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Complex Numbers and the Complex Plane: Why Imaginary Numbers Became Necessary, and Why They Are Rotations

Prerequisite:Limits and Continuity: Reading ε-δ as a Contract on Error

Raw
  • Complex numbers are not “a suspicious symbol −1\sqrt{-1} handed down from above”. Once the plane R2\mathbb{R}^2 is equipped with a suitable product, one obtains, in a single natural way, a field containing the real numbers. Here ii is a concrete element of that field, namely (0,1)(0,1).
  • The meaning of complex multiplication is “multiply the absolute values, add the arguments” — that is, a scaling composed with a rotation. This single fact supports the geometric intuition behind all of complex analysis.
  • If the exponential function is defined by a power series, Euler’s formula eiθ=cos⁡θ+isin⁡θe^{i\theta} = \cos\theta + i\sin\theta can be proved by computation alone. The polar form z=reiθz = re^{i\theta} is a consequence of it.
  • De Moivre’s theorem shows that a nonzero complex number has exactly nn nn-th roots, and that they form the vertices of a regular nn-gon centred at the origin.
  • The field C\mathbb{C} admits no order relation compatible with its arithmetic. Complex numbers are never “larger” or “smaller” than one another; they are always measured by their absolute value.
  • We may identify C\mathbb{C} with the metric space R2\mathbb{R}^2, and there open sets, connectedness and domains are defined. This is the stage on which later chapters place the statement “holomorphic functions are considered on a domain”.

1.1. Imaginary numbers were unavoidable in the search for real roots

Section titled “1.1. Imaginary numbers were unavoidable in the search for real roots”

Square roots of negative numbers were born from the attempt to solve x2+1=0x^2 + 1 = 0 — so one often reads, but history was not that simple. One can perfectly well end the discussion by saying that x2+1=0x^2+1=0 has no real solution. What made it impossible to remain inside the world of the real numbers was the attempt to solve cubic equations that do have real roots.

In sixteenth-century Italy, Cardano published in Ars Magna (1545) a method for solving the cubic x3=px+qx^3 = px + q. In modern notation it reads

x=q2+q24−p3273+q2−q24−p3273.x = \sqrt[3]{\frac{q}{2} + \sqrt{\frac{q^2}{4} - \frac{p^3}{27}}} + \sqrt[3]{\frac{q}{2} - \sqrt{\frac{q^2}{4} - \frac{p^3}{27}}}.

Let us substitute p=15, q=4p = 15,\ q = 4. The equation x3=15x+4x^3 = 15x + 4 has the root x=4x = 4 (indeed 43=64=15⋅4+44^3 = 64 = 15\cdot 4 + 4). But the inner square root of the formula is

q24−p327=4−125=−121,\frac{q^2}{4} - \frac{p^3}{27} = 4 - 125 = -121,

so a square root of a negative number appears. To extract the real root x=4x=4 from the formula, one has no choice but to pass through −121\sqrt{-121}. It is known that this must happen whenever the cubic has three distinct real roots; the phenomenon is called the casus irreducibilis, the irreducible case.

In his Algebra (1572) Bombelli verified that if one manipulates this “quantity that ought not to exist” formally, according to the rules of computation, the imaginary parts cancel along the way and the correct real root emerges. We carry this computation through to the end in Example 2.3. Imaginary numbers were not “introduced because we wanted to solve something”; they appeared as a place one is forced to pass through while solving a problem about real numbers.

1.2. A phenomenon the real world cannot explain

Section titled “1.2. A phenomenon the real world cannot explain”

Algebra is not the only motivation for introducing complex numbers. Consider the following two functions.

f(x)=11−x2,g(x)=11+x2(x∈R)f(x) = \frac{1}{1-x^2}, \qquad g(x) = \frac{1}{1+x^2} \qquad (x \in \mathbb{R})

Both can be expanded around the origin as geometric series.

f(x)=∑n=0∞x2n,g(x)=∑n=0∞(−1)nx2nf(x) = \sum_{n=0}^{\infty} x^{2n}, \qquad g(x) = \sum_{n=0}^{\infty} (-1)^n x^{2n}

Each has radius of convergence 11 and diverges for ∣x∣≥1|x| \ge 1. For ff this is understandable: the denominator vanishes at x=±1x = \pm 1, so the function itself breaks down there. But gg is infinitely differentiable on all of R\mathbb{R} and breaks down nowhere. Why, then, does its power series diverge at ∣x∣=1|x| = 1? Surveying the real line alone, the number 11 carries no special significance.

The answer lies outside the real line. The denominator 1+z21+z^2 of gg vanishes at z=±iz = \pm i, and these two points lie at distance 11 from the origin. The radius of convergence 11 is the distance to the nearest singularity in the complex plane (this fact is proved in a later chapter as radius of convergence and distance to the singularities(Corollary 5.3)[正則関数の強力な性質]). A question about the real numbers that the language of real numbers cannot answer is answered by the complex numbers — and this happens again and again throughout complex analysis. The computation of the definite integral ∫−∞∞dx1+x2=π\int_{-\infty}^{\infty} \frac{dx}{1+x^2} = \pi in an instant by residues (The residue theorem and its applications to definite integrals, improper integrals of rational functions(Proposition 6.2)[留数定理と定積分への応用]) rests on the same pattern.

For power series and radii of convergence themselves see Series and convergence tests, and for the remainder term in Taylor’s theorem see The mean value theorem and Taylor’s theorem.

Defining ii as “the number whose square is −1-1” is circular: whether such a number exists is precisely the question. So we start instead from an object whose existence is already established — ordered pairs of real numbers — and define operations on it.

Definition 2.1(The field of complex numbers)

On the set C:=R2={(a,b)∣a,b∈R}\mathbb{C} := \mathbb{R}^2 = \{(a,b) \mid a, b \in \mathbb{R}\} define two operations by

(a,b)+(c,d):=(a+c, b+d),(a,b)⋅(c,d):=(ac−bd, ad+bc).\begin{aligned} (a,b) + (c,d) &:= (a+c,\ b+d), \\ (a,b) \cdot (c,d) &:= (ac - bd,\ ad + bc). \end{aligned}

Equipped with these operations, C\mathbb{C} is called the field of complex numbers, and its elements complex numbers.

We write 1:=(1,0)1 := (1,0) and i:=(0,1)i := (0,1). For a complex number z=(a,b)z = (a,b) we call aa the real part and bb the imaginary part, written Re⁡z:=a\operatorname{Re} z := a and Im⁡z:=b\operatorname{Im} z := b. A complex number with Im⁡z=0\operatorname{Im} z = 0 is identified with a real number, and a complex number with Re⁡z=0\operatorname{Re} z = 0 and z≠0z \ne 0 is called purely imaginary.

The definition of the product looks abrupt, but it is the unique formula forced by the requirement “write (a,b)(a,b) as a+bia + bi, set i2=−1i^2 = -1, and expand by distributivity”. Indeed

(a+bi)(c+di)=ac+adi+bci+bd i2=(ac−bd)+(ad+bc)i.(a+bi)(c+di) = ac + adi + bci + bd\,i^2 = (ac - bd) + (ad + bc)i.

Thus the product in Definition 2.1 is not written down by anticipating the answer. If one tries to put on the plane a product that extends the arithmetic of the real numbers, preserves distributivity, and admits an element whose square is −1-1, then that product is necessarily given by this formula. Rather than starting from an ii whose existence is in doubt, we adopt as the definition the formula that is forced upon us. That is the intent of Definition 2.1.

Theorem 2.2(Basic properties of the complex field)

For the operations of Definition 2.1 the following hold.

  1. (C,+,⋅)(\mathbb{C}, +, \cdot) is a field. That is, addition and multiplication are commutative and associative, multiplication distributes over addition, there is an additive identity (0,0)(0,0) and a multiplicative identity 1=(1,0)1 = (1,0), and every element other than (0,0)(0,0) has a multiplicative inverse.
  2. The map ι:R→C, a↦(a,0)\iota : \mathbb{R} \to \mathbb{C},\ a \mapsto (a,0) is injective and preserves sums and products: ι(a+b)=ι(a)+ι(b)\iota(a+b) = \iota(a) + \iota(b) and ι(ab)=ι(a)ι(b)\iota(ab) = \iota(a)\iota(b).
  3. i2=−1i^2 = -1; that is, (0,1)⋅(0,1)=(−1,0)(0,1)\cdot(0,1) = (-1,0).
  4. Every z=(a,b)∈Cz = (a,b) \in \mathbb{C} can be written z=ι(a)+ι(b) iz = \iota(a) + \iota(b)\, i, and the numbers a,ba, b in this representation are unique.
Proof(Theorem 2.2)

(1) Addition. Since addition is componentwise, the commutativity and associativity of addition in R\mathbb{R} carry over directly; the identity is (0,0)(0,0) and the inverse of (a,b)(a,b) is (−a,−b)(-a,-b).

(1) Commutativity of multiplication. We have (c,d)⋅(a,b)=(ca−db, cb+da)(c,d)\cdot(a,b) = (ca - db,\ cb + da), and since multiplication in R\mathbb{R} is commutative this equals (ac−bd, ad+bc)=(a,b)⋅(c,d)(ac-bd,\ ad+bc) = (a,b)\cdot(c,d).

(1) Associativity of multiplication. Computing from the left,

((a,b)(c,d))(e,f)=(ac−bd, ad+bc)(e,f)=((ac−bd)e−(ad+bc)f, (ac−bd)f+(ad+bc)e)=(ace−bde−adf−bcf, acf−bdf+ade+bce).\begin{aligned} \bigl((a,b)(c,d)\bigr)(e,f) &= (ac-bd,\ ad+bc)(e,f) \\ &= \bigl((ac-bd)e - (ad+bc)f,\ (ac-bd)f + (ad+bc)e\bigr) \\ &= (ace - bde - adf - bcf,\ acf - bdf + ade + bce). \end{aligned}

Computing from the right,

(a,b)((c,d)(e,f))=(a,b)(ce−df, cf+de)=(a(ce−df)−b(cf+de), a(cf+de)+b(ce−df))=(ace−adf−bcf−bde, acf+ade+bce−bdf).\begin{aligned} (a,b)\bigl((c,d)(e,f)\bigr) &= (a,b)(ce-df,\ cf+de) \\ &= \bigl(a(ce-df) - b(cf+de),\ a(cf+de) + b(ce-df)\bigr) \\ &= (ace - adf - bcf - bde,\ acf + ade + bce - bdf). \end{aligned}

The first components agree and the second components agree, each being a rearrangement of the same terms.

(1) Distributivity.

(a,b)((c,d)+(e,f))=(a,b)(c+e, d+f)=(a(c+e)−b(d+f), a(d+f)+b(c+e))=(ac−bd+ae−bf, ad+bc+af+be)=(ac−bd, ad+bc)+(ae−bf, af+be)=(a,b)(c,d)+(a,b)(e,f).\begin{aligned} (a,b)\bigl((c,d)+(e,f)\bigr) &= (a,b)(c+e,\ d+f) \\ &= \bigl(a(c+e) - b(d+f),\ a(d+f) + b(c+e)\bigr) \\ &= (ac - bd + ae - bf,\ ad + bc + af + be) \\ &= (ac-bd,\ ad+bc) + (ae-bf,\ af+be) \\ &= (a,b)(c,d) + (a,b)(e,f). \end{aligned}

(1) Identity and inverses. Since (a,b)(1,0)=(a⋅1−b⋅0, a⋅0+b⋅1)=(a,b)(a,b)(1,0) = (a\cdot 1 - b\cdot 0,\ a\cdot 0 + b\cdot 1) = (a,b), the element 1=(1,0)1=(1,0) is a multiplicative identity. If (a,b)≠(0,0)(a,b) \ne (0,0) then a2+b2>0a^2+b^2 > 0, and

(a,b)⋅(aa2+b2, −ba2+b2)=(a2+b2a2+b2, −ab+baa2+b2)=(1,0),(a,b) \cdot \left( \frac{a}{a^2+b^2},\ \frac{-b}{a^2+b^2} \right) = \left( \frac{a^2 + b^2}{a^2+b^2},\ \frac{-ab + ba}{a^2+b^2} \right) = (1,0),

so an inverse exists. All the field axioms have now been verified.

(2) The equality ι(a)=ι(b)\iota(a) = \iota(b) means (a,0)=(b,0)(a,0)=(b,0), that is a=ba=b, so ι\iota is injective. For sums, (a,0)+(b,0)=(a+b,0)(a,0)+(b,0) = (a+b,0); for products, (a,0)(b,0)=(ab−0, 0+0)=(ab,0)(a,0)(b,0) = (ab - 0,\ 0 + 0) = (ab, 0). Both are preserved.

(3) Substituting into the definition, (0,1)(0,1)=(0⋅0−1⋅1, 0⋅1+1⋅0)=(−1,0)(0,1)(0,1) = (0\cdot 0 - 1 \cdot 1,\ 0\cdot 1 + 1 \cdot 0) = (-1, 0). Since (−1,0)=ι(−1)(-1,0) = \iota(-1) is −1-1 under the identification, i2=−1i^2 = -1 holds.

(4) We have ι(b) i=(b,0)(0,1)=(b⋅0−0⋅1, b⋅1+0⋅0)=(0,b)\iota(b)\,i = (b,0)(0,1) = (b\cdot 0 - 0 \cdot 1,\ b \cdot 1 + 0 \cdot 0) = (0,b), so ι(a)+ι(b)i=(a,0)+(0,b)=(a,b)\iota(a) + \iota(b)i = (a,0)+(0,b) = (a,b). Uniqueness follows because (a,b)=(a′,b′)(a,b)=(a',b') means a=a′a=a' and b=b′b=b'.

By (2) we may regard R\mathbb{R} as a subfield of C\mathbb{C}, and by (4) we shall from now on write (a,b)(a,b) as a+bia+bi. As a vector space over R\mathbb{R}, the field C\mathbb{C} is two-dimensional with basis {1,i}\{1, i\}.

2.2. Arithmetic, and an answer to the motivating question

Section titled “2.2. Arithmetic, and an answer to the motivating question”

Division is multiplication by the inverse. Using the inverse computed in the proof of Theorem 2.2, for c+di≠0c+di \ne 0 we get

a+bic+di=(a+bi)(c−di)(c+di)(c−di)=(ac+bd)+(bc−ad)ic2+d2.\frac{a+bi}{c+di} = \frac{(a+bi)(c-di)}{(c+di)(c-di)} = \frac{(ac+bd) + (bc-ad)i}{c^2+d^2}.

The operation of “multiplying by the conjugate” to make the denominator real is an application of the identity zzˉ=∣z∣2z\bar z = |z|^2, which we shall see in §3\S 3.

Example 2.3(Bombelli's computation: through the imaginary and back to a real root)

Let us apply Cardano’s formula to the cubic x3=15x+4x^3 = 15x + 4 of §1\S 1. With p=15, q=4p=15,\ q=4,

x=2+−1213+2−−1213=2+11i3+2−11i3.x = \sqrt[3]{2 + \sqrt{-121}} + \sqrt[3]{2 - \sqrt{-121}} = \sqrt[3]{2 + 11i} + \sqrt[3]{2 - 11i}.

Now let us guess a cube root of 2+11i2+11i. Since (2+i)2=4+4i+i2=3+4i(2+i)^2 = 4 + 4i + i^2 = 3 + 4i,

(2+i)3=(2+i)(3+4i)=6+8i+3i+4i2=6+11i−4=2+11i,(2+i)^3 = (2+i)(3+4i) = 6 + 8i + 3i + 4i^2 = 6 + 11i - 4 = 2 + 11i,

so 2+i2+i is one cube root of 2+11i2+11i. Likewise (2−i)2=3−4i(2-i)^2 = 3-4i gives (2−i)3=2−11i(2-i)^3 = 2-11i. Therefore

x=(2+i)+(2−i)=4.x = (2+i) + (2-i) = 4.

The imaginary parts +i+i and −i-i cancel exactly, and the real root x=4x=4 appears. The ii that showed up along the way leaves no trace in the final answer, yet one cannot arrive there without passing through it. This was Bombelli’s discovery.

3. The complex plane, conjugation and absolute value

Section titled “3. The complex plane, conjugation and absolute value”

By Definition 2.1 the set C\mathbb{C} is the plane itself, so a complex number z=a+biz = a+bi may be drawn as the point with coordinates (a,b)(a,b). This plane is called the complex plane or the Gaussian plane, its horizontal axis the real axis and its vertical axis the imaginary axis.

Definition 3.1(Complex conjugate and absolute value)

For z=a+biz = a+bi with a,b∈Ra,b\in\mathbb{R} set

zˉ:=a−bi,∣z∣:=a2+b2.\bar{z} := a - bi, \qquad |z| := \sqrt{a^2+b^2}.

We call zˉ\bar z the complex conjugate of zz, and ∣z∣ (≥0)|z| \ (\ge 0) the absolute value (or modulus) of zz.

Geometrically zˉ\bar z is the reflection of zz in the real axis, and ∣z∣|z| is the Euclidean distance from the origin to zz. When zz is real, ∣z∣|z| agrees with the absolute value of a real number.

z = a + bia − bi (conjugate)Orθabreal axisimaginary axis
The point z = a + bi in the complex plane. Here r is the distance from the origin and θ is the angle measured from the positive real axis. The lower point is the conjugate a − bi, the mirror image of z in the real axis.

Proposition 3.2(Basic laws of conjugation and absolute value)

Let z,w∈Cz, w \in \mathbb{C}.

  1. z+w‾=zˉ+wˉ\overline{z+w} = \bar z + \bar w, zw‾=zˉ wˉ\overline{zw} = \bar z\,\bar w, zˉ‾=z\overline{\bar z} = z.
  2. Re⁡z=z+zˉ2\operatorname{Re} z = \dfrac{z + \bar z}{2}, Im⁡z=z−zˉ2i\operatorname{Im} z = \dfrac{z - \bar z}{2i}. In particular z∈R  ⟺  zˉ=zz \in \mathbb{R} \iff \bar z = z.
  3. zzˉ=∣z∣2z\bar z = |z|^2. In particular z−1=zˉ∣z∣2z^{-1} = \dfrac{\bar z}{|z|^2} when z≠0z \ne 0.
  4. ∣zw∣=∣z∣ ∣w∣|zw| = |z|\,|w|, and ∣zw∣=∣z∣∣w∣\left| \dfrac{z}{w} \right| = \dfrac{|z|}{|w|} when w≠0w \ne 0.
  5. ∣z∣=0  ⟺  z=0|z| = 0 \iff z = 0, and ∣zˉ∣=∣z∣|\bar z| = |z|.
Proof(Proposition 3.2)

Write z=a+biz = a+bi and w=c+diw = c+di with a,b,c,d∈Ra,b,c,d\in\mathbb{R}.

(1) For sums, (a+c)+(b+d)i‾=(a+c)−(b+d)i=(a−bi)+(c−di)\overline{(a+c)+(b+d)i} = (a+c) - (b+d)i = (a-bi)+(c-di). For products, zw=(ac−bd)+(ad+bc)izw = (ac-bd)+(ad+bc)i gives zw‾=(ac−bd)−(ad+bc)i\overline{zw} = (ac-bd) - (ad+bc)i, while on the other hand

zˉ wˉ=(a−bi)(c−di)=(ac−bd)+(a(−d)+(−b)c)i=(ac−bd)−(ad+bc)i,\bar z\,\bar w = (a-bi)(c-di) = (ac - bd) + \bigl(a(-d) + (-b)c\bigr)i = (ac-bd) - (ad+bc)i,

and the two agree. Finally zˉ‾=a−bi‾=a+bi=z\overline{\bar z} = \overline{a-bi} = a+bi = z.

(2) From z+zˉ=(a+bi)+(a−bi)=2az+\bar z = (a+bi)+(a-bi) = 2a we get Re⁡z=(z+zˉ)/2\operatorname{Re} z = (z+\bar z)/2, and from z−zˉ=2biz - \bar z = 2bi we get Im⁡z=b=(z−zˉ)/(2i)\operatorname{Im} z = b = (z-\bar z)/(2i). Hence zˉ=z\bar z = z is equivalent to 2bi=02bi = 0, that is b=0b=0, which is equivalent to z∈Rz \in \mathbb{R}.

(3) zzˉ=(a+bi)(a−bi)=a2−(bi)2=a2+b2=∣z∣2z\bar z = (a+bi)(a-bi) = a^2 - (bi)^2 = a^2 + b^2 = |z|^2, where we used i2=−1i^2=-1 (Theorem 2.2 (3)). If z≠0z \ne 0 then ∣z∣2≠0|z|^2 \ne 0, so dividing both sides by ∣z∣2|z|^2 gives z⋅zˉ/∣z∣2=1z \cdot \bar z /|z|^2 = 1, that is z−1=zˉ/∣z∣2z^{-1} = \bar z/|z|^2.

(4) Using (3) and (1),

∣zw∣2=(zw)(zw)‾=zwzˉwˉ=(zzˉ)(wwˉ)=∣z∣2∣w∣2|zw|^2 = (zw)\overline{(zw)} = z w \bar z \bar w = (z\bar z)(w\bar w) = |z|^2|w|^2

(along the way we used commutativity of multiplication, Theorem 2.2 (1)). Both sides are nonnegative reals, so taking square roots gives ∣zw∣=∣z∣∣w∣|zw| = |z||w|. For quotients, apply the first part to z=(z/w)⋅wz = (z/w)\cdot w to get ∣z∣=∣z/w∣∣w∣|z| = |z/w||w| and divide by ∣w∣≠0|w| \ne 0.

(5) ∣z∣=0|z| = 0 is equivalent to a2+b2=0a^2+b^2 = 0, and since squares of real numbers are nonnegative this is equivalent to a=b=0a=b=0. Also ∣zˉ∣=a2+(−b)2=a2+b2=∣z∣|\bar z| = \sqrt{a^2 + (-b)^2} = \sqrt{a^2+b^2} = |z|.

Example 3.3(The two-squares identity given by multiplicativity of |zw| = |z||w|)

Squaring both sides of Proposition 3.2 (4) and writing things out in components, we obtain for z=a+biz=a+bi and w=c+diw=c+di

(a2+b2)(c2+d2)=(ac−bd)2+(ad+bc)2.(a^2+b^2)(c^2+d^2) = (ac-bd)^2 + (ad+bc)^2.

This is the Brahmagupta–Fibonacci identity, which asserts that a product of two sums of two squares is again a sum of two squares.

Let us check a concrete case. Take z=2+3iz = 2+3i and w=1+4iw = 1+4i, so that ∣z∣2=13|z|^2 = 13 and ∣w∣2=17|w|^2 = 17, and zw=(2⋅1−3⋅4)+(2⋅4+3⋅1)i=−10+11izw = (2\cdot 1 - 3\cdot 4) + (2\cdot 4 + 3 \cdot 1)i = -10 + 11i. Then

13⋅17=221=(−10)2+112=100+121=221,13 \cdot 17 = 221 = (-10)^2 + 11^2 = 100 + 121 = 221,

as it should be. If instead of ww we multiply by wˉ=1−4i\bar w = 1-4i, we get zwˉ=(2+12)+(−8+3)i=14−5iz\bar w = (2+12) + (-8+3)i = 14 - 5i, giving the alternative representation 221=142+52=196+25221 = 14^2+5^2 = 196+25. In number theory this multiplicativity of complex numbers is what one uses to show that the set of numbers representable as a sum of two squares is closed under multiplication.

Theorem 3.4(The triangle inequality)

Let z,w∈Cz, w \in \mathbb{C}.

  1. ∣Re⁡z∣≤∣z∣|\operatorname{Re} z| \le |z| and ∣Im⁡z∣≤∣z∣|\operatorname{Im} z| \le |z|.
  2. ∣z+w∣≤∣z∣+∣w∣|z + w| \le |z| + |w|. Equality holds if and only if z=0z = 0, or there exists a real number t≥0t \ge 0 with w=tzw = tz.
  3. ∣ ∣z∣−∣w∣ ∣≤∣z−w∣\bigl|\,|z| - |w|\,\bigr| \le |z - w| (the reverse triangle inequality).
Proof(Theorem 3.4)

(1) Writing z=a+biz=a+bi, we have ∣a∣=a2≤a2+b2=∣z∣|a| = \sqrt{a^2} \le \sqrt{a^2+b^2} = |z| (using b2≥0b^2 \ge 0 and monotonicity of  ⋅ \sqrt{\ \cdot\ }). The imaginary part is handled in the same way.

(2) Using Proposition 3.2 (3), (1) and (2) in turn,

∣z+w∣2=(z+w)(z+w)‾=(z+w)(zˉ+wˉ)=zzˉ+zwˉ+wzˉ+wwˉ=∣z∣2+(zwˉ+zwˉ‾)+∣w∣2=∣z∣2+2Re⁡(zwˉ)+∣w∣2\begin{aligned} |z+w|^2 &= (z+w)\overline{(z+w)} = (z+w)(\bar z + \bar w) \\ &= z\bar z + z\bar w + w \bar z + w\bar w \\ &= |z|^2 + \bigl(z\bar w + \overline{z \bar w}\bigr) + |w|^2 \\ &= |z|^2 + 2\operatorname{Re}(z\bar w) + |w|^2 \end{aligned}

(here we used wzˉ=wˉz‾=zwˉ‾w\bar z = \overline{\bar w z} = \overline{z\bar w}). Now by (1) together with Proposition 3.2 (4) and (5),

Re⁡(zwˉ)≤∣zwˉ∣=∣z∣∣wˉ∣=∣z∣∣w∣,\operatorname{Re}(z\bar w) \le |z\bar w| = |z||\bar w| = |z||w|,

whence

∣z+w∣2≤∣z∣2+2∣z∣∣w∣+∣w∣2=(∣z∣+∣w∣)2,|z+w|^2 \le |z|^2 + 2|z||w| + |w|^2 = (|z|+|w|)^2,

and taking nonnegative square roots gives ∣z+w∣≤∣z∣+∣w∣|z+w| \le |z|+|w|.

Let us examine equality. Equality in the estimate above holds precisely when Re⁡(zwˉ)=∣zwˉ∣\operatorname{Re}(z\bar w) = |z\bar w|, that is, when ζ:=zwˉ\zeta := z\bar w satisfies Re⁡ζ=∣ζ∣\operatorname{Re}\zeta = |\zeta|. Writing ζ=α+βi\zeta = \alpha + \beta i this reads α=α2+β2\alpha = \sqrt{\alpha^2+\beta^2}; squaring both sides shows that β=0\beta = 0 together with α≥0\alpha \ge 0 is necessary and sufficient. In other words, the condition is that zwˉz\bar w be a nonnegative real number.

If z=0z = 0 this holds automatically. If z≠0z \ne 0 and zwˉ=sz\bar w = s with s≥0s \ge 0 real, then wˉ=s/z\bar w = s/z, and taking conjugates, by Proposition 3.2 (1) and (3),

w=(sz)‾=szˉ=szzˉz=s∣z∣2 z,w = \overline{\left(\frac{s}{z}\right)} = \frac{s}{\bar z} = \frac{s z}{\bar z z} = \frac{s}{|z|^2}\, z,

so setting t:=s/∣z∣2≥0t := s/|z|^2 \ge 0 we get w=tzw = tz. Conversely, if w=tzw = tz with t≥0t\ge 0 then zwˉ=tzzˉ=t∣z∣2≥0z\bar w = t z \bar z = t|z|^2 \ge 0, so equality holds.

(3) Applying (2) to ∣z∣=∣(z−w)+w∣≤∣z−w∣+∣w∣|z| = |(z-w) + w| \le |z-w| + |w| gives ∣z∣−∣w∣≤∣z−w∣|z| - |w| \le |z-w|. Exchanging zz and ww gives ∣w∣−∣z∣≤∣w−z∣=∣z−w∣|w| - |z| \le |w-z| = |z-w| (that ∣−ζ∣=∣ζ∣|-\zeta| = |\zeta| follows from Proposition 3.2 (4) with ∣−1∣=1|-1|=1). Combining the two yields the claim.

The triangle inequality guarantees that d(z,w):=∣z−w∣d(z,w) := |z-w| is a metric on C\mathbb{C}. Indeed d(z,w)=0  ⟺  z=wd(z,w) = 0 \iff z=w (Proposition 3.2 (5)), d(z,w)=d(w,z)d(z,w)=d(w,z), and d(z,w)≤d(z,ζ)+d(ζ,w)d(z,w) \le d(z,\zeta)+d(\zeta,w). This metric is exactly the metric of the Euclidean plane R2\mathbb{R}^2, so arguments about limits and continuity in C\mathbb{C} coincide completely with those in R2\mathbb{R}^2. The framework of ε\varepsilon-δ\delta arguments can be taken over unchanged from Limits and continuity.

4.1. Defining the exponential by a power series

Section titled “4.1. Defining the exponential by a power series”

The key to understanding complex multiplication geometrically is the exponential function. We define it by the same series as in the real case:

exp⁡(z):=∑n=0∞znn!(z∈C).\exp(z) := \sum_{n=0}^{\infty} \frac{z^n}{n!} \qquad (z \in \mathbb{C}).

This series converges absolutely for every zz. Indeed ∑n≥0∣zn/n!∣=∑n≥0∣z∣n/n!\sum_{n\ge 0} |z^n/n!| = \sum_{n \ge 0} |z|^n/n! is a series of nonnegative terms, and it converges by the ratio test (d'Alembert's ratio test(Theorem 6.2)[級数と収束判定]), since ∣z∣n+1/(n+1)!÷∣z∣n/n!=∣z∣/(n+1)→0|z|^{n+1}/(n+1)! \div |z|^n/n! = |z|/(n+1) \to 0. An absolutely convergent series of complex numbers converges (Lemma 7.8[級数と収束判定] (3)), and the product of two absolutely convergent series can be computed by the Cauchy product (Theorem 7.9[級数と収束判定]).

Lemma 4.1(The exponential law)

For all z,w∈Cz, w \in \mathbb{C} we have exp⁡(z+w)=exp⁡(z)exp⁡(w)\exp(z+w) = \exp(z)\exp(w). In particular exp⁡(z)≠0\exp(z) \ne 0 and exp⁡(z)−1=exp⁡(−z)\exp(z)^{-1} = \exp(-z).

Proof(Lemma 4.1)

The series ∑zn/n!\sum z^n/n! and ∑wn/n!\sum w^n/n! both converge absolutely (as checked above with the ratio test, Theorem 6.2[級数と収束判定] (1)). Hence, by the theorem on Cauchy products (Theorem 7.9[級数と収束判定]), their Cauchy product converges to the product exp⁡(z)exp⁡(w)\exp(z)\exp(w). The nn-th term of the Cauchy product is

∑k=0nzkk!⋅wn−k(n−k)!=1n!∑k=0nn!k! (n−k)!zkwn−k=1n!∑k=0n(nk)zkwn−k=(z+w)nn!,\sum_{k=0}^{n} \frac{z^k}{k!}\cdot\frac{w^{n-k}}{(n-k)!} = \frac{1}{n!}\sum_{k=0}^{n} \frac{n!}{k!\,(n-k)!} z^k w^{n-k} = \frac{1}{n!}\sum_{k=0}^{n} \binom{n}{k} z^k w^{n-k} = \frac{(z+w)^n}{n!},

the last equality being the binomial theorem, which holds verbatim because C\mathbb{C} is a commutative ring (Theorem 2.2). Therefore

exp⁡(z)exp⁡(w)=∑n=0∞(z+w)nn!=exp⁡(z+w).\exp(z)\exp(w) = \sum_{n=0}^{\infty} \frac{(z+w)^n}{n!} = \exp(z+w).

Setting w=−zw = -z gives exp⁡(z)exp⁡(−z)=exp⁡(0)=1\exp(z)\exp(-z) = \exp(0) = 1, so exp⁡(z)\exp(z) is nonzero with inverse exp⁡(−z)\exp(-z).

Theorem 4.2(Euler's formula)

For every real number θ\theta,

exp⁡(iθ)=cos⁡θ+isin⁡θ.\exp(i\theta) = \cos\theta + i \sin\theta.

In particular ∣exp⁡(iθ)∣=1|\exp(i\theta)| = 1, and taking θ=π\theta = \pi gives exp⁡(iπ)+1=0\exp(i\pi) + 1 = 0.

Proof(Theorem 4.2)

On Rikai, cos⁡\cos and sin⁡\sin are defined by the series

cos⁡θ=∑m=0∞(−1)mθ2m(2m)!,sin⁡θ=∑m=0∞(−1)mθ2m+1(2m+1)!\cos\theta=\sum_{m=0}^{\infty}\frac{(-1)^m\theta^{2m}}{(2m)!},\qquad\sin\theta=\sum_{m=0}^{\infty}\frac{(-1)^m\theta^{2m+1}}{(2m+1)!}

(Definition 6.1[指数・対数・三角関数をきちんと定義する]); π\pi is defined from them too, and the relation with the unit circle and arc length is derived as a theorem (Elementary functions defined by series). The powers of ii cycle with period 44, i2m=(−1)mi^{2m}=(-1)^m and i2m+1=(−1)mii^{2m+1}=(-1)^mi, so the even-degree partial sums of the series for exp⁡(iθ)\exp(i\theta) are partial sums of cos⁡θ\cos\theta, and the odd-degree ones are partial sums of isin⁡θi\sin\theta. Following this observation carefully to the limit is Lemma 6.3[指数・対数・三角関数をきちんと定義する], which gives exp⁡(iθ)=cos⁡θ+isin⁡θ\exp(i\theta) = \cos\theta + i\sin\theta for every real θ\theta.

As for the absolute value, by Definition 3.1 and cos⁡2θ+sin⁡2θ=1\cos^2\theta+\sin^2\theta=1 (Theorem 6.5[指数・対数・三角関数をきちんと定義する]) we have ∣exp⁡(iθ)∣2=cos⁡2θ+sin⁡2θ=1|\exp(i\theta)|^2 = \cos^2\theta + \sin^2\theta = 1, so ∣exp⁡(iθ)∣=1|\exp(i\theta)| = 1. For θ=π\theta=\pi we have cos⁡π=−1\cos\pi = -1 and sin⁡π=0\sin\pi = 0 (Theorem 7.3[指数・対数・三角関数をきちんと定義する] (2)), so exp⁡(iπ)=−1\exp(i\pi) = -1, that is, exp⁡(iπ)+1=0\exp(i\pi)+1=0.

From now on we write exp⁡(z)\exp(z) as eze^z. From Lemma 4.1 and Theorem 4.2, for real xx and yy,

ex+iy=ex(cos⁡y+isin⁡y),∣ex+iy∣=ex.e^{x+iy} = e^x(\cos y + i \sin y), \qquad |e^{x+iy}| = e^x.

Definition 4.3(Argument and polar form)

Let z≠0z \ne 0 and put ∣z∣=r|z| = r. If a real number θ\theta satisfies z=reiθz = r e^{i\theta}, then θ\theta is called an argument of zz, written θ∈arg⁡z\theta \in \arg z. The representation z=reiθz = re^{i\theta} is called the polar form of zz. The element of arg⁡z\arg z satisfying −π<θ≤π-\pi < \theta \le \pi is called the principal value of the argument and is written Arg⁡z\operatorname{Arg} z.

Let us verify that an argument exists at all, and how many there are.

Remark 4.4

For z≠0z \ne 0 the polar form exists, and the argument is unique up to integer multiples of 2π2\pi.

Existence. Put r=∣z∣>0r=|z| > 0 and u:=z/ru := z/r, so that ∣u∣=1|u| = 1 (Proposition 3.2 (4)) and hence u=a+biu = a+bi satisfies a2+b2=1a^2+b^2=1; in particular a∈[−1,1]a \in [-1,1]. Since cos⁡\cos is continuous and strictly decreasing on [0,π][0,\pi] with cos⁡0=1\cos 0 = 1 and cos⁡π=−1\cos\pi=-1, the intermediate value theorem gives a unique θ0∈[0,π]\theta_0 \in [0,\pi] with cos⁡θ0=a\cos\theta_0 = a (Limits and continuity). Then sin⁡θ0=1−a2=∣b∣\sin\theta_0 = \sqrt{1-a^2} = |b| (because sin⁡≥0\sin \ge 0 on [0,π][0,\pi]). Taking θ:=θ0\theta := \theta_0 if b≥0b \ge 0 and θ:=−θ0\theta := -\theta_0 if b<0b < 0, we get cos⁡θ=a\cos\theta = a and sin⁡θ=b\sin\theta = b, so u=eiθu = e^{i\theta} and therefore z=reiθz = re^{i\theta}.

Uniqueness. If eiα=eiβe^{i\alpha} = e^{i\beta} then Lemma 4.1 gives ei(α−β)=1e^{i(\alpha-\beta)} = 1, that is cos⁡(α−β)=1\cos(\alpha-\beta) = 1 and sin⁡(α−β)=0\sin(\alpha-\beta)=0. Since cos⁡\cos has period 2π2\pi and cos⁡t<1\cos t < 1 on (0,2π)(0,2\pi) (it decreases strictly from 11 to −1-1 on (0,π)(0,\pi) and increases strictly from −1-1 to 11 on (π,2π)(\pi,2\pi)), the equation cos⁡t=1\cos t = 1 forces t∈2πZt \in 2\pi\mathbb{Z}. Hence α−β∈2πZ\alpha - \beta \in 2\pi\mathbb{Z}.

5. De Moivre’s theorem and the n-th roots of unity

Section titled “5. De Moivre’s theorem and the n-th roots of unity”

Theorem 5.1(De Moivre's theorem)

Let z1=r1eiθ1z_1 = r_1 e^{i\theta_1} and z2=r2eiθ2z_2 = r_2 e^{i\theta_2} with r1,r2>0r_1, r_2 > 0 and θ1,θ2∈R\theta_1,\theta_2 \in \mathbb{R}.

  1. z1z2=r1r2 ei(θ1+θ2)z_1 z_2 = r_1 r_2\, e^{i(\theta_1+\theta_2)} and z1z2=r1r2ei(θ1−θ2)\dfrac{z_1}{z_2} = \dfrac{r_1}{r_2} e^{i(\theta_1-\theta_2)}. That is, in a product of complex numbers the absolute values are multiplied and the arguments are added.
  2. For r>0r > 0 and θ∈R\theta \in \mathbb{R}, and for every integer nn, we have (reiθ)n=rneinθ\bigl(re^{i\theta}\bigr)^n = r^n e^{in\theta}.

In particular, taking r=1r = 1 in 2 and rewriting in terms of trigonometric functions, (cos⁡θ+isin⁡θ)n=cos⁡nθ+isin⁡nθ(\cos\theta + i \sin\theta)^n = \cos n\theta + i \sin n\theta for every real θ\theta and every integer nn.

Proof(Theorem 5.1)

(1) By Lemma 4.1 we have eiθ1eiθ2=ei(θ1+θ2)e^{i\theta_1}e^{i\theta_2} = e^{i(\theta_1+\theta_2)}, and since the real factors r1,r2r_1,r_2 commute and can be pulled out, z1z2=r1r2ei(θ1+θ2)z_1z_2 = r_1r_2 e^{i(\theta_1+\theta_2)}. For the quotient, Lemma 4.1 gives (eiθ2)−1=e−iθ2(e^{i\theta_2})^{-1} = e^{-i\theta_2}, so

z1z2=r1eiθ1⋅1r2e−iθ2=r1r2ei(θ1−θ2).\frac{z_1}{z_2} = r_1 e^{i\theta_1}\cdot \frac{1}{r_2}e^{-i\theta_2} = \frac{r_1}{r_2}e^{i(\theta_1-\theta_2)}.

(2) First we treat n≥0n \ge 0 by induction. For n=0n=0 both sides equal 11. Assuming the claim for nn, apply (1) with z1=rneinθz_1 = r^n e^{in\theta} and z2=reiθz_2 = re^{i\theta}:

(reiθ)n+1=(reiθ)n⋅reiθ=rneinθ⋅reiθ=rn+1ei(n+1)θ.(re^{i\theta})^{n+1} = (re^{i\theta})^n \cdot re^{i\theta} = r^n e^{in\theta}\cdot re^{i\theta} = r^{n+1}e^{i(n+1)\theta}.

For n<0n < 0 put m:=−n>0m := -n > 0; then by the case already proved and Lemma 4.1,

(reiθ)n=((reiθ)m)−1=(rmeimθ)−1=r−me−imθ=rneinθ.(re^{i\theta})^{n} = \bigl((re^{i\theta})^{m}\bigr)^{-1} = \bigl(r^m e^{im\theta}\bigr)^{-1} = r^{-m}e^{-im\theta} = r^n e^{in\theta}.

Finally, setting r=1r=1 and applying Theorem 4.2 to both sides gives the trigonometric form.

What (1) says is that the map z↦z2zz \mapsto z_2 z, “multiplication by z2z_2”, is a scaling by the factor r2r_2 about the origin composed with a rotation by θ2\theta_2. Whereas multiplication of real numbers was a stretching of the number line, multiplication of complex numbers is a rotation-and-scaling of the plane. This fact reappears in a later chapter in the form of conformality: the derivative of a holomorphic function behaves locally like a rotation-and-scaling (Holomorphic functions and the Cauchy–Riemann equations, Conformal mappings and the Riemann mapping theorem, local behaviour of angles under holomorphic maps(Theorem 3.2)[等角写像とリーマン写像定理]).

Example 5.2(Computing powers via the polar form)

Let us compute z10z^{10} for z=−1+3 iz = -1 + \sqrt{3}\,i. First, ∣z∣=(−1)2+(3)2=4=2|z| = \sqrt{(-1)^2 + (\sqrt3)^2} = \sqrt{4} = 2. Next, z/2=−12+32iz/2 = -\frac12 + \frac{\sqrt3}{2}i, and cos⁡θ=−12, sin⁡θ=32\cos\theta = -\frac12,\ \sin\theta = \frac{\sqrt3}{2} is satisfied by θ=2π3\theta = \frac{2\pi}{3}, so z=2e2πi/3z = 2e^{2\pi i/3}. By Theorem 5.1 (2),

z10=210e20πi/3=1024 ei(20π/3−6π)=1024 e2πi/3z^{10} = 2^{10} e^{20\pi i/3} = 1024\, e^{i(20\pi/3 - 6\pi)} = 1024\, e^{2\pi i/3}

(we used e−6πi=1e^{-6\pi i} = 1). Therefore

z10=1024(−12+32i)=−512+5123 i.z^{10} = 1024\left(-\frac12 + \frac{\sqrt3}{2}i\right) = -512 + 512\sqrt{3}\, i.

Expanding (−1+3i)10(-1+\sqrt3 i)^{10} by the binomial theorem would mean computing 1111 terms; with the polar form two lines suffice.

Example 5.3(Generating multiple-angle formulas wholesale)

Expanding the left-hand side of Theorem 5.1 (2) by the binomial theorem and comparing real parts expresses cos⁡nθ\cos n\theta as a polynomial in cos⁡θ\cos\theta and sin⁡θ\sin\theta. Let us do this for n=5n=5. Abbreviating c=cos⁡θc=\cos\theta and s=sin⁡θs=\sin\theta,

(c+is)5=c5+5c4(is)+10c3(is)2+10c2(is)3+5c(is)4+(is)5,(c+is)^5 = c^5 + 5c^4(is) + 10c^3(is)^2 + 10c^2(is)^3 + 5c(is)^4 + (is)^5,

and, noting that i2=−1, i3=−i, i4=1, i5=ii^2=-1,\ i^3=-i,\ i^4=1,\ i^5=i, extracting the real part alone gives

cos⁡5θ=c5−10c3s2+5cs4.\cos 5\theta = c^5 - 10c^3s^2 + 5cs^4.

Substituting s2=1−c2s^2 = 1-c^2,

cos⁡5θ=c5−10c3(1−c2)+5c(1−c2)2=c5−10c3+10c5+5c(1−2c2+c4)=c5−10c3+10c5+5c−10c3+5c5=16c5−20c3+5c.\begin{aligned} \cos 5\theta &= c^5 - 10c^3(1-c^2) + 5c(1-c^2)^2 \\ &= c^5 - 10c^3 + 10c^5 + 5c(1 - 2c^2 + c^4) \\ &= c^5 - 10c^3 + 10c^5 + 5c - 10c^3 + 5c^5 \\ &= 16c^5 - 20c^3 + 5c. \end{aligned}

Let us check this. For θ=0\theta = 0 the right-hand side is 16−20+5=1=cos⁡016-20+5 = 1 = \cos 0, and for θ=π\theta=\pi it is −16+20−5=−1=cos⁡π-16+20-5 = -1 = \cos\pi; both agree. This polynomial is nothing other than the fifth Chebyshev polynomial T5T_5.

Theorem 5.4(The n-th roots of a complex number)

Let nn be a positive integer and let w=ρeiφw = \rho e^{i\varphi}, with ρ>0\rho > 0 and φ∈R\varphi\in\mathbb{R}, be a nonzero complex number. Then the equation zn=wz^n = w has exactly nn solutions, given by

zk=ρ1/n exp⁡ ⁣(i φ+2πkn)(k=0,1,…,n−1),z_k = \rho^{1/n}\, \exp\!\left( i\,\frac{\varphi + 2\pi k}{n} \right) \qquad (k = 0, 1, \ldots, n-1),

where ρ1/n\rho^{1/n} denotes the positive nn-th root of the positive real number ρ\rho. These points are equally spaced on the circle of radius ρ1/n\rho^{1/n} centred at the origin, and for n≥3n \ge 3 they form the vertices of a regular nn-gon.

In particular, for w=1w=1 the set of all solutions μn={1,ζ,ζ2,…,ζn−1}\mu_n = \{1, \zeta, \zeta^2, \ldots, \zeta^{n-1}\}, where ζ:=e2πi/n\zeta := e^{2\pi i/n}, is a cyclic group of order nn under multiplication, and for n≥2n \ge 2

1+ζ+ζ2+⋯+ζn−1=0.1 + \zeta + \zeta^2 + \cdots + \zeta^{n-1} = 0.
Proof(Theorem 5.4)

Each zkz_k is a solution. By Theorem 5.1 (2),

zkn=ρ exp⁡ ⁣(i n⋅φ+2πkn)=ρ ei(φ+2πk)=ρ eiφe2πik=w,z_k^n = \rho\,\exp\!\left(i\, n\cdot \frac{\varphi+2\pi k}{n}\right) = \rho\, e^{i(\varphi + 2\pi k)} = \rho\, e^{i\varphi}e^{2\pi i k} = w,

where at the last step we used e2πik=(cos⁡2π+isin⁡2π)k=1e^{2\pi i k} = (\cos 2\pi + i \sin 2\pi)^k = 1 (Theorem 4.2).

They are distinct. Suppose zk=zlz_k = z_l for 0≤k<l≤n−10 \le k < l \le n-1. By the uniqueness part of Remark 4.4,

φ+2πln−φ+2πkn=2π(l−k)n∈2πZ,\frac{\varphi+2\pi l}{n} - \frac{\varphi+2\pi k}{n} = \frac{2\pi(l-k)}{n} \in 2\pi\mathbb{Z},

that is (l−k)/n∈Z(l-k)/n \in \mathbb{Z}, which is impossible since 0<l−k≤n−10 < l-k \le n-1. Hence z0,…,zn−1z_0,\ldots,z_{n-1} are pairwise distinct.

There are no other solutions. If zn=w≠0z^n = w \ne 0 then z≠0z \ne 0, so by Remark 4.4 we may write z=reiθz = re^{i\theta} with r>0r>0. By Theorem 5.1 (2) we get rneinθ=ρeiφr^n e^{in\theta} = \rho e^{i\varphi}, and taking absolute values of both sides (using ∣eit∣=1|e^{it}|=1 from Theorem 4.2) gives rn=ρr^n = \rho. Since t↦tnt \mapsto t^n is strictly increasing on the positive reals, r=ρ1/nr = \rho^{1/n} is determined. From the remaining equation einθ=eiφe^{in\theta} = e^{i\varphi}, the uniqueness part of Remark 4.4 yields an integer kk with nθ−φ=2πkn\theta - \varphi = 2\pi k, so θ=(φ+2πk)/n\theta = (\varphi+2\pi k)/n. Replacing kk by its remainder modulo nn changes θ\theta only by an integer multiple of 2π2\pi and leaves zz unchanged, so z∈{z0,…,zn−1}z \in \{z_0,\ldots,z_{n-1}\}.

Geometric arrangement. The modulus ∣zk∣=ρ1/n|z_k| = \rho^{1/n} does not depend on kk, and the difference of the arguments of consecutive points zk,zk+1z_k, z_{k+1} is constantly 2π/n2\pi/n. Hence the nn points lie equally spaced on one circle and, for n≥3n\ge3, form the vertices of a regular nn-gon.

It is a cyclic group. For w=1w=1 we may take φ=0\varphi=0 and ρ=1\rho=1, giving zk=e2πik/n=ζkz_k = e^{2\pi i k/n} = \zeta^k (Theorem 5.1 (2)). Since ζn=1\zeta^n = 1, the set μn\mu_n is closed under multiplication, and (ζk)−1=ζn−k∈μn(\zeta^k)^{-1} = \zeta^{n-k} \in \mu_n, so it is a group; it is cyclic of order nn with generator ζ\zeta.

The sum is 00. For n≥2n \ge 2 we have ζ≠1\zeta \ne 1 (since 2π/n∉2πZ2\pi/n \notin 2\pi\mathbb{Z}, by Remark 4.4). The formula for the sum of a geometric progression in a field (that C\mathbb{C} is a field is Theorem 2.2) gives

∑k=0n−1ζk=ζn−1ζ−1=1−1ζ−1=0.\sum_{k=0}^{n-1}\zeta^k = \frac{\zeta^n - 1}{\zeta - 1} = \frac{1-1}{\zeta-1} = 0.
1ζζ²ζ³ζ⁴O2π/5
The fifth roots of unity. The powers of ζ = exp(2πi/5) are equally spaced on the unit circle and form the vertices of a regular pentagon. The five points sum to 0.

Example 5.5(Computing cos(2π/5) from the fifth roots of unity)

Let ζ=e2πi/5\zeta = e^{2\pi i/5}. By Theorem 5.4 we have 1+ζ+ζ2+ζ3+ζ4=01+\zeta+\zeta^2+\zeta^3+\zeta^4 = 0. Using Theorem 4.2 together with ζk‾=ζ−k=ζ5−k\overline{\zeta^k} = \zeta^{-k} = \zeta^{5-k},

ζ+ζ4=2cos⁡2π5,ζ2+ζ3=2cos⁡4π5.\zeta + \zeta^4 = 2\cos\frac{2\pi}{5}, \qquad \zeta^2 + \zeta^3 = 2\cos\frac{4\pi}{5}.

Put u:=ζ+ζ4u := \zeta+\zeta^4 and v:=ζ2+ζ3v := \zeta^2+\zeta^3. Their sum is

u+v=(ζ+ζ2+ζ3+ζ4)=−1.u + v = (\zeta+\zeta^2+\zeta^3+\zeta^4) = -1.

Their product, using ζ5=1\zeta^5=1, is

uv=(ζ+ζ4)(ζ2+ζ3)=ζ3+ζ4+ζ6+ζ7=ζ3+ζ4+ζ+ζ2=−1.uv = (\zeta+\zeta^4)(\zeta^2+\zeta^3) = \zeta^3 + \zeta^4 + \zeta^6 + \zeta^7 = \zeta^3+\zeta^4+\zeta+\zeta^2 = -1.

Hence uu and vv are the two roots of t2+t−1=0t^2 + t - 1 = 0, namely t=−1±52t = \dfrac{-1\pm\sqrt5}{2}. Since 2π/5=72∘2\pi/5 = 72^\circ is an angle in the first quadrant, u=2cos⁡(2π/5)>0u = 2\cos(2\pi/5) > 0, and therefore

u=−1+52,cos⁡2π5=5−14.u = \frac{-1+\sqrt5}{2}, \qquad \cos\frac{2\pi}{5} = \frac{\sqrt5 - 1}{4}.

Numerically, (5−1)/4=(2.2360679…−1)/4=0.3090169…(\sqrt5-1)/4 = (2.2360679\ldots-1)/4 = 0.3090169\ldots, which agrees with cos⁡72∘=0.309016…\cos 72^\circ = 0.309016\ldots. That the value can be written using only the square root 5\sqrt5 is the algebraic reason why the regular pentagon is constructible with ruler and compass.

6. Topology of the complex plane: open sets and domains

Section titled “6. Topology of the complex plane: open sets and domains”

As we saw in §3\S 3, the metric on C\mathbb{C} coincides with the Euclidean metric on R2\mathbb{R}^2. In order to say precisely what Ω\Omega means when later chapters speak of “a function holomorphic on Ω\Omega”, we fix here the necessary topological vocabulary.

Definition 6.1(Discs, open sets, closed sets)

For a∈Ca \in \mathbb{C} and r>0r > 0 the set

D(a,r):={z∈C:∣z−a∣<r}D(a,r) := \{ z \in \mathbb{C} : |z - a| < r \}

is called the open disc of radius rr centred at aa. For a set S⊆CS \subseteq \mathbb{C}:

  • A point a∈Sa \in S is an interior point of SS if there exists r>0r>0 with D(a,r)⊆SD(a,r) \subseteq S.
  • SS is open if every point of SS is an interior point of SS.
  • SS is closed if the complement C∖S\mathbb{C}\setminus S is open.
  • SS is bounded if there exists M>0M>0 such that ∣z∣≤M|z| \le M for all z∈Sz \in S.
  • A point a∈Ca \in \mathbb{C} is a boundary point of SS if for every r>0r>0 the disc D(a,r)D(a,r) contains both a point of SS and a point of C∖S\mathbb{C}\setminus S. The set of all boundary points is written ∂S\partial S.

Definition 6.2(Connectedness and domains)

An open set Ω⊆C\Omega \subseteq \mathbb{C} is connected if, whenever Ω=U∪V\Omega = U \cup V with U∩V=∅U \cap V = \varnothing and U,VU, V both open, necessarily U=∅U = \varnothing or V=∅V = \varnothing.

A nonempty connected open set is called a domain.

The definition of connectedness is a negative statement — “cannot be split in two” — and as such is awkward to use directly. For open sets it can be restated concretely as follows.

Proposition 6.3(Connectedness and polygonal connectedness of open sets)

Let Ω⊆C\Omega \subseteq \mathbb{C} be a nonempty open set. The following two conditions are equivalent.

  1. Ω\Omega is connected in the sense of Definition 6.2.
  2. For all p,q∈Ωp, q \in \Omega there exists a polygonal path starting at pp, ending at qq, all of whose segments are contained in Ω\Omega.
Proof(Proposition 6.3)

(2) ⇒\Rightarrow (1). We prove the contrapositive. Suppose Ω=U∪V\Omega = U \cup V with U∩V=∅U\cap V = \varnothing and U,VU,V open and both nonempty. Choose p∈Up \in U and q∈Vq \in V, and let p=p0,p1,…,pm=qp = p_0, p_1, \ldots, p_m = q be the polygonal path given by (2). Since p0∈Up_0 \in U and pm∈Vp_m \in V, there is an index jj with pj∈Up_j \in U and pj+1∈Vp_{j+1}\in V.

Write the segment as γ(t):=pj+t(pj+1−pj)\gamma(t) := p_j + t(p_{j+1}-p_j) for t∈[0,1]t\in[0,1], and set S:={t∈[0,1]:γ(t)∈U}S := \{t \in [0,1] : \gamma(t) \in U\} and t∗:=sup⁡St^* := \sup S. Since 0∈S0 \in S we have S≠∅S \ne \varnothing, and S⊆[0,1]S \subseteq [0,1] is bounded above, so the supremum exists. For c:=γ(t∗)∈Ω=U∪Vc := \gamma(t^*) \in \Omega = U \cup V we rule out two cases.

Case c∈Uc \in U. Since UU is open there is ε>0\varepsilon>0 with D(c,ε)⊆UD(c,\varepsilon)\subseteq U. Because ∣γ(t)−γ(t∗)∣=∣t−t∗∣ ∣pj+1−pj∣|\gamma(t)-\gamma(t^*)| = |t-t^*|\,|p_{j+1}-p_j|, we have γ(t)∈U\gamma(t) \in U whenever ∣t−t∗∣|t - t^*| is small enough. If t∗=1t^* = 1 then c=pj+1∈U∩V=∅c = p_{j+1} \in U \cap V = \varnothing, a contradiction. If t∗<1t^* < 1 then some t∈St \in S exceeds t∗t^*, contradicting that t∗t^* is the supremum.

Case c∈Vc \in V. Similarly take ε>0\varepsilon>0 with D(c,ε)⊆VD(c,\varepsilon)\subseteq V; then there is δ>0\delta>0 such that γ(t)∈V\gamma(t)\in V for all t∈[0,1]t\in[0,1] with ∣t−t∗∣<δ|t-t^*| < \delta, hence γ(t)∉U\gamma(t)\notin U (as U∩V=∅U\cap V=\varnothing). But then S∩(t∗−δ,t∗]=∅S \cap (t^*-\delta, t^*] = \varnothing, so sup⁡S≤t∗−δ<t∗\sup S \le t^* - \delta < t^*, contradicting the definition of t∗t^*. (Note that t∗>0t^*>0 follows from 0∈S0 \in S and the openness of UU: since γ(0)=pj∈U\gamma(0)=p_j\in U, nearby values of tt also lie in SS.)

Both cases are contradictory, so no such splitting U,VU, V exists and Ω\Omega is connected.

(1) ⇒\Rightarrow (2). Fix a∈Ωa \in \Omega and set

U:={z∈Ω:a and z can be joined by a polygonal path inside Ω},V:=Ω∖U.U := \{ z\in\Omega : a \text{ and } z \text{ can be joined by a polygonal path inside } \Omega\}, \qquad V := \Omega\setminus U.

Since a∈Ua \in U (via the path of length 00), we have U≠∅U \ne \varnothing.

UU is open. Given z∈Uz \in U, openness of Ω\Omega provides r>0r>0 with D(z,r)⊆ΩD(z,r)\subseteq\Omega. A disc is convex, so for every w∈D(z,r)w \in D(z,r) the segment [z,w][z,w] lies in D(z,r)⊆ΩD(z,r)\subseteq\Omega. Appending this segment to a polygonal path from aa to zz produces a polygonal path from aa to ww, so w∈Uw \in U. Hence D(z,r)⊆UD(z,r)\subseteq U.

VV is open. Given z∈Vz\in V, take D(z,r)⊆ΩD(z,r)\subseteq\Omega in the same way. If some w∈D(z,r)w\in D(z,r) belonged to UU, then appending the segment [w,z][w,z] to a polygonal path from aa to ww would give z∈Uz \in U, a contradiction. Hence D(z,r)⊆VD(z,r)\subseteq V.

Thus U,VU, V split Ω\Omega into open sets with U∩V=∅U\cap V=\varnothing and U≠∅U\ne\varnothing, so (1) forces V=∅V=\varnothing; that is, every point of Ω\Omega can be joined to aa by a polygonal path. For two points p,q∈Ωp,q\in\Omega, concatenate a polygonal path from pp to aa (traverse the path from aa to pp backwards) with one from aa to qq.

Example 6.4(Deciding openness, closedness and being a domain)

(a) The annulus A={z:1<∣z∣<2}A = \{ z : 1 < |z| < 2 \} is a domain. Let us show it is open. For a∈Aa \in A put r:=min⁡{ ∣a∣−1, 2−∣a∣ }>0r := \min\{\,|a|-1,\ 2-|a|\,\} > 0. If ∣z−a∣<r|z-a| < r then by Theorem 3.4 (3) we have ∣∣z∣−∣a∣∣≤∣z−a∣<r\bigl||z|-|a|\bigr| \le |z-a| < r, hence

∣z∣>∣a∣−r≥∣a∣−(∣a∣−1)=1,∣z∣<∣a∣+r≤∣a∣+(2−∣a∣)=2,|z| > |a| - r \ge |a| - (|a|-1) = 1, \qquad |z| < |a| + r \le |a| + (2-|a|) = 2,

so z∈Az \in A, that is D(a,r)⊆AD(a,r)\subseteq A. Connectedness is checked with Proposition 6.3: any two points of AA can be joined by first moving radially along a segment to a point on the circle ∣z∣=3/2|z| = 3/2, and then following a polygonal path inscribed in that circle (each segment can be taken inside AA).

(b) The closed disc D‾={z:∣z∣≤1}\overline{D} = \{ z : |z| \le 1\} is closed but not open. That the complement {∣z∣>1}\{|z| > 1\} is open follows from the same estimate as in (a). It is not open because 1∈D‾1 \in \overline{D} is not an interior point: for any r>0r > 0, taking z:=1+min⁡{r,1}/2z := 1 + \min\{r,1\}/2 gives ∣z−1∣<r|z - 1| < r and ∣z∣>1|z| > 1, so D(1,r)⊈D‾D(1,r) \not\subseteq \overline D.

(c) The set H={z:Re⁡z≠0}H = \{ z : \operatorname{Re} z \ne 0 \} is open but not a domain. Let us show it is open. For a∈Ha \in H put r:=∣Re⁡a∣>0r := |\operatorname{Re} a| > 0. If ∣z−a∣<r|z-a| < r then by Theorem 3.4 (1)

∣Re⁡z−Re⁡a∣=∣Re⁡(z−a)∣≤∣z−a∣<r=∣Re⁡a∣.|\operatorname{Re} z - \operatorname{Re} a| = |\operatorname{Re}(z-a)| \le |z-a| < r = |\operatorname{Re} a|.

If Re⁡z=0\operatorname{Re} z = 0 the left-hand side would equal ∣Re⁡a∣|\operatorname{Re} a|, contradicting this inequality. Hence Re⁡z≠0\operatorname{Re} z \ne 0, that is D(a,r)⊆HD(a,r)\subseteq H. But H={Re⁡z>0}∪{Re⁡z<0}H = \{\operatorname{Re} z > 0\} \cup \{\operatorname{Re} z < 0\} is a disjoint union of two nonempty open sets, so HH is not connected in the sense of Definition 6.2. Indeed there is no polygonal path inside HH joining −1-1 to 11, since such a path would have to cross the imaginary axis.

(d) The punctured disc D(0,1)∖{0}D(0,1)\setminus\{0\} is a domain. Let us show it is open. For 0<∣a∣<10 < |a| < 1 put r:=min⁡{ ∣a∣, 1−∣a∣ }>0r := \min\{\,|a|,\ 1-|a|\,\} > 0. If ∣z−a∣<r|z-a| < r then, as in (a), Theorem 3.4 (3) gives ∣z∣>∣a∣−r≥0|z| > |a| - r \ge 0 and ∣z∣<∣a∣+r≤1|z| < |a| + r \le 1; in particular ∣z∣>0|z| > 0, that is z≠0z \ne 0. As for connectedness: unless two points are collinear with the origin they can be joined directly by a line segment avoiding the origin, and if they are collinear with it a single slight detour to the side keeps the path clear of the origin. This set is the standard stage on which later chapters consider the Laurent expansion(Theorem 6.1)[正則関数の強力な性質] and residues.

Remark 6.5

Since the metric on C\mathbb{C} coincides with the Euclidean metric on R2\mathbb{R}^2 (§3\S 3), the topological properties of R2\mathbb{R}^2 become properties of C\mathbb{C} verbatim. In particular the following hold.

  • Completeness: every Cauchy sequence (zn)(z_n) of complex numbers converges. This follows because the real and imaginary parts are each Cauchy sequences in R\mathbb{R} (by Theorem 3.4 (1)), together with the completeness of R\mathbb{R}.
  • The Bolzano–Weierstrass theorem: every bounded sequence of complex numbers has a convergent subsequence.
  • The Heine–Borel theorem: a set K⊆CK\subseteq\mathbb{C} is compact (every open cover has a finite subcover) if and only if KK is closed and bounded.

In each case the proof is the standard one for R2\mathbb{R}^2 (split into real and imaginary parts and apply the result for R\mathbb{R}), so we leave it to the textbooks listed in the references.

Exercise 7.1Standard

Show that there is no total order ≤\le on C\mathbb{C} compatible with the field operations — that is, no total order such that x≤yx \le y implies x+z≤y+zx+z \le y+z for every zz, and such that 0≤x0 \le x and 0≤y0\le y imply 0≤xy0 \le xy. Consequently an inequality "z<wz < w" has no meaning unless zz and ww are real.

Solution

Suppose such an order ≤\le existed.

Lemma: if x≠0x \ne 0 then 0<x20 < x^2. Since the order is total, either 0≤x0 \le x or x≤0x \le 0. In the case 0≤x0 \le x, apply the compatibility condition (0≤x, 0≤y⇒0≤xy0\le x,\ 0\le y \Rightarrow 0 \le xy) with y=xy=x to get 0≤x20 \le x^2. In the case x≤0x \le 0, apply the translation condition with z=−xz = -x to get x+(−x)≤0+(−x)x + (-x) \le 0 + (-x), that is 0≤−x0 \le -x, and then the same compatibility condition gives 0≤(−x)(−x)=x20 \le (-x)(-x) = x^2. In either case 0≤x20 \le x^2, and if x≠0x \ne 0 then x2≠0x^2 \ne 0 (a field has no zero divisors, Theorem 2.2), so 0<x20 < x^2.

Applying the lemma with x=1x=1 gives 0<12=10 < 1^2 = 1, and applying it with x=ix=i gives 0<i2=−10 < i^2 = -1 (Theorem 2.2 (3)). Adding 11 to both sides of the latter gives 1<01 < 0, contradicting 0<10 < 1. Hence no such order exists.

Because of this result, the “size” of a complex number is always measured by the absolute value ∣z∣|z|, which is real. Looking back at the places where inequalities occur from §3\S 3 onwards, one finds that both sides of every inequality sign are real numbers.

Exercise 7.2Easy

Show that for all z,w∈Cz, w \in \mathbb{C}

∣z+w∣2+∣z−w∣2=2(∣z∣2+∣w∣2),|z+w|^2 + |z-w|^2 = 2\bigl(|z|^2 + |w|^2\bigr),

and state the geometric meaning of this identity.

Solution

We expand both terms using Proposition 3.2 (3) and (1). As shown in the proof of Theorem 3.4,

∣z+w∣2=∣z∣2+2Re⁡(zwˉ)+∣w∣2,|z+w|^2 = |z|^2 + 2\operatorname{Re}(z\bar w) + |w|^2,

and replacing ww by −w-w, using Re⁡(z(−w)‾)=−Re⁡(zwˉ)\operatorname{Re}(z\overline{(-w)}) = -\operatorname{Re}(z\bar w) and ∣−w∣=∣w∣|-w| = |w|,

∣z−w∣2=∣z∣2−2Re⁡(zwˉ)+∣w∣2.|z-w|^2 = |z|^2 - 2\operatorname{Re}(z\bar w) + |w|^2.

Adding the two identities, the terms in Re⁡(zwˉ)\operatorname{Re}(z\bar w) cancel and we obtain ∣z+w∣2+∣z−w∣2=2∣z∣2+2∣w∣2|z+w|^2+|z-w|^2 = 2|z|^2+2|w|^2.

Geometrically, in the parallelogram with vertices 0, z, z+w, w0,\ z,\ z+w,\ w, the quantities ∣z+w∣|z+w| and ∣z−w∣|z-w| are the lengths of the two diagonals, while ∣z∣|z| and ∣w∣|w| are the lengths of the two pairs of sides. The identity therefore states the parallelogram law: the sum of the squares of the two diagonals of a parallelogram equals the sum of the squares of its four sides. In the theory of normed spaces it is known that this identity holds precisely when the norm is induced by an inner product.

Exercise 7.3Standard

Find all solutions of the equation z4=−4z^4 = -4, and use the result to factor the real polynomial x4+4x^4+4 into a product of two quadratics with real coefficients.

Solution

Since −4=4eiπ-4 = 4e^{i\pi}, applying Theorem 5.4 with n=4, ρ=4, φ=πn=4,\ \rho=4,\ \varphi=\pi gives solutions with modulus 41/4=24^{1/4} = \sqrt2:

zk=2 exp⁡ ⁣(i π+2πk4)(k=0,1,2,3).z_k = \sqrt{2}\,\exp\!\left(i\,\frac{\pi + 2\pi k}{4}\right)\qquad (k=0,1,2,3).

Writing these out with Theorem 4.2, and using cos⁡(π/4)=sin⁡(π/4)=22\cos(\pi/4)=\sin(\pi/4)=\frac{\sqrt2}{2},

z0=2(22+22i)=1+i,z1=−1+i,z2=−1−i,z3=1−iz_0 = \sqrt2\left(\tfrac{\sqrt2}{2}+\tfrac{\sqrt2}{2}i\right) = 1+i,\quad z_1 = -1+i,\quad z_2 = -1-i,\quad z_3 = 1-i

(each of z1,z2,z3z_1,z_2,z_3 is z0z_0 rotated successively by π/2\pi/2, Theorem 5.1 (1)). As a check, (1+i)2=2i(1+i)^2 = 2i, so (1+i)4=(2i)2=−4(1+i)^4 = (2i)^2 = -4; it is indeed a solution.

Now the factorization. The complex roots of x4+4x^4+4 are the four numbers above, and pairing conjugate roots produces quadratics with real coefficients.

(x−(1+i))(x−(1−i))=(x−1)2−i2=x2−2x+2\bigl(x-(1+i)\bigr)\bigl(x-(1-i)\bigr) = (x-1)^2 - i^2 = x^2-2x+2(x−(−1+i))(x−(−1−i))=(x+1)2−i2=x2+2x+2\bigl(x-(-1+i)\bigr)\bigl(x-(-1-i)\bigr) = (x+1)^2 - i^2 = x^2+2x+2

Hence x4+4=(x2−2x+2)(x2+2x+2)x^4+4 = (x^2-2x+2)(x^2+2x+2). As a check,

(x2+2−2x)(x2+2+2x)=(x2+2)2−(2x)2=x4+4x2+4−4x2=x4+4,(x^2+2-2x)(x^2+2+2x) = (x^2+2)^2 - (2x)^2 = x^4+4x^2+4-4x^2 = x^4+4,

which agrees. (This is the case b=1b=1 of Sophie Germain’s identity a4+4b4=(a2−2ab+2b2)(a2+2ab+2b2)a^4+4b^4 = (a^2-2ab+2b^2)(a^2+2ab+2b^2).)

Exercise 7.4Hard

Let θ\theta be a real number that is not an integer multiple of 2π2\pi, and let nn be a positive integer. Express ∑k=0n−1eikθ\sum_{k=0}^{n-1} e^{ik\theta} in closed form using the sum of a geometric progression, and deduce from it

∑k=0n−1cos⁡kθ,∑k=0n−1sin⁡kθ.\sum_{k=0}^{n-1}\cos k\theta, \qquad \sum_{k=0}^{n-1}\sin k\theta.
Solution

By hypothesis eiθ≠1e^{i\theta}\ne 1 (uniqueness in Remark 4.4). Since C\mathbb{C} is a field (Theorem 2.2) we may use the formula for the sum of a geometric progression, and (eiθ)k=eikθ(e^{i\theta})^k = e^{ik\theta} by Theorem 5.1 (2), so

S:=∑k=0n−1eikθ=einθ−1eiθ−1.S := \sum_{k=0}^{n-1} e^{ik\theta} = \frac{e^{in\theta}-1}{e^{i\theta}-1}.

The standard move is to factor out half-angles from numerator and denominator. By Lemma 4.1 and Theorem 4.2,

eiα−1=eiα/2(eiα/2−e−iα/2)=eiα/2⋅2isin⁡α2e^{i\alpha}-1 = e^{i\alpha/2}\bigl(e^{i\alpha/2}-e^{-i\alpha/2}\bigr) = e^{i\alpha/2}\cdot 2i\sin\frac{\alpha}{2}

(we used eiβ−e−iβ=(cos⁡β+isin⁡β)−(cos⁡β−isin⁡β)=2isin⁡βe^{i\beta}-e^{-i\beta} = (\cos\beta+i\sin\beta)-(\cos\beta-i\sin\beta) = 2i\sin\beta). Applying this with α=nθ\alpha = n\theta in the numerator and α=θ\alpha=\theta in the denominator, and noting sin⁡(θ/2)≠0\sin(\theta/2)\ne0 (since θ∉2πZ\theta\notin2\pi\mathbb{Z}),

S=einθ/2⋅2isin⁡(nθ/2)eiθ/2⋅2isin⁡(θ/2)=ei(n−1)θ/2 sin⁡(nθ/2)sin⁡(θ/2).S = \frac{e^{in\theta/2}\cdot 2i\sin(n\theta/2)}{e^{i\theta/2}\cdot 2i \sin(\theta/2)} = e^{i(n-1)\theta/2}\,\frac{\sin(n\theta/2)}{\sin(\theta/2)}.

Since sin⁡(nθ/2)/sin⁡(θ/2)\sin(n\theta/2)/\sin(\theta/2) is real, reading off real and imaginary parts with Theorem 4.2 gives

∑k=0n−1cos⁡kθ=cos⁡(n−1)θ2⋅sin⁡(nθ/2)sin⁡(θ/2),∑k=0n−1sin⁡kθ=sin⁡(n−1)θ2⋅sin⁡(nθ/2)sin⁡(θ/2).\sum_{k=0}^{n-1}\cos k\theta = \cos\frac{(n-1)\theta}{2}\cdot\frac{\sin(n\theta/2)}{\sin(\theta/2)}, \qquad \sum_{k=0}^{n-1}\sin k\theta = \sin\frac{(n-1)\theta}{2}\cdot\frac{\sin(n\theta/2)}{\sin(\theta/2)}.

Let us check this. For n=2n=2 the first right-hand side is

cos⁡θ2⋅sin⁡θsin⁡(θ/2)=cos⁡θ2⋅2sin⁡(θ/2)cos⁡(θ/2)sin⁡(θ/2)=2cos⁡2θ2=1+cos⁡θ,\cos\frac{\theta}{2}\cdot\frac{\sin\theta}{\sin(\theta/2)} = \cos\frac\theta2\cdot\frac{2\sin(\theta/2)\cos(\theta/2)}{\sin(\theta/2)} = 2\cos^2\frac\theta2 = 1+\cos\theta,

which agrees with the left-hand side cos⁡0+cos⁡θ=1+cos⁡θ\cos 0 + \cos\theta = 1 + \cos\theta. Handling sums of trigonometric functions directly is laborious, but collecting them into complex exponentials reduces everything to a single geometric sum. The kernel sin⁡(nθ/2)/sin⁡(θ/2)\sin(n\theta/2)/\sin(\theta/2) obtained here is the main part of the Dirichlet kernel of Fourier series.

  • L. V. Ahlfors, Complex Analysis, 3rd ed., McGraw-Hill, 1979 — Chapter 1 (the algebra and geometry of complex numbers, the topology of the complex plane). The standard English textbook.
  • E. M. Stein and R. Shakarchi, Complex Analysis (Princeton Lectures in Analysis II), Princeton University Press, 2003 — Chapter 1. A concise account of the topology of the complex plane and an introduction to holomorphic functions.
  • R. Remmert, Theory of Complex Functions, Graduate Texts in Mathematics 122, Springer, 1991 — a reference with a detailed account of the historical background of complex numbers (Cardano, Bombelli, Gauss, Hamilton).
  • Takagi Teiji, Kaiseki Gairon (A Course of Analysis), revised 3rd ed., Iwanami Shoten, 1983 (in Japanese) — complex numbers and elementary functions treated by power series.
  • Jimbo Michio, Fukuso Kansū Nyūmon (Introduction to Complex Functions), Iwanami Shoten, 2003 (in Japanese) — an introductory text in Japanese, giving a unified account from the complex plane and the polar form through to residue calculus.

Appendix: Is there anything beyond the complex numbers?

Section titled “Appendix: Is there anything beyond the complex numbers?”

Why the road stops at C\mathbb{C}. Having extended the reals to the complex numbers, it is natural to ask whether one can extend further. Hamilton in fact worked on that problem for more than ten years and in 1843 discovered the four-dimensional quaternions H\mathbb{H} — at the cost of abandoning commutativity of multiplication (ij=−jiij = -ji). For the eight-dimensional octonions, associativity is lost as well.

This is no accident. By Frobenius’s theorem (1878), the only finite-dimensional associative division algebras over R\mathbb{R} are R\mathbb{R}, C\mathbb{C} and H\mathbb{H}, and among these only R\mathbb{R} and C\mathbb{C} are commutative. In other words, as long as one demands a commutative field containing R\mathbb{R} and finite-dimensional over R\mathbb{R}, nothing strictly larger than C\mathbb{C} exists. The complex numbers are special precisely because they are a dead end.

The fundamental theorem of algebra. The motive for introducing C\mathbb{C} was “to solve x2+1=0x^2+1=0”, but what we obtained was far more. The fundamental theorem of algebra (Gauss, in his 1799 dissertation and elsewhere) asserts that every polynomial of degree at least 11 with complex coefficients has a root in C\mathbb{C}. Adjoining the single element ii makes every algebraic equation solvable. One of the shortest proofs of this theorem uses Liouville's theorem(Theorem 4.2)[正則関数の強力な性質] (a bounded entire function is constant), and is available once the machinery of complex analysis is in place (Cauchy’s integral theorem and integral formula, Powerful properties of holomorphic functions).

A bridge to the next chapter. The stage is set. In the next chapter we consider, for a function f:Ω→Cf : \Omega \to \mathbb{C} defined on a domain Ω\Omega of the complex plane, the derivative

f′(z0)=lim⁡h→0f(z0+h)−f(z0)h(h∈C).f'(z_0) = \lim_{h\to 0}\frac{f(z_0+h)-f(z_0)}{h} \qquad (h \in \mathbb{C}).

The form is the same as for real functions, but the decisive difference is that hh may approach 00 from every direction in the complex plane. The consequence is the Cauchy–Riemann equations(Theorem 4.1)[Holomorphic Functions and the Cauchy-Riemann Equations], and from there begins a phenomenon impossible in real analysis: once differentiable, differentiable infinitely often (Holomorphic functions and the Cauchy–Riemann equations).

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