Singularities of Complex Functions Thursday, November 07, 2013 1:56 PM

Total Page:16

File Type:pdf, Size:1020Kb

Singularities of Complex Functions Thursday, November 07, 2013 1:56 PM Singularities of Complex Functions Thursday, November 07, 2013 1:56 PM Homework 3 due Friday, November 15 at 5 PM. From last time, we saw that if we have in hand a function that is known to be analytic over some annular domain, then one can represent that function as a Laurent series which is convergent over that annulus and uniformly convergent over any compact subset of that annulus. In particular, if a function is known to be analytic over an open disc, then one can write a Taylor series representation for that function which converges over that disc, and is uniformly convergent over any compact subset. One interesting consequence of this theorem is it gives an alternative, and often easier way of determining the radius of convergence of a Taylor series, other than using the root test. In particular, a Taylor series representation of an analytic function, centered at a point will have a radius of convergence equal to the distance to the nearest singularity (point where analyticity fails). This property is not true for real analytic functions. Consider the complex analytic function Imagine we compute the Taylor series for this function about Because Taylor series representations are unique, any way we get the Taylor series through power series manipulations is OK, within the radius of convergence. So for example, expand it as a geometric series: Radius of convergence by root test: This simple geometric observation doesn't work on real analytic functions. Consider the real- valued function New Section 2 Page 1 valued function The real-valued Taylor series will be the same (with x instead of z), so its radius of convergence will be the same. But the function itself has no singularities on the real axis. In addition to analytic functions being shown to have Taylor series representations expanded about arbitrary points of analyticity, one can show conversely that a convergent power series (Taylor series) defines an analytic function. That is, if we're given a power series: and we show (by say the root test) that this converges over a domain at least as big as then this power series defines an analytic function inside that domain, whose derivatives can be obtained by differentiating the power series term by term. Proof: By the Weierstrass M-test we know that the power series will actually converge uniformly over any closed bounded region if Notice that each term in the power series is analytic. A uniformly convergent series of analytic functions must itself be analytic because of Morera's theorem. Therefore the power series defines an analytic function on but is any number so we have analyticity on The fact that the derivative of the power series is simply the sum of the derivatives: because one can use the Cauchy integral formula for the derivative and interchange integrals and sums by uniform convergence. Between these theorems, and Cauchy's theorem, and Morera's theorem, we see that there are three equivalent ways to characterize analyticity (holomorphicity) over a open domain: • Existence of the complex derivative over the open domain • The integral of the function over any closed contour in the domain is zero • The ability to express the function as a power series anywhere within the domain. The interaction of power series with analyticity enables an interesting procedure called analytic continuation which can take a power series representation of a function, with only a limited domain of convergence, and extend it to define an analytic function over a broader domain of the complex plane. More generally analytic continuation is a way to extend a limited domain of definition of a complex function to a broader domain. Analytic continuation can be shown to prescribe a unique analytic function over the broader domain so long as it remains simply connected. But sometimes (very important in practice) the analytic continuation New Section 2 Page 2 connected. But sometimes (very important in practice) the analytic continuation leads to a multivalued function. Simple example: imagine power series expansions of Log z. This is the notion of monodromy. One other consequence of note from the above developments is that Laurent series can be added, multiplied, composed, integrated, differentiated by formal series manipulations within their domain of convergence, justified by uniform convergence and the special consideration for differentiation. Singularities of Complex Functions If singularities of complex functions are not isolated, then no particular good theory. Isolated: the function is analytic in a punctured neighborhood of the singularity : Examples of non-isolated singularities: • has a non-isolated singularity at z=0: Cluster singularity You can find examples of natural barriers in the texts corresponding to certain power series. New Section 2 Page 3 But isolated singularities have a good comprehensive theory because one can develop a Laurent series representation of the complex function at least over the punctured neighborhood of analyticity of that singularity. And therefore one can classify isolated singularities by the behavior of the Laurent series in this punctured neighborhood. converges absolutely over a punctured neighborhood and uniformly over any compact subset of this neighborhood. Principal part of the Laurent series is Three cases: 1. There is no principal part ( if ): removable singularity 2. The principal part has a finite number of nonzero terms: pole 3. The principal part has infinitely many nonzero terms: essential singularity Removable singularity: Example: We'll show later that: converge for Has no principal part. But we might have been hesitant to say that was analytic at z=0 because it looks like we're dividing by zero there. The apparent singularity at z=0 can easily be removed by simply defining the function to take the value at the singularity by using the Laurent series (which just looks like a Taylor series) and plugging in the value of z at the removable singularity. In other words, there is no problem in simply extending the definition of the Laurent series to be a Taylor series by continuous extension to the removable singularity (here at z=0). New Section 2 Page 4 (here at z=0). By defining We get an analytic function defined on the non-punctured neighborhood and represented by the Taylor series (which is the same as the Laurent series). Note in particular that since the Laurent series will have a well-defined limit at the removable singularity, a Laurent series is bounded near a removable singularity. Poles: Principal part of the Laurent series about a pole has the form: N is the order of the pole is the strength of the pole. Examples of functions with poles: Notice that if f(z) has a pole of order N, then will have a removable singularity at , and has a limit there. So, by unwinding the defintion of continuity, etc.: Given any when R is the outer radius of convergence of the Laurent series, there exist constants such that: New Section 2 Page 5 That is, at a pole, a function diverges as a negative power law with exponent equal to the order of the pole. Actually this is fairly nice behavior on the Riemann sphere; it implies that: at a pole . Essential singularity Two theorems that characterize how nasty functions behave near essential singularities: Casarati-Weierstrass theorem: At an essential singularity, one can specify any complex value on the extended complex plane and a tolerance and one can find arbitrarily small neighborhoods of the essential singularity where . Picard theorem: In any neighborhood of an essential singularity, the complex function will assume every value on the complex plane, except possibly for one value. Removable singularity Pole Essential singularity Prototype example of an essential singularity is at z=0. New Section 2 Page 6 Principal part has infinitely many negative terms. Let's see how Picard theorem applies to this function. Realize that, by elementary properties of exponential function: In a neighborhood the function will cover the exterior of a disc of radius One other note: What about branch points? They don't even have Laurent series representations about them because...they're multivalued. To analyze them in the same way requires the use of Puiseux series (fractional powers); can be done but we won't. New Section 2 Page 7 .
Recommended publications
  • Global Subanalytic Cmc Surfaces
    GLOBALLY SUBANALYTIC CMC SURFACES IN R3 WITH SINGULARITIES JOSE´ EDSON SAMPAIO Abstract. In this paper we present a classification of a class of globally sub- 3 analytic CMC surfaces in R that generalizes the recent classification made by Barbosa and do Carmo in 2016. We show that a globally subanalytic CMC 3 surface in R with isolated singularities and a suitable condition of local con- nectedness is a plane or a finite union of round spheres and right circular cylinders touching at the singularities. As a consequence, we obtain that a 3 globally subanalytic CMC surface in R that is a topological manifold does not have isolated singularities. It is also proved that a connected closed glob- 3 ally subanalytic CMC surface in R with isolated singularities which is locally Lipschitz normally embedded needs to be a plane or a round sphere or a right circular cylinder. A result in the case of non-isolated singularities is also pre- sented. It is also presented some results on regularity of semialgebraic sets and, in particular, it is proved a real version of Mumford's Theorem on regu- larity of normal complex analytic surfaces and a result about C1 regularity of minimal varieties. 1. Introduction The question of describing minimal surfaces or, more generally, surfaces of con- stant mean curvature (CMC surfaces) is known in Analysis and Differential Geom- etry since the classical papers of Bernstein [4], Bombieri, De Giorgi and Giusti [9], Hopf [26] and Alexandrov [1]. Recently, in the paper [2], Barbosa and do Carmo showed that the connected algebraic smooth CMC surfaces in R3 are only the planes, round spheres and right circular cylinders.
    [Show full text]
  • 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.
    [Show full text]
  • 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]
  • Residue Theorem
    Topic 8 Notes Jeremy Orloff 8 Residue Theorem 8.1 Poles and zeros f z z We remind you of the following terminology: Suppose . / is analytic at 0 and f z a z z n a z z n+1 ; . / = n. * 0/ + n+1. * 0/ + § a ≠ f n z n z with n 0. Then we say has a zero of order at 0. If = 1 we say 0 is a simple zero. f z Suppose has an isolated singularity at 0 and Laurent series b b b n n*1 1 f .z/ = + + § + + a + a .z * z / + § z z n z z n*1 z z 0 1 0 . * 0/ . * 0/ * 0 < z z < R b ≠ f n z which converges on 0 * 0 and with n 0. Then we say has a pole of order at 0. n z If = 1 we say 0 is a simple pole. There are several examples in the Topic 7 notes. Here is one more Example 8.1. z + 1 f .z/ = z3.z2 + 1/ has isolated singularities at z = 0; ,i and a zero at z = *1. We will show that z = 0 is a pole of order 3, z = ,i are poles of order 1 and z = *1 is a zero of order 1. The style of argument is the same in each case. At z = 0: 1 z + 1 f .z/ = ⋅ : z3 z2 + 1 Call the second factor g.z/. Since g.z/ is analytic at z = 0 and g.0/ = 1, it has a Taylor series z + 1 g.z/ = = 1 + a z + a z2 + § z2 + 1 1 2 Therefore 1 a a f .z/ = + 1 +2 + § : z3 z2 z This shows z = 0 is a pole of order 3.
    [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]
  • Compex Analysis
    ( ! ) 1. The amplitu.e of a comple2 number isisis a) 0 b) 89: c) 8 .) :8 2.The amplitu.e of the quotient of two comple2 numbers is a) the sum of their amplitu.es b) the .ifference of their amplitu.es c) the pro.uct of their amplitu.es .) the quotient of their amplitu.es 3. The ? = A B then ?C = : : : : : : a) AB b) A B c) DB .) imaginary J ? K ?: J 4. If ? I ?: are any two comple2 numbers, then J ?.?: J isisis J ? K ?: J J ? K ?: J J ? K ?: J J J J J a)a)a) J ?: J b) J ?. J c) J ?: JJ? J .) J ? J J ?: J : : 555.5...MNO?P:Q: A B R = a) S b) DS c) T .) U 666.The6.The equation J? A UJ A J? D UJ = W represents a) Circle b) ellipse c) parparabolaabola .) hyperbola 777.The7.The equation J? A ZJ = J? D ZJ represents a) Circle b) ellipse c) parparabolaabola .) Real a2is 888.The8.The equation J? A J = ]:J? D J represents a) Circle b) ellipse c) parparabolaabola .) hyperbola 999.The9.The equation J?A:J A J?D:J = U represents a) Circle b) a st. line c) parabola .) hyperbohyperbolalalala 101010.The10.The equation J:? D J = J?D:J represents a) Circle b) a st. line c) parabola .) hyperbola : : 111111.The11.The equation J? D J A J?D:J = U represents a) Circle b) a st. line c) parabola .) hyperbola ?a 121212.The12.The equation !_ `?a b = c represents a) Circle b) a st.
    [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 Notes Lent 2006 T. K. Carne
    Department of Pure Mathematics and Mathematical Statistics University of Cambridge COMPLEX ANALYSIS Notes Lent 2006 T. K. Carne. [email protected] c Copyright. Not for distribution outside Cambridge University. CONTENTS 1. ANALYTIC FUNCTIONS 1 Domains 1 Analytic Functions 1 Cauchy – Riemann Equations 1 2. POWER SERIES 3 Proposition 2.1 Radius of convergence 3 Proposition 2.2 Power series are differentiable. 3 Corollary 2.3 Power series are infinitely differentiable 4 The Exponential Function 4 Proposition 2.4 Products of exponentials 5 Corollary 2.5 Properties of the exponential 5 Logarithms 6 Branches of the logarithm 6 Logarithmic singularity 6 Powers 7 Branches of powers 7 Branch point 7 Conformal Maps 8 3. INTEGRATION ALONG CURVES 9 Definition of curves 9 Integral along a curve 9 Integral with respect to arc length 9 Proposition 3.1 10 Proposition 3.2 Fundamental Theorem of Calculus 11 Closed curves 11 Winding Numbers 11 Definition of the winding number 11 Lemma 3.3 12 Proposition 3.4 Winding numbers under perturbation 13 Proposition 3.5 Winding number constant on each component 13 Homotopy 13 Definition of homotopy 13 Definition of simply-connected 14 Definition of star domains 14 Proposition 3.6 Winding number and homotopy 14 Chains and Cycles 14 4 CAUCHY’S THEOREM 15 Proposition 4.1 Cauchy’s theorem for triangles 15 Theorem 4.2 Cauchy’s theorem for a star domain 16 Proposition 4.10 Cauchy’s theorem for triangles 17 Theorem 4.20 Cauchy’s theorem for a star domain 18 Theorem 4.3 Cauchy’s Representation Formula 18 Theorem 4.4 Liouville’s theorem 19 Corollary 4.5 The Fundamental Theorem of Algebra 19 Homotopy form of Cauchy’s Theorem.
    [Show full text]
  • Laurent Series and Residue Calculus
    Laurent Series and Residue Calculus Nikhil Srivastava March 19, 2015 If f is analytic at z0, then it may be written as a power series: 2 f(z) = a0 + a1(z − z0) + a2(z − z0) + ::: which converges in an open disk around z0. In fact, this power series is simply the Taylor series of f at z0, and its coefficients are given by I 1 (n) 1 f(z) an = f (z0) = n+1 ; n! 2πi (z − z0) where the latter equality comes from Cauchy's integral formula, and the integral is over a positively oriented contour containing z0 contained in the disk where it f(z) is analytic. The existence of this power series is an extremely useful characterization of f near z0, and from it many other useful properties may be deduced (such as the existence of infinitely many derivatives, vanishing of simple closed contour integrals around z0 contained in the disk of convergence, and many more). The situation is not much worse when z0 is an isolated singularity of f, i.e., f(z) is analytic in a puncured disk 0 < jz − z0j < r for some r. In this case, we have: Laurent's Theorem. If z0 is an isolated singularity of f and f(z) is analytic in the annulus 0 < jz − z0j < r, then 2 b1 b2 bn f(z) = a0 + a1(z − z0) + a2(z − z0) + ::: + + 2 + ::: + n + :::; (∗) z − z0 (z − z0) (z − z0) where the series converges absolutely in the annulus. In class I described how this can be done for any annulus, but the most useful case is a punctured disk around an isolated singularity.
    [Show full text]
  • Lecture #31: the Cauchy Residue Theorem
    Mathematics312(Fall2013) November25,2013 Prof. Michael Kozdron Lecture #31: The Cauchy Residue Theorem Recall that last class we showed that a function f(z)hasapoleoforderm at z0 if and only if g(z) f(z)= (z z )m − 0 for some function g(z)thatisanalyticinaneighbourhoodofz and has g(z ) =0.Wealso 0 0 derived a formula for Res(f; z0). Theorem 31.1. If f(z) is analytic for 0 < z z0 <Rand has a pole of order m at z0, then | − | m 1 m 1 1 d − m 1 d − m Res(f; z0)= m 1 (z z0) f(z) = lim m 1 (z z0) f(z). (m 1)! dz − − (m 1)! z z0 dz − − z=z0 → − − In particular, if z0 is a simple pole, then Res(f; z0)=(z z0)f(z) =lim(z z0)f(z). − z z0 − z=z0 → Example 31.2. Suppose that sin z f(z)= . (z2 1)2 − Determine the order of the pole at z0 =1. Solution. Observe that z2 1=(z 1)(z +1)andso − − sin z sin z sin z/(z +1)2 f(z)= = = . (z2 1)2 (z 1)2(z +1)2 (z 1)2 − − − Since sin z g(z)= (z +1)2 2 is analytic at 1 and g(1) = 2− sin(1) =0,weconcludethatz =1isapoleoforder2. 0 Example 31.3. Determine the residue at z0 =1of sin z f(z)= (z2 1)2 − and compute f(z)dz C where C = z 1 =1/2 is the circle of radius 1/2centredat1orientedcounterclockwise. {| − | } 31–1 Solution. Since we can write (z 1)2f(z)=g(z)where − sin z g(z)= (z +1)2 is analytic at z =1withg(1) =0,theresidueoff(z)atz =1is 0 0 1 d2 1 d Res(f;1)= − (z 1)2f(z) = (z 1)2f(z) (2 1)! dz2 1 − dz − − − z=1 z=1 d sin z = dz (z +1)2 z=1 (z +1)2 cosz 2(z +1)sinz = − (z +1)4 z=1 4cos1 4sin1 = − 16 cos 1 sin 1 = − .
    [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]