 7.7.7 Lack of A Minimum Principle (143)
    • 7.7.8 Basic Properties of Subharmonic Functions (143)
    • 7.7.9 The Concept of a Barrier (143)
  • 7.8 The General Solution of the Dirichlet Problem (144)
    • 7.8.1 Enunciation of the Solution of the Dirichlet Problem . 120 (144)
  • 8.1 Basic Concepts Concerning Infinite Sums and Products (147)
    • 8.1.1 Uniform Convergence of a Sequence (147)
    • 8.1.2 The Cauchy Condition for a Sequence of Functions (147)
    • 8.1.3 Normal Convergence of a Sequence (148)
    • 8.1.4 Normal Convergence of a Series (148)
    • 8.1.5 The Cauchy Condition for a Series (148)
    • 8.1.6 The Concept of an Infinite Product (149)
    • 8.1.7 Infinite Products of Scalars (149)
    • 8.1.8 Partial Products (149)
    • 8.1.9 Convergence of an Infinite Product (150)
    • 8.1.10 The Value of an Infinite Product (150)
    • 8.1.11 Products That Are Disallowed (150)
    • 8.1.12 Condition for Convergence of an Infinite Product (151)
    • 8.1.13 Infinite Products of Holomorphic Functions (152)
    • 8.1.14 Vanishing of an Infinite Product (153)
    • 8.1.15 Uniform Convergence of an Infinite Product of Functions127 (153)
    • 8.1.16 Condition for the Uniform Convergence of an Infinite (153)
  • 8.2 The Weierstrass Factorization Theorem (154)
    • 8.2.1 Prologue (154)
    • 8.2.2 Weierstrass Factors (154)
    • 8.2.3 Convergence of the Weierstrass Product (155)
    • 8.2.4 Existence of an Entire Function with Prescribed Zeros 129 (155)
    • 8.2.5 The Weierstrass Factorization Theorem (155)
  • 8.3 The Theorems of Weierstrass and Mittag-Leffler (156)
    • 8.3.1 The Concept of Weierstrass’s Theorem (156)
    • 8.3.2 Weierstrass’s Theorem (156)
    • 8.3.3 Construction of a Discrete Set (156)
    • 8.3.4 Domains of Existence for Holomorphic Functions (156)
    • 8.3.5 The Field Generated by the Ring of Holomorphic Func- (157)
    • 8.3.6 The Mittag-Leffler Theorem (158)
    • 8.3.7 Prescribing Principal Parts (159)
  • 8.4 Normal Families (159)
    • 8.4.1 Normal Convergence (159)
    • 8.4.2 Normal Families (159)
    • 8.4.3 Montel’s Theorem, First Version (160)
    • 8.4.4 Montel’s Theorem, Second Version (160)
    • 8.4.5 Examples of Normal Families (160)
  • 9.1 Definition of an Analytic Function Element (163)
    • 9.1.1 Continuation of Holomorphic Functions (163)
    • 9.1.2 Examples of Analytic Continuation (164)
    • 9.1.3 Function Elements (168)
    • 9.1.4 Direct Analytic Continuation (168)
    • 9.1.5 Analytic Continuation of a Function (169)
    • 9.1.6 Global Analytic Functions (169)
    • 9.1.7 An Example of Analytic Continuation (170)
  • 9.2 Analytic Continuation along a Curve (171)
    • 9.2.1 Continuation on a Curve (171)
    • 9.2.2 Uniqueness of Continuation along a Curve (172)
  • 9.3 The Monodromy Theorem (173)
    • 9.3.1 Unambiguity of Analytic Continuation (173)
    • 9.3.2 The Concept of Homotopy (173)
    • 9.3.3 Fixed Endpoint Homotopy (174)
    • 9.3.4 Unrestricted Continuation (174)
    • 9.3.5 The Monodromy Theorem (175)
    • 9.3.6 Monodromy and Globally Defined Analytic Functions . 147 (175)
  • 9.4 The Idea of a Riemann Surface (176)
    • 9.4.1 What is a Riemann Surface? (176)
    • 9.4.2 Examples of Riemann Surfaces (176)
    • 9.4.3 The Riemann Surface for the Square Root Function (178)
    • 9.4.4 Holomorphic Functions on a Riemann Surface (179)
    • 9.4.5 The Riemann Surface for the Logarithm (179)
    • 9.4.6 Riemann Surfaces in General (180)
  • 9.5 Picard’s Theorems (181)
    • 9.5.1 Value Distribution for Entire Functions (181)
    • 9.5.2 Picard’s Little Theorem (181)
    • 9.5.3 Picard’s Great Theorem (182)
    • 9.5.4 The Little Theorem, the Great Theorem, and the Casorati- (182)

Nội dung

Complex Arithmetic

The Real Numbers

We assume the reader to be familiar with the real number systemR We let

R 2 = {(x, y) : x ∈R , y ∈ R} (Figure 1.1) These are ordered pairs of real numbers.

As we shall see, the complex numbers are nothing other thanR 2 equipped with a special algebraic structure.

The Complex Numbers

The complex numbers C consist of R 2 equipped with some binary algebraic operations One defines

These operations of + andã are commutative and associative.

We denote (1,0) by 1 and (0,1) by i If α ∈ R, then we identify α with the complex number (α,0) Using this notation, we see that αã(x, y) = (α,0)ã(x, y) = (αx, αy) (1.1.2.1)

As a result, if (x, y) isany complex number, then

(x, y) = (x,0) + (0, y) =xã(1,0) +yã(0,1) =xã1 +yãi≡x+iy

Every complex number can be uniquely expressed in the form x + iy, where x and y are real numbers This notation simplifies the representation of complex numbers, allowing for clearer mathematical operations The fundamental laws of addition and multiplication apply to these numbers, facilitating their use in various mathematical contexts.

(x+iy)ã(x 0 +iy 0 ) = (xx 0 −yy 0 ) +i(xy 0 +yx 0 ).

Observe thatiãi=−1.Finally, the multiplication law is consistent with the scalar multiplication introduced in line (1.1.2.1).

In the realm of complex numbers, the symbols z, w, and ζ represent complex values, typically expressed as z = x + iy, w = u + iv, and ζ = ξ + iη Here, the real part of z is denoted as x, written as Re(z), while the imaginary part is represented by y, noted as Im(z).

The complex conjugate of a complex number is defined as x - iy, where x + iy represents the original complex number Denoted as z, the conjugate is expressed as z = x - iy This concept is particularly important because if p is a quadratic polynomial with real coefficients and z is one of its roots, then the conjugate z is also a root of the polynomial.

Figure 1.2: Euclidean distance (modulus) in the plane.

Complex Conjugate

Note that z+z = 2x , z−z = 2iy Also z+w=z+w , (1.1.3.1) zãw=zãw (1.1.3.2)

A complex number is real (has no imaginary part) if and only ifz =z.It is imaginary (has no real part) if and only ifz =−z.

Modulus of a Complex Number

The ordinary Euclidean distance of (x, y) to (0,0) is p x 2 +y 2 (Figure 1.2).

We also call this number themodulusof the complex numberz =x+iy and we write|z|=p x 2 +y 2 Note that zãz =x 2 +y 2 =|z| 2

The distance fromztowis|z−w|.We also have the formulas|zãw|=|z|ã|w| and|Rez| ≤ |z| and |Imz| ≤ |z|.

The Topology of the Complex Plane

IfP is a complex number and r >0, then we set

Figure 1.3: Open and closed discs. and

The first type of disc is the open disc centered at point P with radius r, while the second type is the closed disc with the same center and radius For convenience, we commonly use the symbols D and D to represent the open disc D(0,1) and the closed disc D(0,1), respectively.

A subset U of the complex numbers C is defined as open if, for every point P in C, there exists a radius r > 0 such that the disk D(P, r) is entirely contained within U This means that each point P in the set has neighboring points within a distance less than r that also belong to the set For instance, the set U = {z ∈ C: Re(z) > 1} is open, whereas the set F = {z ∈ C: Re(z) ≤ 1} is not.

A set E ⊆ C is said to be closed if C\E ≡ {z ∈ C : z 6∈ E} (the complement of E inC) is open The setF in the last paragraph is closed.

It isnotthe case that any given set is either open or closed For example, the setW ={z ∈C: 10 be such that D(P, r)⊆U Let γ : [0,1]→Cbe theC 1 curve γ(t) =P +rcos(2πt) +irsin(2πt) Then, for eachz ∈D(P, r), f(z) = 1

One may derive this result directly from Stokes’s theorem (see [KRA5] and also our Subsection 2.3.1).

More General Forms of the Cauchy Theorems

Now we present the very useful general statements of the Cauchy integral theorem and formula First we need a piece of terminology A curve γ : [a, b]→C is said to be piecewiseC k if

[a, b] = [a0, a1]∪[a1, a2]∪ ã ã ã ∪[am − 1, am] (2.3.3.1) with a =a0 < a1 0 We apply the Cauchy estimate (3.1.2.1) for k = 1 on

Since this inequality is true for everyr >0,we conclude that

Since P was arbitrary, we conclude that

The end of the last proof bears some commentary We prove that∂f/∂z ≡

0 But we know, since f is holomorphic, that ∂f/∂z ≡ 0 It follows from linear algebra that∂f/∂x≡0 and ∂f/∂y≡0 Then calculus tells us that f is constant.

Liouville's theorem can be applied to demonstrate a broader principle: for an entire function f: C → C, if there exists a real number C and a positive integer k such that certain conditions are met, then specific conclusions about the function can be drawn.

|f(z)| ≤Cã(1 +|z|) k for allz, thenf is a polynomial in z of degree at most k.

3.1 The Derivatives of a Holomorphic Function 41

The Fundamental Theorem of Algebra

One of the most elegant applications of Liouville’s Theorem is a proof of what is known as the Fundamental Theorem of Algebra (see also§§1.1.7):

The Fundamental Theorem of Algebra: Letp(z) be a non- constant (holomorphic) polynomial Then p has a root That is, there exists an α∈C such that p(α) = 0.

Proof: Suppose not Then g(z) = 1/p(z) is entire Also when |z| → ∞, then |p(z)| → +∞ Thus 1/|p(z)| → 0 as |z| → ∞; hence g is bounded.

By Liouville’s Theorem, g is constant, hence p is constant Contradiction.

For a polynomial \( p \) of degree \( k \geq 1 \), the Fundamental Theorem guarantees the existence of a root \( \alpha_1 \) Utilizing the Euclidean algorithm, we can divide \( z - \alpha_1 \) into \( p \) without any remainder, resulting in the expression \( p(z) = (z - \alpha_1) \tilde{p_1}(z) \).

A polynomial \( p_1 \) of degree \( k-1 \) has a root \( \alpha_2 \) if \( k-1 \geq 1 \), making it divisible by \( (z - \alpha_2) \) This leads to the expression \( p(z) = (z - \alpha_1)^{a}(z - \alpha_2)^{a} p_2(z) \), where \( p_2(z) \) is a polynomial of degree \( k - 2 \) This factorization process continues until reaching a constant polynomial \( p_k \) of degree 0 Consequently, if \( p(z) \) is a holomorphic polynomial of degree \( k \), it can be expressed in the form \( p(z) = C (z - \alpha_1)^{a} (z - \alpha_2)^{a} \cdots (z - \alpha_k)^{a} \), where \( C \) is a non-zero constant and \( \alpha_1, \ldots, \alpha_k \) are complex numbers that may not be distinct.

If some of the roots of p coincide, then we say that p has multiple roots.

A polynomial \( p \) is said to have a root of order \( m \) at a complex number \( \alpha \) if \( m \) of its values \( \alpha_j \) are equal to \( \alpha \) This implies that \( p(\alpha) = 0 \) and all derivatives up to order \( m-1 \) at \( \alpha \) also equal zero, indicating the root's multiplicity.

An example will make the idea clear: Let p(z) = (z−5) 3 ã(z+ 2) 8 ã(z−3i)ã(z+ 6).

The polynomial p exhibits a root of order 3 at the value 5, an order 8 root at -2, and simple roots of order 1 at 3i and -6 Additionally, p has simple roots at both 1 and -6.

Sequences of Holomorphic Functions and their Deriva-

A sequence of functions \( g_j \) defined on a common domain \( E \) converges uniformly to a limit function \( g \) if, for every \( \epsilon > 0 \), there exists a number \( N > 0 \) such that for all \( j > N \), the inequality \( |g_j(x) - g(x)| < \epsilon \) holds for every \( x \in E \) This means that the proximity of \( g_j(x) \) to \( g(x) \) does not depend on the choice of \( x \) within the domain \( E \).

Let \( f_j : U \rightarrow \mathbb{C} \) (for \( j = 1, 2, 3, \ldots \)) be a sequence of holomorphic functions defined on an open set \( U \) in \( \mathbb{C} \) If there exists a function \( f : U \rightarrow \mathbb{C} \) such that the sequence \( f_j \) converges uniformly to \( f \) on every compact subset \( E \) of \( U \), then \( f \) is holomorphic on \( U \) Consequently, \( f \) is infinitely differentiable, meaning \( f \in C^\infty(U) \).

Iffj, f, U are as in the preceding paragraph, then, for anyk ∈ {0,1,2, }, we have

3.1 The Derivatives of a Holomorphic Function 43 uniformly on compact sets 1 The proof is immediate from (3.1.1.1), which we derived from the Cauchy integral formula, for the derivative of a holomorphic function.

The Power Series Representation of a Holomorphic Func-

The ideas being considered in this section can be used to develop our under- standing of power series A power series

X∞ j=0 aj(z−P) j (3.1.6.1) is defined to be the limit of its partial sums

We say that the partial sumsconvergeto the sum of the entire series. Any given power series has adisc of convergence More precisely, let r= 1 lim sup j →∞ |aj| 1/j (3.1.6.3)

The power series (3.1.6.2) converges within the disc D(P, r), exhibiting absolute and uniform convergence on any smaller disc D(P, r0) where r0 < r It is important to note that in numerous examples, the sequence demonstrates this behavior.

The sequence |aj|^(1/j) converges as j approaches infinity, allowing us to define r as 1/lim(j→∞)|aj|^(1/j) However, if the sequence {|aj|^(1/j)} does not converge, it is necessary to refer to the formal definition of r For further details, consult sources [KRA3] and [RUD1].

The partial sums of the power series are polynomials that are holomorphic within any disc D(P, r) If the power series converges in the disc D(P, r), we denote the resulting function as f, which represents the limit of the series.

1 It is also common to say that the functions converge normally. uniformly on D(P, r 0 ) We can conclude immediately that f(z) is holomor- phic onD(P, r) Moreover, we know that

A differentiated power series maintains a disc of convergence that is at least as large as that of the original series, centered at the same point Within this disc, the differentiated power series converges to the derivative of the sum of the original series.

In complex function theory, a key aspect of power series is that if \( f \) is a holomorphic function defined on a domain \( U \subseteq \mathbb{C} \), and \( P \) is a point within \( U \) such that the disk \( D(P, r) \) is entirely contained in \( U \), then \( f \) can be expressed as a convergent power series within that disk Specifically, this is represented by the formula \( f(z) = \sum_{j=0}^{\infty} a_j(z - P)^j \), where the coefficients \( a_j \) are determined by \( a_j = \frac{f^{(j)}(P)}{j!} \).

The formula presented allows for the explicit calculation of the power series expansion of any holomorphic function f around a point P within its domain Additionally, it provides a priori knowledge regarding the convergence disc of the power series representation.

The topic warrants deeper exploration, particularly regarding Taylor series expansions of smooth functions While every smooth function \( f(x) \) can be expressed as a Taylor series around any point \( p \) within its domain, this series often fails to converge, and even when it does, it may not equal \( f \) In contrast, holomorphic functions of a complex variable exhibit a significant difference: their Taylor or power series expansions consistently converge The proof of this is straightforward, as demonstrated by applying the Cauchy formula with the center of the disc set at the origin.

The Zeros of a Holomorphic Function

The Zero Set of a Holomorphic Function

If \( f \) is a holomorphic function that is not identically zero, it cannot have too many zeros, reflecting the principle that holomorphic functions share characteristics with polynomials To articulate this idea clearly, we must consider the topological concept of connectedness.

Discreteness of the Zeros of a Holomorphic Function

Let U ⊆C be a connected (§§1.1.5) open set and let f :U →C be holomorphic Let the zero set of f beZ ={z ∈U :f(z) = 0}.

If there are a z0 ∈ Z and {zj} ∞ j=1 ⊆ Z \ {z0} such that zj →z0, then f ≡0.

In topological terms, a point \( z_0 \) is considered an accumulation point of a set \( Z \) if there exists a sequence \( \{z_j\} \subset Z \setminus \{z_0\} \) such that \( \lim_{j \to \infty} z_j = z_0 \) The theorem can be restated as follows: if \( f: U \to \mathbb{C} \) is a holomorphic function defined on a connected open set \( U \), and if the set \( Z = \{ z \in U : f(z) = 0 \} \) contains an accumulation point in \( U \), then it follows that \( f \equiv 0 \).

If the point 0 is an interior accumulation point of the zeros {zj} of the holomorphic function f, then f(0) must equal 0 This allows us to express f(z) as z^a f*(z), where f* also vanishes at {zj}, indicating that 0 remains an accumulation point of these zeros Consequently, we find that f*(0) = 0, leading to the conclusion that f has a zero of order 2 at 0 By continuing this process, we can determine that f has a zero of infinite order at 0, resulting in the power series expansion of f around 0 being identically 0 This implies, through a straightforward connectedness argument, that f is identically equal to 0.

Discrete Sets and Zero Sets

In the study of holomorphic functions, a set is defined as discrete if each point in the set has a neighborhood that contains no other points from the set This concept leads to the understanding that the zero set of a non-constant holomorphic function on a connected open set consists of isolated points However, it is crucial to note that this does not exclude the possibility of accumulation points existing outside the open set For example, the function \( f(z) = \sin(1/[1-z]) \) demonstrates that zeros can accumulate at the boundary of the unit disc, specifically at the point 1.

3.2 The Zeros of a Holomorphic Function 47

Figure 3.3: Zeros accumulating at a boundary point.

Uniqueness of Analytic Continuation

A consequence of the preceding basic fact (§§3.2.2) about the zeros of a holomorphic function is this: Let U ⊆ C be a connected open set and D(P, r) ⊆ U If f is holomorphic on U and f

U In fact if f ≡0 on a segment then it must follows that f ≡0.

Here are some further corollaries:

(3.2.4.1) Let U ⊆ C be a connected open set Let f, g be holomorphic on

U If {z∈U :f(z) =g(z)} has an accumulation point inU, then f ≡g. (3.2.4.2)LetU ⊆Cbe a connected open set and letf, g be holomorphic on

U If fãg ≡0 on U, then eitherf ≡0 on U or g ≡0 on U.

(3.2.4.3) Let U ⊆ C be connected and open and let f be holomorphic on

U If there is a P ∈U such that

If f and g are entire holomorphic functions such that f(x) = g(x) for all real x, then it follows that f is identically equal to g Additionally, functional identities that hold for all real values also extend to complex values For example, the identity sin²z + cos²z = 1 is valid for all z in the complex plane, as it is true for all real numbers x.

“principle of persistence of functional relations”—see [GRK].

3.2 The Zeros of a Holomorphic Function 49

Figure 3.4: Principle of persistence of functional relations.

The Behavior of a Holomorphic Function near an Isolated Sin-

Isolated Singularities

It is often important to consider a function that is holomorphic on a punc- tured open setU \ {P} ⊂C Refer to Figure 4.1.

This chapter introduces a novel infinite series expansion that extends the concept of power series expansion for holomorphic functions around nonsingular points Additionally, it provides a comprehensive classification of the behavior of holomorphic functions in the vicinity of isolated singular points.

A Holomorphic Function on a Punctured Domain

In the context of complex analysis, let U be an open set in the complex plane, and let P be a point within U The set U \ {P} is referred to as a punctured domain When a function f is holomorphic on this punctured domain, we describe P as an isolated singular point of f This terminology indicates that f remains defined and holomorphic in a neighborhood surrounding P, excluding the point itself While the specific characteristics of the open set U are of secondary importance, our primary focus lies in analyzing the behavior of the function f near the isolated singularity at P.

Classification of Singularities

There are three possibilities for the behavior of f near P that are worth distinguishing:

(4.1.3.1) |f(z)| is bounded onD(P, r)\ {P}for some r >0 with D(P, r) ⊆

U; i.e., there is some r > 0 and some M > 0 such that |f(z)| ≤ M for all z ∈U ∩D(P, r)\ {P}.

Elementary logic indicates that these three conditions encompass all possibilities Although the description in (4.1.3.3) may seem unsatisfactory, it highlights a complex situation that lacks a straightforward explanation We will delve deeper into each of these three conditions in the following discussion.

4.1 Behavior Near an Isolated Singularity 53

Removable Singularities, Poles, and Essential Singu-

If condition (4.1.3.1) is satisfied, then the function f has a limit at point P, allowing it to be extended and become holomorphic throughout the region U, which is a result established by Riemann In this scenario, f is described as having a removable singularity at P Conversely, if condition (4.1.3.2) applies, f is characterized as having a pole at P Lastly, in the case of condition (4.1.3.3), f is said to exhibit an essential singularity at P.

P.Our goal in this and the next two subsections is to understand (4.1.3.1)–(4.1.3.3)in some further detail.

The Riemann Removable Singularities Theorem

Letf :D(P, r)\ {P} →Cbe holomorphic and bounded Then

(4.1.5.2) The function fb:D(P, r)→C defined by fb(z) ( f(z) if z 6=P ζlim→ Pf(ζ) if z =P is holomorphic.

To prove the statement, let P = 0 and define the function g(z) = z²f(z) It can be verified that g is continuously differentiable (C¹) and satisfies the Cauchy-Riemann equations throughout the disk D(P, r) The boundedness condition ensures that both g and its first derivative approach a limit at 0 Consequently, g is holomorphic within the disk and has a zero of second order at 0 Therefore, the function f(z) = g(z)/z² is also a well-defined holomorphic function across the entire disk D(P, r).

The Casorati-Weierstrass Theorem

If f : D(P, r0)\ {P} → C is holomorphic and P is an essential singularity of f, then f(D(P, r) \ {P}) is dense in C for any

Assuming the assertion is false, we find a complex value and a positive number such that the image of D(P, r) \ {P} under the function f does not include the disc D(à, ) Consequently, the function g(z) = 1/[f(z)−à] remains bounded and non-vanishing near P, indicating that it possesses a removable singularity This leads us to conclude that f is bounded near P, which contradicts our initial assumption.

At a removable singularity P, a holomorphic function f defined on D(P, r0) \ {P} can be extended to be holomorphic on the entire domain D(P, r0) In contrast, near an essential singularity at P, a holomorphic function g on D(P, r0) \ {P} exhibits a dense image in the complex plane C The third scenario, where a holomorphic function h has a pole at P, will be explored in greater detail in the following sections.

We next develop a new type of doubly infinite series that will serve as a tool for understanding isolated singularities—especially poles.

Expansion around Singular Points

Laurent Series

A Laurent series on D(P, r) is a (formal) expression of the form

Note that the individual terms are each defined for all z ∈ D(P, r)\ {P}.The series sums fromj =−∞ toj = +∞.

Convergence of a Doubly Infinite Series

To discuss convergence of Laurent series, we must first make a general agree- ment as to the meaning of the convergence of a “doubly infinite” series

P+ ∞ j= −∞αj We say that such a series converges if P+ ∞ j=0αj and P+ ∞ j=1α − j P − 1 j= −∞αj converge in the usual sense In this case, we set

In other words, the question of convergence for a bi-infinite series devolves to two separate questions about two sub-series.

We can now present the analogues for Laurent series of our basic results for power series.

Annulus of Convergence

The convergence set of a Laurent series can be described as an open set of the form {z: 0≤r1

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