CHAPTER 7 Classification of Singularities Dr. Pulak Sahoo

Total Page:16

File Type:pdf, Size:1020Kb

CHAPTER 7 Classification of Singularities Dr. Pulak Sahoo CHAPTER 7 Classification of Singularities BY Dr. Pulak Sahoo Assistant Professor Department of Mathematics University Of Kalyani West Bengal, India E-mail : sahoopulak1@gmail:com 1 Module-2: Zeros of an Analytic Function Definition 1. If z0 is a regular point of an analytic function f and if f(z0) = 0, then z0 is called a zero of f. The point z0 is called a zero of f of order m if in some neighbourhood of z0, f can be expanded in a Taylor series of the form 1 X n f(z) = an(z − z0) ; where am 6= 0: n=m Theorem 1. A point z = z0 is a zero of f of order m if and only if in some neighbourhood m of z0, f can be expressed in the form f(z) = (z − z0) φ(z), where φ(z) is analytic at z0 and φ(z0) 6= 0. Proof. First we assume that z0 is a zero of f of order m. Then in some neighbourhood of z0 we can expand f as 1 X n f(z) = an(z − z0) ; where am 6= 0: n=m Then 1 m X n−m f(z) = (z − z0) an(z − z0) n=m 1 m X p = (z − z0) bp(z − z0) ; where n − m = p and bp = ap+m p=0 m = (z − z0) φ(z); 1 X p where φ(z) = bp(z − z0) is analytic at z0 and φ(z0) = b0 = am 6= 0: p=0 Next we assume that in some neighbourhood of z0, f can be expressed as f(z) = m (z − z0) φ(z), where φ(z) is analytic at z0 and φ(z0) 6= 0. Then we can expand φ(z) in 2 Taylor series about z0 to obtain 1 X n φ(z) = an(z − z0) ; where a0 = φ(z0) 6= 0: n=0 Therefore, in some neighbourhood of z0, we have 1 1 m X n X n+m f(z) = (z − z0) an(z − z0) = an(z − z0) n=0 n=0 1 X p = bp(z − z0) ; where m + n = p and bp = ap−m: p=m Since bm = a0 6= 0; z0 is a zero of f of order m. This proves the theorem. Theorem 2. The zeros of a nonconstant analytic function are isolated points. Proof. Let z0 be a zero of f of order m. Then in some neighbourhood of z0, f can be m expressed in the form f(z) = (z − z0) φ(z), where φ(z) is analytic at z0 and φ(z0) 6= 0. 1 Let " = 2 j φ(z0) j> 0. Since φ(z) is continuous at z0, there exists δ > 0 such that 1 j φ(z) − φ(z ) j < " = j φ(z ) j whenever j z − z j < δ: 0 2 0 0 Therefore, 1 j φ(z ) j − j φ(z) j ≤| φ(z) − φ(z ) j < j φ(z ) j whenever j z − z j < δ: 0 0 2 0 0 1 From this we obtain 2 j φ(z0) j <j φ(z) j whenever j z − z0 j < δ: This means that φ(z) 6= 0 in j z −z0 j < δ: Hence f cannot vanish in 0 <j z −z0 j < δ: Thus z0 is an isolated zero of f. z0 being arbitrary, we thus conclude that the zeros of an analytic function are isolated points. This proves the theorem. Theorem 3. The number of zeros of an analytic function (not identically zero) interior to a simple closed contour are finite. Proof. If possible, we may assume that f(z) has infinite number of zeros inside a region en- closed by a closed contour. The region being bounded and closed, by Bolzano-Weierstrass theorem any sequence of zeros fa1; a2;::: g in the region has a limit point in the region. Let a be the limit point of the sequence, i.e. there exists a subsequence fank g such that ank ! a as k ! 1: This implies f(a) = lim f(an ) = 0: k!1 k 3 Therefore, a is a zero of the function, and in every neighbourhood of a, however small it may be, there are infinitely many zeros. This means that a is not isolated which contradicts the fact that the zeros of an analytic function are isolated points. Hence, the number of zeros of an analytic function interior to a simple closed contour are finite. This proves the theorem. Note 1. If f(z) and g(z) are analytic at z0 and have zeros of order m and n, respectively, then the product function h(z) = f(z)g(z) has a zero of order m + n at z0. Example 1. Find order of zero of the function f(z) = z4 sin z at z = 0. Solution. At z = 0, the function z4 has a zero of order 4 and the function sin z has zero of order 1. Therefore, the function f(z) = z4 sin z has a zero of order 4 + 1 = 5 at z = 0: Theorem 4. (Weierstrass and Casorati Theorem) If f(z) has an isolated essential singularity at z = z0, then f(z) comes arbitrarily close to every complex value in each deleted neighbourhood of z0 . Proof. Since z = z0 is an isolated essential singularity of f(z), it is analytic throughout a deleted neighbourhood of z0. Suppose, for some complex number c, that j f(z) − c j ≥ " > 0 1 for all z in a punctured disk 0 <j z − z0 j< δ: Let g(z) = f(z)−c : Then 1 1 j g(z) j =j j ≤ for 0 <j z − z j< δ: f(z) − c " 0 Hence by Riemann's theorem, g(z) has a removable singularity at z0 and we may write 1 g(z) = = a + a (z − z ) + a (z − z )2 + :::: f(z) − c 0 1 0 2 0 Observe that limz!z0 1=(f(z) − c) = a0: Now we consider two cases. Case (i). a0 6= 0: Then limz!z0 f(z) = c + 1=a0; and f(z) has a removable singularity at z0; a contradiction. Case (ii). a0 = 0. Assume that ak is the first nonzero coefficient. Then 1 2 k = ak + ak+1(z − z0) + ak+2(z − z0) + :::: (f(z) − c)(z − z0) 4 Therefore, k 1 lim (z − z0) (f(z) − c) = 6= 0; z!z0 ak and f(z) has a pole of order k at z0; a contradiction. This proves the theorem. Corollary 1. Suppose that f(z) has an isolated essential singularity at z0. Given any complex number c, there exists a sequence fzng such that zn ! z0 and f(zn) ! c: Proof. We choose a sequence fδng for which δn > 0 for each n and lim δn = 0: Therefore n!1 by Weierstrass-Casorati theorem, we can find a sequence of points fzng such that j f(zn) − c j < 1=n for 0 <j zn − z0 j< δn: Thus, f(zn) ! c as zn ! z0. This proves the corollary. Theorem 5. A point z0 is a pole of order m of a function f if and only if it is a zero of order m of the function 1=f. Proof. First we assume that z0 is a pole of f of order m. Then in some neighbourhood of z0, we can write g(z) f(z) = m (z − z0) 1 m 1 where g is analytic at z0 and g(z0) 6= 0: Therefore, f(z) = (z−z0) h(z) where h(z) = g(z) is analytic at z0 and h(z0) 6= 0: This shows that z0 is a zero of 1=f of order m. Next we assume that z0 is a zero of 1=f of order m. Then in some neighbourhood of z0, we can write 1 = (z − z )mg(z) f(z) 0 h(z) 1 where g is analytic at z0 and g(z0) 6= 0: Then f(z) = m where h(z) = is (z−z0) g(z) analytic at z0 and h(z0) 6= 0: This shows that z0 is a pole of f of order m. Theorem 6. If a function f has an essential singularity at z0, then the function 1=f has also an essential singularity at z0. Proof. If possible, we assume that z0 is a regular point of 1=f and it is not a zero of 1=f. Then z0 is a regular point of f contradicting the nature of z0. 5 Let z0 be a regular point of 1=f and it is a zero of 1=f of order m. Then z0 is a pole of f of order m which contradicts the nature of z0. Let z0 be a pole of 1=f of order m. Then z0 is a zero of f of order m which contradicts the nature of z0. Therefore the only possibility that remains for z0 is to be essential singularity of 1=f: Singularities at Point at Infinity 1 The behavior of a function f(z) at z = 1 is considered by making the substitution z = w and examining the nature of f(1=w) at w = 0. It is to be noted that f(z) is regular or has a pole or has an essential singularity at z = 1 if f(1=w) has the same property at w = 0: For instance, the function f(z) = z2 has a pole of order 2 at z = 1. Again the function f(z) = ez has an essential singularity at z = 1, since f(1=w) = e1=w has an essential singularity at w = 0: Theorem 7.
Recommended publications
  • Complex Analysis Class 24: Wednesday April 2
    Complex Analysis Math 214 Spring 2014 Fowler 307 MWF 3:00pm - 3:55pm c 2014 Ron Buckmire http://faculty.oxy.edu/ron/math/312/14/ Class 24: Wednesday April 2 TITLE Classifying Singularities using Laurent Series CURRENT READING Zill & Shanahan, §6.2-6.3 HOMEWORK Zill & Shanahan, §6.2 3, 15, 20, 24 33*. §6.3 7, 8, 9, 10. SUMMARY We shall be introduced to Laurent Series and learn how to use them to classify different various kinds of singularities (locations where complex functions are no longer analytic). Classifying Singularities There are basically three types of singularities (points where f(z) is not analytic) in the complex plane. Isolated Singularity An isolated singularity of a function f(z) is a point z0 such that f(z) is analytic on the punctured disc 0 < |z − z0| <rbut is undefined at z = z0. We usually call isolated singularities poles. An example is z = i for the function z/(z − i). Removable Singularity A removable singularity is a point z0 where the function f(z0) appears to be undefined but if we assign f(z0) the value w0 with the knowledge that lim f(z)=w0 then we can say that we z→z0 have “removed” the singularity. An example would be the point z = 0 for f(z) = sin(z)/z. Branch Singularity A branch singularity is a point z0 through which all possible branch cuts of a multi-valued function can be drawn to produce a single-valued function. An example of such a point would be the point z = 0 for Log (z).
    [Show full text]
  • 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.
    [Show full text]
  • Lecture 18: Analytic Functions and Integrals
    Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas) This is a good point to take a brief detour and expand on our previous discussions of complex variables and complex functions of complex variables. In particular, we want to consider the properties of so-called analytic functions, especially those properties that allow us to perform integrals relevant to evaluating an inverse Fourier transform. More generally we want to motivate the process of thinking about the functions that appear in physics in terms of their properties in the complex plane (where “real life” is the real axis). In the complex plane we can more usefully define a well “behaved function”; we want both the function and its derivative to be well defined. Consider a complex valued function of a complex variable defined by F z U x,,, y iV x y (17.1) where UV, are real functions of the real variables xy, . The function Fz is said to be analytic (or regular or holomorphic) in a region of the complex plane if, at every (complex) point z in the region, it possesses a unique (finite) derivative that is independent of the direction in the complex plane along which we take the derivative. (This implies that there is always a, perhaps small, region around every point of analyticity within which the derivatives exist.) This property of the function is summarized by the Cauchy-Riemann conditions, i.e., a function is analytic/regular at the point z x iy if and only if (iff) UVVU , (17.2) x y x y at that point.
    [Show full text]
  • Complex Analysis in a Nutshell
    Complex analysis in a nutshell. Definition. A function f of one complex variable is said to be differentiable at z0 2 C if the limit f(z) − f(z ) lim 0 z z0 ! z − z0 exists and does not depend on the manner in which the variable z 2 C approaches z0. Cauchy-Riemann equations. A function f(z) = f(x; y) = u(x; y) + iv(x; y) (with u and v the real and the imaginary parts of f respectively) is differentiable at z0 = x0 + iy0 if and only if it satisfies the Cauchy-Riemann equations @u @v @u @v = ; = − at (x ; y ): @x @v @y @x 0 0 Definition. A function f is analytic at z0 if it is differentiable in a neighborhood of z0. Harmonic functions. Let D be a region in IR2 identified with C. A function u : D ! IR is the real (or imaginary) part of an analytic function if and only if it is harmonic, i.e., if it satisfies @2u @2u + = 0: @x2 @y2 Cauchy formulas. Let a function f be analytic in an open simply connected region D, let Γ be a simple closed curve contained entirely in D and traversed once counterclockwise, and let z0 lie inside Γ. Then f(z) dz = 0; IΓ f(z) dz = 2πif(z0); IΓ z − z0 f(z) dz 2πi (n) n+1 = f (z0); n 2 IN: IΓ (z − z0) n! Definition. A function analytic in C is called entire. Zeros and poles. If a function f analytic in a neighborhood of a point z0, vanishes at z0, k and is not identically zero, then f(z) = (z − z0) g(z) where k 2 IN, g is another function analytic in a neighborhood of z0, and g(z0) =6 0.
    [Show full text]
  • Complex Analysis Course Notes
    NOTES FOR MATH 520: COMPLEX ANALYSIS KO HONDA 1. Complex numbers 1.1. Definition of C. As a set, C = R2 = (x; y) x; y R . In other words, elements of C are pairs of real numbers. f j 2 g C as a field: C can be made into a field, by introducing addition and multiplication as follows: (1) (Addition) (a; b) + (c; d) = (a + c; b + d). (2) (Multiplication) (a; b) (c; d) = (ac bd; ad + bc). · − C is an Abelian (commutative) group under +: (1) (Associativity) ((a; b) + (c; d)) + (e; f) = (a; b) + ((c; d) + (e; f)). (2) (Identity) (0; 0) satisfies (0; 0) + (a; b) = (a; b) + (0; 0) = (a; b). (3) (Inverse) Given (a; b), ( a; b) satisfies (a; b) + ( a; b) = ( a; b) + (a; b). (4) (Commutativity) (a; b) +− (c;−d) = (c; d) + (a; b). − − − − C (0; 0) is also an Abelian group under multiplication. It is easy to verify the properties − f g 1 a b above. Note that (1; 0) is the identity and (a; b)− = ( a2+b2 ; a2−+b2 ). (Distributivity) If z ; z ; z C, then z (z + z ) = (z z ) + (z z ). 1 2 3 2 1 2 3 1 2 1 3 Also, we require that (1; 0) = (0; 0), i.e., the additive identity is not the same as the multi- plicative identity. 6 1.2. Basic properties of C. From now on, we will denote an element of C by z = x + iy (the standard notation) instead of (x; y). Hence (a + ib) + (c + id) = (a + c) + i(b + d) and (a + ib)(c + id) = (ac bd) + i(ad + bc).
    [Show full text]
  • COMPLEX ANALYSIS — Example Sheet 2 TKC Lent 2006
    COMPLEX ANALYSIS — Example Sheet 2 TKC Lent 2006 The first set of questions are intended to be short and straightforward, the second set are longer, and the final set are additional exercises for those who have completed the earlier ones. Z ez Z ez 1. Evaluate dz and dz when C(0, 2) is the circle with radius 2, centre 0. C(0,2) z − 1 C(0,2) πi − 2z 2. Prove Liouville’s theorem. The analytic function f : C → C never takes values in the disc D(c, ε) = {z ∈ C : |z − c| < ε}. Prove that f is constant. 3. Let D be a domain in C, c a point in D, and f : D \{c} → C an analytic function. Let T ⊂ D be a closed triangle with boundary ∂D positively oriented. By dividing T into smaller triangles prove that there is a number R, depending on f but not on T , with Z n 0 c∈ / T ; f(z) dz = ◦ ∂T R c ∈ T . Find the value of R for the functions f : z 7→ (z − c)−1 and f : z 7→ (z − c)−2. 4. Let f be an analytic function on a domain which contains the closed disc D(zo,R). Prove that n! |f (n)(z )| sup{|f(z)| : |z − z | = R} . o 6 Rn o Use this to prove Liouville’s Theorem. 5. Give an example of an analytic function f : C \{0} → C that has an essential singularity at 0. For this example, find a sequence of points zn → 0 with f(zn) → 2 as n → ∞.
    [Show full text]
  • Lecture 11 29Th Aug
    Lecture 11 : Isolated Sungularities: continued Application to Evaluation of Real Integrals Trigonometric Integrals Improper Integrals INDIAN INSTITUTE OF TECHNOLOGY BOMBAY MA205 Complex Analysis Autumn 2012 Anant R. Shastri August 29, 2012 Anant R. Shastri IITB MA205 Complex Analysis Lecture 11 : Isolated Sungularities: continued Application to Evaluation of Real Integrals Trigonometric Integrals Improper Integrals Lecture 11 : Isolated Sungularities: continued Essential Singularities Singularity at infinity Residues Application to Evaluation of Real Integrals Trigonometric Integrals Improper Integrals Anant R. Shastri IITB MA205 Complex Analysis I A natural question is what happens when we allow infinitely many terms. I Of course, we need to assume that such an ‘infinite sum' is convergent Lecture 11 : Isolated Sungularities: continued Essential Singularities Application to Evaluation of Real Integrals Singularity at infinity Trigonometric Integrals Residues Improper Integrals Essential Singularity I The singular part of a function around a pole consisted finitely many negative powers of z − a: Anant R. Shastri IITB MA205 Complex Analysis I Of course, we need to assume that such an ‘infinite sum' is convergent Lecture 11 : Isolated Sungularities: continued Essential Singularities Application to Evaluation of Real Integrals Singularity at infinity Trigonometric Integrals Residues Improper Integrals Essential Singularity I The singular part of a function around a pole consisted finitely many negative powers of z − a: I A natural question is what happens when we allow infinitely many terms. Anant R. Shastri IITB MA205 Complex Analysis Lecture 11 : Isolated Sungularities: continued Essential Singularities Application to Evaluation of Real Integrals Singularity at infinity Trigonometric Integrals Residues Improper Integrals Essential Singularity I The singular part of a function around a pole consisted finitely many negative powers of z − a: I A natural question is what happens when we allow infinitely many terms.
    [Show full text]
  • Complex Integration
    Chapter 1 Complex integration 1.1 Complex number quiz 1 1. Simplify 3+4i . 1 2. Simplify | 3+4i |. 3. Find the cube roots of 1. 4. Here are some identities for complex conjugate. Which ones need correc- tion? z + w =z ¯+w ¯, z − w =z ¯− w¯, zw =z ¯w¯, z/w =z/ ¯ w¯. Make suitable corrections, perhaps changing an equality to an inequality. 5. Here are some identities for absolute value. Which ones need correction? |z + w| = |z| + |w|, |z − w| = |z| − |w|, |zw| = |z||w|, |z/w| = |z|/|w|. Make suitable corrections, perhaps changing an equality to an inequality. 6. Define log(z) so that −π < = log(z) ≤ π. Discuss the identities elog(z) = z and log(ew) = w. 7. Define zw = ew log z. Find ii. 8. What is the power series of log(1 + z) about z = 0? What is the radius of convergence of this power series? 9. What is the power series of cos(z) about z = 0? What is its radius of convergence? 10. Fix w. How many solutions are there of cos(z) = w with −π < <z ≤ π. 1 2 CHAPTER 1. COMPLEX INTEGRATION 1.2 Complex functions 1.2.1 Closed and exact forms In the following a region will refer to an open subset of the plane. A differential form p dx + q dy is said to be closed in a region R if throughout the region ∂q ∂p = . (1.1) ∂x ∂y It is said to be exact in a region R if there is a function h defined on the region with dh = p dx + q dy.
    [Show full text]
  • Complex Analysis Fall 2007 Homework 11: Solutions
    Complex Analysis Fall 2007 Homework 11: Solutions k 3.3.16 If f has a zero of multiplicity k at z0 then we can write f(z) = (z − z0) φ(z), where 0 k−1 φ is analytic and φ(z0) 6= 0. Differentiating this expression yields f (z) = k(z − z0) φ(z) + k 0 (z − z0) φ (z). Therefore 0 k−1 k 0 0 f (z) k(z − z0) φ(z) + (z − z0) φ (z) k φ (z) = k = + . f(z) (z − z0) φ(z) z − z0 φ(z) 0 Since φ(z0) 6= 0, the function φ (z)/φ(z) is analytic at z0 and therefore has a convergent Taylor series in a neighborhood of z0. Thus ∞ f 0(z) k φ0(z) k X = + = + a (z − z )n. f(z) z − z φ(z) z − z n 0 0 0 n=0 for all z in a deleted neighborhood of z0. Uniqueness of such expressions implies that this is 0 0 the Laurent series for f /f in a deleted neighborhood of z0 and therefore f /f has a simple pole at z0 with residue k. 3.3.20(a) The closure of a set A is the intersection of all the closed sets that contain A. It is not hard to show that an element belongs to the closure of A if and only if every neighborhood of that point intersects A. Therefore, what we need to prove the following: given any w ∈ C and any > 0, there exists z ∈ U so that f(z) ∈ D(w; ).
    [Show full text]
  • Chapter 4 Complex Analysis
    Chapter 4 Complex Analysis 4.1 Complex Differentiation Recall the definition of differentiation for a real function f(x): f(x + δx) − f(x) f 0(x) = lim . δx→0 δx In this definition, it is important that the limit is the same whichever direction we approach from. Consider |x| at x = 0 for example; if we approach from the right (δx → 0+) then the limit is +1, whereas if we approach from the left (δx → 0−) the limit is −1. Because these limits are different, we say that |x| is not differentiable at x = 0. Now extend the definition to complex functions f(z): f(z + δz) − f(z) f 0(z) = lim . δz→0 δz Again, the limit must be the same whichever direction we approach from; but now there is an infinity of possible directions. Definition: if f 0(z) exists and is continuous in some region R of the complex plane, we say that f is analytic in R. If f(z) is analytic in some small region around a point z0, then we say that f(z) is analytic at z0. The term regular is also used instead of analytic. Note: the property of analyticity is in fact a surprisingly strong one! For example, two consequences include: (i) If a function is analytic then it is differentiable infinitely many times. (Cf. the existence of real functions which can be differentiated N times but no more, for any given N.) 64 © R. E. Hunt, 2002 (ii) If a function is analytic and bounded in the whole complex plane, then it is constant.
    [Show full text]
  • 1. a Maximum Modulus Principle for Analytic Polynomials in the Following Problems, We Outline Two Proofs of a Version of Maximum Mod- Ulus Principle
    PROBLEMS IN COMPLEX ANALYSIS SAMEER CHAVAN 1. A Maximum Modulus Principle for Analytic Polynomials In the following problems, we outline two proofs of a version of Maximum Mod- ulus Principle. The first one is based on linear algebra (not the simplest one). Problem 1.1 (Orr Morshe Shalit, Amer. Math. Monthly). Let p(z) = a0 + a1z + n p 2 ··· + anz be an analytic polynomial and let s := 1 − jzj for z 2 C with jzj ≤ 1. Let ei denote the column n × 1 matrix with 1 at the ith place and 0 else. Verify: (1) Consider the (n+1)×(n+1) matrix U with columns ze1+se2; e3; e4; ··· ; en+1, and se1 − ze¯ 2 (in order). Then U is unitary with eigenvalues λ1; ··· ; λn+1 of modulus 1 (Hint. Check that columns of U are mutually orthonormal). k t k (2) z = (e1) U e1 (Check: Apply induction on k), and hence t p(z) = (e1) p(U)e1: (3) maxjz|≤1 jp(z)j ≤ kp(U)k (Hint. Recall that kABk ≤ kAkkBk) (4) If D is the diagonal matrix with diagonal entries λ1; ··· ; λn+1 then kp(U)k = kp(D)k = max jp(λi)j: i=1;··· ;n+1 Conclude that maxjz|≤1 jp(z)j = maxjzj=1 jp(z)j. Problem 1.2 (Walter Rudin, Real and Complex Analysis). Let p(z) = a0 + a1z + n ··· + anz be an analytic polynomial. Let z0 2 C be such that jf(z)j ≤ jf(z0)j: n Assume jz0j < 1; and write p(z) = b0+b1(z−z0)+···+bn(z−z0) .
    [Show full text]
  • Class 2/14 1 Singularities
    Math 752 Spring 2011 Class 2/14 1 Singularities Definition 1. f has an isolated singularity at z = a if there is a punctured disk B(a, R)\{a} such that f is defined and analytic on this set, but not on the full disk. a is called removable singularity if there is an analytic g : B(a, R) → C such that g(z) = f(z) for 0 < |z − a| < R. Investigation of removable singularities. Example 1. f(z) = z−1 sin z has a removable singularity at the origin. To see this, divide the power expansion of sin z by z. Theorem 1. If f has an isolated singularity at a, then the point z = a is a removable singularity if and only if lim(z − a)f(z) = 0. z→a Proof. Need to show ⇐=: Suppose that f is analytic for 0 < |z − a| < R. Define g(z) = (z − a)f(z) for z 6= a and g(a) = 0, and note that by assumption g is continuous at a. We will show that g is analytic in B(a, R). Since an analytic function has zeros of integer order, it then follows that f is analytic in this disk. We apply Morera’s theorem. Let T be a triangular path in B(a, R), R enclosing the triangle ∆. If a∈ / ∆, then T g = 0. If a is a vertex of ∆, partition ∆ into two triangles, one a very small one with vertex a, and use continuity of g on the smaller to bound the contribution to the integral by ε.
    [Show full text]