Complex numbers are not “a suspicious symbol −1 handed down from above”. Once the plane R2 is equipped with a suitable product, one obtains, in a single natural way, a field containing the real numbers. Here i is a concrete element of that field, namely (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=cosθ+isinθ can be proved by computation alone. The polar form z=reiθ is a consequence of it.
De Moivre’s theorem shows that a nonzero complex number has exactly nn-th roots, and that they form the vertices of a regular n-gon centred at the origin.
The field 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 with the metric space R2, 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”.
Square roots of negative numbers were born from the attempt to solve x2+1=0 — so one often reads, but history was not that simple. One can perfectly well end the discussion by saying that x2+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+q. In modern notation it reads
x=32q+4q2−27p3+32q−4q2−27p3.
Let us substitute p=15,q=4. The equation x3=15x+4 has the root x=4 (indeed 43=64=15⋅4+4). But the inner square root of the formula is
4q2−27p3=4−125=−121,
so a square root of a negative number appears. To extract the real root x=4 from the formula, one has no choice but to pass through −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.
Algebra is not the only motivation for introducing complex numbers. Consider the following two functions.
f(x)=1−x21,g(x)=1+x21(x∈R)
Both can be expanded around the origin as geometric series.
f(x)=n=0∑∞x2n,g(x)=n=0∑∞(−1)nx2n
Each has radius of convergence 1 and diverges for ∣x∣≥1. For f this is understandable: the denominator vanishes at x=±1, so the function itself breaks down there. But g is infinitely differentiable on all of R and breaks down nowhere. Why, then, does its power series diverge at ∣x∣=1? Surveying the real line alone, the number 1 carries no special significance.
Defining i as “the number whose square is −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.
Equipped with these operations, C is called the field of complex numbers, and its elements complex numbers.
We write 1:=(1,0) and i:=(0,1). For a complex number z=(a,b) we call a the real part and b the imaginary part, written Rez:=a and Imz:=b. A complex number with Imz=0 is identified with a real number, and a complex number with Rez=0 and z=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) as a+bi, set i2=−1, and expand by distributivity”. Indeed
(a+bi)(c+di)=ac+adi+bci+bdi2=(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, then that product is necessarily given by this formula. Rather than starting from an i 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.
(C,+,⋅) is a field. That is, addition and multiplication are commutative and associative, multiplication distributes over addition, there is an additive identity (0,0) and a multiplicative identity 1=(1,0), and every element other than (0,0) has a multiplicative inverse.
The map ι:R→C,a↦(a,0) is injective and preserves sums and products: ι(a+b)=ι(a)+ι(b) and ι(ab)=ι(a)ι(b).
i2=−1; that is, (0,1)⋅(0,1)=(−1,0).
Every z=(a,b)∈C can be written z=ι(a)+ι(b)i, and the numbers a,b in this representation are unique.
Proof(Theorem 2.2)
(1) Addition. Since addition is componentwise, the commutativity and associativity of addition in R carry over directly; the identity is (0,0) and the inverse of (a,b) is (−a,−b).
(1) Commutativity of multiplication. We have (c,d)⋅(a,b)=(ca−db,cb+da), and since multiplication in R is commutative this equals (ac−bd,ad+bc)=(a,b)⋅(c,d).
(1) Associativity of multiplication. Computing from the left,
(1) Identity and inverses. Since (a,b)(1,0)=(a⋅1−b⋅0,a⋅0+b⋅1)=(a,b), the element 1=(1,0) is a multiplicative identity. If (a,b)=(0,0) then a2+b2>0, and
so an inverse exists. All the field axioms have now been verified.
(2) The equality ι(a)=ι(b) means (a,0)=(b,0), that is a=b, so ι is injective. For sums, (a,0)+(b,0)=(a+b,0); for products, (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). Since (−1,0)=ι(−1) is −1 under the identification, i2=−1 holds.
(4) We have ι(b)i=(b,0)(0,1)=(b⋅0−0⋅1,b⋅1+0⋅0)=(0,b), so ι(a)+ι(b)i=(a,0)+(0,b)=(a,b). Uniqueness follows because (a,b)=(a′,b′) means a=a′ and b=b′.
∎
By (2) we may regard R as a subfield of C, and by (4) we shall from now on write (a,b) as a+bi. As a vector space over R, the field C is two-dimensional with basis {1,i}.
2.2. Arithmetic, and an answer to the motivating question
The operation of “multiplying by the conjugate” to make the denominator real is an application of the identity zzˉ=∣z∣2, which we shall see in §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+4 of §1. With p=15,q=4,
x=32+−121+32−−121=32+11i+32−11i.
Now let us guess a cube root of 2+11i. Since (2+i)2=4+4i+i2=3+4i,
(2+i)3=(2+i)(3+4i)=6+8i+3i+4i2=6+11i−4=2+11i,
so 2+i is one cube root of 2+11i. Likewise (2−i)2=3−4i gives (2−i)3=2−11i. Therefore
x=(2+i)+(2−i)=4.
The imaginary parts +i and −i cancel exactly, and the real root x=4 appears. The i 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
By Definition 2.1 the set C is the plane itself, so a complex number z=a+bi may be drawn as the point with coordinates (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.
We call zˉ the complex conjugate of z, and ∣z∣(≥0) the absolute value (or modulus) of z.
Geometrically zˉ is the reflection of z in the real axis, and ∣z∣ is the Euclidean distance from the origin to z. When z is real, ∣z∣ agrees with the absolute value of a real number.
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∈C.
z+w=zˉ+wˉ, zw=zˉwˉ, zˉ=z.
Rez=2z+zˉ, Imz=2iz−zˉ. In particular z∈R⟺zˉ=z.
zzˉ=∣z∣2. In particular z−1=∣z∣2zˉ when z=0.
∣zw∣=∣z∣∣w∣, and wz=∣w∣∣z∣ when w=0.
∣z∣=0⟺z=0, and ∣zˉ∣=∣z∣.
Proof(Proposition 3.2)
Write z=a+bi and w=c+di with a,b,c,d∈R.
(1) For sums, (a+c)+(b+d)i=(a+c)−(b+d)i=(a−bi)+(c−di). For products, zw=(ac−bd)+(ad+bc)i gives zw=(ac−bd)−(ad+bc)i, while on the other hand
(2) From z+zˉ=(a+bi)+(a−bi)=2a we get Rez=(z+zˉ)/2, and from z−zˉ=2bi we get Imz=b=(z−zˉ)/(2i). Hence zˉ=z is equivalent to 2bi=0, that is b=0, which is equivalent to z∈R.
(3)zzˉ=(a+bi)(a−bi)=a2−(bi)2=a2+b2=∣z∣2, where we used i2=−1 (Theorem 2.2 (3)). If z=0 then ∣z∣2=0, so dividing both sides by ∣z∣2 gives z⋅zˉ/∣z∣2=1, that is z−1=zˉ/∣z∣2.
(4) Using (3) and (1),
∣zw∣2=(zw)(zw)=zwzˉwˉ=(zzˉ)(wwˉ)=∣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∣. For quotients, apply the first part to z=(z/w)⋅w to get ∣z∣=∣z/w∣∣w∣ and divide by ∣w∣=0.
(5)∣z∣=0 is equivalent to a2+b2=0, and since squares of real numbers are nonnegative this is equivalent to a=b=0. Also ∣zˉ∣=a2+(−b)2=a2+b2=∣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+bi and w=c+di
(a2+b2)(c2+d2)=(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+3i and w=1+4i, so that ∣z∣2=13 and ∣w∣2=17, and zw=(2⋅1−3⋅4)+(2⋅4+3⋅1)i=−10+11i. Then
13⋅17=221=(−10)2+112=100+121=221,
as it should be. If instead of w we multiply by wˉ=1−4i, we get zwˉ=(2+12)+(−8+3)i=14−5i, giving the alternative representation 221=142+52=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.
(here we used wzˉ=wˉz=zwˉ). Now by (1) together with Proposition 3.2 (4) and (5),
Re(zwˉ)≤∣zwˉ∣=∣z∣∣wˉ∣=∣z∣∣w∣,
whence
∣z+w∣2≤∣z∣2+2∣z∣∣w∣+∣w∣2=(∣z∣+∣w∣)2,
and taking nonnegative square roots gives ∣z+w∣≤∣z∣+∣w∣.
Let us examine equality. Equality in the estimate above holds precisely when Re(zwˉ)=∣zwˉ∣, that is, when ζ:=zwˉ satisfies Reζ=∣ζ∣. Writing ζ=α+βi this reads α=α2+β2; squaring both sides shows that β=0 together with α≥0 is necessary and sufficient. In other words, the condition is that zwˉ be a nonnegative real number.
If z=0 this holds automatically. If z=0 and zwˉ=s with s≥0 real, then wˉ=s/z, and taking conjugates, by Proposition 3.2 (1) and (3),
w=(zs)=zˉs=zˉzsz=∣z∣2sz,
so setting t:=s/∣z∣2≥0 we get w=tz. Conversely, if w=tz with t≥0 then zwˉ=tzzˉ=t∣z∣2≥0, so equality holds.
(3) Applying (2) to ∣z∣=∣(z−w)+w∣≤∣z−w∣+∣w∣ gives ∣z∣−∣w∣≤∣z−w∣. Exchanging z and w gives ∣w∣−∣z∣≤∣w−z∣=∣z−w∣ (that ∣−ζ∣=∣ζ∣ follows from Proposition 3.2 (4) with ∣−1∣=1). Combining the two yields the claim.
∎
The triangle inequality guarantees that d(z,w):=∣z−w∣ is a metric on C. Indeed d(z,w)=0⟺z=w (Proposition 3.2 (5)), d(z,w)=d(w,z), and d(z,w)≤d(z,ζ)+d(ζ,w). This metric is exactly the metric of the Euclidean plane R2, so arguments about limits and continuity in C coincide completely with those in R2. The framework of ε-δ arguments can be taken over unchanged from Limits and continuity.
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∑∞n!zn(z∈C).
This series converges absolutely for every z. Indeed ∑n≥0∣zn/n!∣=∑n≥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. An absolutely convergent series has a sum unchanged by rearrangement, and two absolutely convergent series may be multiplied by the Cauchy product (Series and convergence tests). We use both facts below.
The two series on the right are precisely the Maclaurin expansions of cosθ and sinθ for real θ (this follows from the estimate ∣θ∣N+1/(N+1)!→0 for the remainder term in Taylor’s theorem; see The mean value theorem and Taylor’s theorem). Hence exp(iθ)=cosθ+isinθ.
As for the absolute value, by Definition 3.1 we have ∣exp(iθ)∣2=cos2θ+sin2θ=1, so ∣exp(iθ)∣=1. For θ=π we have cosπ=−1 and sinπ=0, so exp(iπ)=−1.
∎
From now on we write exp(z) as ez. From Lemma 4.1 and Theorem 4.2, for real x and y,
Let z=0 and put ∣z∣=r. If a real number θ satisfies z=reiθ, then θ is called an argument of z, written θ∈argz. The representation z=reiθ is called the polar form of z. The element of argz satisfying −π<θ≤π is called the principal value of the argument and is written Argz.
Let us verify that an argument exists at all, and how many there are.
For z=0 the polar form exists, and the argument is unique up to integer multiples of 2π.
Existence. Put r=∣z∣>0 and u:=z/r, so that ∣u∣=1 (Proposition 3.2 (4)) and hence u=a+bi satisfies a2+b2=1; in particular a∈[−1,1]. Since cos is continuous and strictly decreasing on [0,π] with cos0=1 and cosπ=−1, the intermediate value theorem gives a unique θ0∈[0,π] with cosθ0=a (Limits and continuity). Then sinθ0=1−a2=∣b∣ (because sin≥0 on [0,π]). Taking θ:=θ0 if b≥0 and θ:=−θ0 if b<0, we get cosθ=a and sinθ=b, so u=eiθ and therefore z=reiθ.
Uniqueness. If eiα=eiβ then Lemma 4.1 gives ei(α−β)=1, that is cos(α−β)=1 and sin(α−β)=0. Since cos has period 2π and cost<1 on (0,2π) (it decreases strictly from 1 to −1 on (0,π) and increases strictly from −1 to 1 on (π,2π)), the equation cost=1 forces t∈2πZ. Hence α−β∈2πZ.
5. De Moivre’s theorem and the n-th roots of unity
Let z1=r1eiθ1 and z2=r2eiθ2 with r1,r2>0 and θ1,θ2∈R.
z1z2=r1r2ei(θ1+θ2) and z2z1=r2r1ei(θ1−θ2). That is, in a product of complex numbers the absolute values are multiplied and the arguments are added.
For r>0 and θ∈R, and for every integer n, we have (reiθ)n=rneinθ.
In particular, taking r=1 in 2 and rewriting in terms of trigonometric functions, (cosθ+isinθ)n=cosnθ+isinnθ for every real θ and every integer n.
Proof(Theorem 5.1)
(1) By Lemma 4.1 we have eiθ1eiθ2=ei(θ1+θ2), and since the real factors r1,r2 commute and can be pulled out, z1z2=r1r2ei(θ1+θ2). For the quotient, Lemma 4.1 gives (eiθ2)−1=e−iθ2, so
z2z1=r1eiθ1⋅r21e−iθ2=r2r1ei(θ1−θ2).
(2) First we treat n≥0 by induction. For n=0 both sides equal 1. Assuming the claim for n, apply (1) with z1=rneinθ and z2=reiθ:
(reiθ)n+1=(reiθ)n⋅reiθ=rneinθ⋅reiθ=rn+1ei(n+1)θ.
For n<0 put m:=−n>0; then by the case already proved and Lemma 4.1,
(reiθ)n=((reiθ)m)−1=(rmeimθ)−1=r−me−imθ=rneinθ.
Finally, setting r=1 and applying Theorem 4.2 to both sides gives the trigonometric form.
Let us compute z10 for z=−1+3i. First, ∣z∣=(−1)2+(3)2=4=2. Next, z/2=−21+23i, and cosθ=−21,sinθ=23 is satisfied by θ=32π, so z=2e2πi/3. By Theorem 5.1 (2),
z10=210e20πi/3=1024ei(20π/3−6π)=1024e2πi/3
(we used e−6πi=1). Therefore
z10=1024(−21+23i)=−512+5123i.
Expanding (−1+3i)10 by the binomial theorem would mean computing 11 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 cosnθ as a polynomial in cosθ and sinθ. Let us do this for n=5. Abbreviating c=cosθ and s=sinθ,
Let us check this. For θ=0 the right-hand side is 16−20+5=1=cos0, and for θ=π it is −16+20−5=−1=cosπ; both agree. This polynomial is nothing other than the fifth Chebyshev polynomial T5.
Let n be a positive integer and let w=ρeiφ, with ρ>0 and φ∈R, be a nonzero complex number. Then the equation zn=w has exactly n solutions, given by
zk=ρ1/nexp(inφ+2πk)(k=0,1,…,n−1),
where ρ1/n denotes the positive n-th root of the positive real number ρ. These points are equally spaced on the circle of radius ρ1/n centred at the origin, and for n≥3 they form the vertices of a regular n-gon.
In particular, for w=1 the set of all solutions μn={1,ζ,ζ2,…,ζn−1}, where ζ:=e2πi/n, is a cyclic group of order n under multiplication, and for n≥2
where at the last step we used e2πik=(cos2π+isin2π)k=1 (Theorem 4.2).
They are distinct. Suppose zk=zl for 0≤k<l≤n−1. By the uniqueness part of Remark 4.4,
nφ+2πl−nφ+2πk=n2π(l−k)∈2πZ,
that is (l−k)/n∈Z, which is impossible since 0<l−k≤n−1. Hence z0,…,zn−1 are pairwise distinct.
There are no other solutions. If zn=w=0 then z=0, so by Remark 4.4 we may write z=reiθ with r>0. By Theorem 5.1 (2) we get rneinθ=ρeiφ, and taking absolute values of both sides (using ∣eit∣=1 from Theorem 4.2) gives rn=ρ. Since t↦tn is strictly increasing on the positive reals, r=ρ1/n is determined. From the remaining equation einθ=eiφ, the uniqueness part of Remark 4.4 yields an integer k with nθ−φ=2πk, so θ=(φ+2πk)/n. Replacing k by its remainder modulo n changes θ only by an integer multiple of 2π and leaves z unchanged, so z∈{z0,…,zn−1}.
Geometric arrangement. The modulus ∣zk∣=ρ1/n does not depend on k, and the difference of the arguments of consecutive points zk,zk+1 is constantly 2π/n. Hence the n points lie equally spaced on one circle and, for n≥3, form the vertices of a regular n-gon.
It is a cyclic group. For w=1 we may take φ=0 and ρ=1, giving zk=e2πik/n=ζk (Theorem 5.1 (2)). Since ζn=1, the set μn is closed under multiplication, and (ζk)−1=ζn−k∈μn, so it is a group; it is cyclic of order n with generator ζ.
The sum is 0. For n≥2 we have ζ=1 (since 2π/n∈/2πZ, by Remark 4.4). The formula for the sum of a geometric progression in a field (that C is a field is Theorem 2.2) gives
k=0∑n−1ζk=ζ−1ζn−1=ζ−11−1=0.∎
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. By Theorem 5.4 we have 1+ζ+ζ2+ζ3+ζ4=0. Using Theorem 4.2 together with ζk=ζ−k=ζ5−k,
ζ+ζ4=2cos52π,ζ2+ζ3=2cos54π.
Put u:=ζ+ζ4 and v:=ζ2+ζ3. Their sum is
u+v=(ζ+ζ2+ζ3+ζ4)=−1.
Their product, using ζ5=1, is
uv=(ζ+ζ4)(ζ2+ζ3)=ζ3+ζ4+ζ6+ζ7=ζ3+ζ4+ζ+ζ2=−1.
Hence u and v are the two roots of t2+t−1=0, namely t=2−1±5. Since 2π/5=72∘ is an angle in the first quadrant, u=2cos(2π/5)>0, and therefore
u=2−1+5,cos52π=45−1.
Numerically, (5−1)/4=(2.2360679…−1)/4=0.3090169…, which agrees with cos72∘=0.309016…. That the value can be written using only the square root 5 is the algebraic reason why the regular pentagon is constructible with ruler and compass.
6. Topology of the complex plane: open sets and domains
As we saw in §3, the metric on C coincides with the Euclidean metric on R2. In order to say precisely what Ω means when later chapters speak of “a function holomorphic on Ω”, we fix here the necessary topological vocabulary.
is called the open disc of radius r centred at a. For a set S⊆C:
A point a∈S is an interior point of S if there exists r>0 with D(a,r)⊆S.
S is open if every point of S is an interior point of S.
S is closed if the complement C∖S is open.
S is bounded if there exists M>0 such that ∣z∣≤M for all z∈S.
A point a∈C is a boundary point of S if for every r>0 the disc D(a,r) contains both a point of S and a point of C∖S. The set of all boundary points is written ∂S.
An open set Ω⊆C is connected if, whenever Ω=U∪V with U∩V=∅ and U,V both open, necessarily U=∅ or V=∅.
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 be a nonempty open set. The following two conditions are equivalent.
For all p,q∈Ω there exists a polygonal path starting at p, ending at q, all of whose segments are contained in Ω.
Proof(Proposition 6.3)
(2) ⇒ (1). We prove the contrapositive. Suppose Ω=U∪V with U∩V=∅ and U,V open and both nonempty. Choose p∈U and q∈V, and let p=p0,p1,…,pm=q be the polygonal path given by (2). Since p0∈U and pm∈V, there is an index j with pj∈U and pj+1∈V.
Write the segment as γ(t):=pj+t(pj+1−pj) for t∈[0,1], and set S:={t∈[0,1]:γ(t)∈U} and t∗:=supS. Since 0∈S we have S=∅, and S⊆[0,1] is bounded above, so the supremum exists. For c:=γ(t∗)∈Ω=U∪V we rule out two cases.
Case c∈U. Since U is open there is ε>0 with D(c,ε)⊆U. Because ∣γ(t)−γ(t∗)∣=∣t−t∗∣∣pj+1−pj∣, we have γ(t)∈U whenever ∣t−t∗∣ is small enough. If t∗=1 then c=pj+1∈U∩V=∅, a contradiction. If t∗<1 then some t∈S exceeds t∗, contradicting that t∗ is the supremum.
Case c∈V. Similarly take ε>0 with D(c,ε)⊆V; then there is δ>0 such that γ(t)∈V for all t∈[0,1] with ∣t−t∗∣<δ, hence γ(t)∈/U (as U∩V=∅). But then S∩(t∗−δ,t∗]=∅, so supS≤t∗−δ<t∗, contradicting the definition of t∗. (Note that t∗>0 follows from 0∈S and the openness of U: since γ(0)=pj∈U, nearby values of t also lie in S.)
Both cases are contradictory, so no such splitting U,V exists and Ω is connected.
(1) ⇒ (2). Fix a∈Ω and set
U:={z∈Ω:a and z can be joined by a polygonal path inside Ω},V:=Ω∖U.
Since a∈U (via the path of length 0), we have U=∅.
U is open. Given z∈U, openness of Ω provides r>0 with D(z,r)⊆Ω. A disc is convex, so for every w∈D(z,r) the segment [z,w] lies in D(z,r)⊆Ω. Appending this segment to a polygonal path from a to z produces a polygonal path from a to w, so w∈U. Hence D(z,r)⊆U.
V is open. Given z∈V, take D(z,r)⊆Ω in the same way. If some w∈D(z,r) belonged to U, then appending the segment [w,z] to a polygonal path from a to w would give z∈U, a contradiction. Hence D(z,r)⊆V.
Thus U,V split Ω into open sets with U∩V=∅ and U=∅, so (1) forces V=∅; that is, every point of Ω can be joined to a by a polygonal path. For two points p,q∈Ω, concatenate a polygonal path from p to a (traverse the path from a to p backwards) with one from a to q.
∎
Example 6.4(Deciding openness, closedness and being a domain)
(a) The annulus A={z:1<∣z∣<2} is a domain. Let us show it is open. For a∈A put r:=min{∣a∣−1,2−∣a∣}>0. If ∣z−a∣<r then by Theorem 3.4 (3) we have ∣z∣−∣a∣≤∣z−a∣<r, hence
∣z∣>∣a∣−r≥∣a∣−(∣a∣−1)=1,∣z∣<∣a∣+r≤∣a∣+(2−∣a∣)=2,
so z∈A, that is D(a,r)⊆A. Connectedness is checked with Proposition 6.3: any two points of A can be joined by first moving radially along a segment to a point on the circle ∣z∣=3/2, and then following a polygonal path inscribed in that circle (each segment can be taken inside A).
(b) The closed disc D={z:∣z∣≤1} is closed but not open. That the complement {∣z∣>1} is open follows from the same estimate as in (a). It is not open because 1∈D is not an interior point: for any r>0, taking z:=1+min{r,1}/2 gives ∣z−1∣<r and ∣z∣>1, so D(1,r)⊆D.
(c) The set H={z:Rez=0} is open but not a domain. Let us show it is open. For a∈H put r:=∣Rea∣>0. If ∣z−a∣<r then by Theorem 3.4 (1)
∣Rez−Rea∣=∣Re(z−a)∣≤∣z−a∣<r=∣Rea∣.
If Rez=0 the left-hand side would equal ∣Rea∣, contradicting this inequality. Hence Rez=0, that is D(a,r)⊆H. But H={Rez>0}∪{Rez<0} is a disjoint union of two nonempty open sets, so H is not connected in the sense of Definition 6.2. Indeed there is no polygonal path inside H joining −1 to 1, since such a path would have to cross the imaginary axis.
(d) The punctured disc D(0,1)∖{0} is a domain. Let us show it is open. For 0<∣a∣<1 put r:=min{∣a∣,1−∣a∣}>0. If ∣z−a∣<r then, as in (a), Theorem 3.4 (3) gives ∣z∣>∣a∣−r≥0 and ∣z∣<∣a∣+r≤1; in particular ∣z∣>0, that is z=0. As for connectedness: unless two points lie on the same ray from the origin they can be joined directly by a polygonal path avoiding the origin, and if they do lie on the same ray it suffices to step slightly to the side once. 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.
Since the metric on C coincides with the Euclidean metric on R2 (§3), the topological properties of R2 become properties of C verbatim. In particular the following hold.
Completeness: every Cauchy sequence (zn) of complex numbers converges. This follows because the real and imaginary parts are each Cauchy sequences in R (by Theorem 3.4 (1)), together with the completeness of R.
The Bolzano–Weierstrass theorem: every bounded sequence of complex numbers has a convergent subsequence.
The Heine–Borel theorem: a set K⊆C is compact (every open cover has a finite subcover) if and only if K is closed and bounded.
In each case the proof is the standard one for R2 (split into real and imaginary parts and apply the result for R), so we leave it to the textbooks listed in the references.
Show that there is no total order ≤ on C compatible with the field operations — that is, no total order such that x≤y implies x+z≤y+z for every z, and such that 0≤x and 0≤y imply 0≤xy. Consequently an inequality "z<w" has no meaning unless z and w are real.
Solution
Suppose such an order ≤ existed.
Lemma: if x=0 then 0<x2. Since the order is total, either 0≤x or x≤0. In the case 0≤x, apply the compatibility condition (0≤x,0≤y⇒0≤xy) with y=x to get 0≤x2. In the case x≤0, apply the translation condition with z=−x to get x+(−x)≤0+(−x), that is 0≤−x, and then the same compatibility condition gives 0≤(−x)(−x)=x2. In either case 0≤x2, and if x=0 then x2=0 (a field has no zero divisors, Theorem 2.2), so 0<x2.
Applying the lemma with x=1 gives 0<12=1, and applying it with x=i gives 0<i2=−1 (Theorem 2.2 (3)). Adding 1 to both sides of the latter gives 1<0, contradicting 0<1. Hence no such order exists.
Because of this result, the “size” of a complex number is always measured by the absolute value ∣z∣, which is real. Looking back at the places where inequalities occur from §3 onwards, one finds that both sides of every inequality sign are real numbers.
and replacing w by −w, using Re(z(−w))=−Re(zwˉ) and ∣−w∣=∣w∣,
∣z−w∣2=∣z∣2−2Re(zwˉ)+∣w∣2.
Adding the two identities, the terms in Re(zwˉ) cancel and we obtain ∣z+w∣2+∣z−w∣2=2∣z∣2+2∣w∣2.
Geometrically, in the parallelogram with vertices 0,z,z+w,w, the quantities ∣z+w∣ and ∣z−w∣ are the lengths of the two diagonals, while ∣z∣ and ∣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.
Find all solutions of the equation z4=−4, and use the result to factor the real polynomial x4+4 into a product of two quadratics with real coefficients.
Solution
Since −4=4eiπ, applying Theorem 5.4 with n=4,ρ=4,φ=π gives solutions with modulus 41/4=2:
zk=2exp(i4π+2πk)(k=0,1,2,3).
Writing these out with Theorem 4.2, and using cos(π/4)=sin(π/4)=22,
z0=2(22+22i)=1+i,z1=−1+i,z2=−1−i,z3=1−i
(each of z1,z2,z3 is z0 rotated successively by π/2, Theorem 5.1 (1)). As a check, (1+i)2=2i, so (1+i)4=(2i)2=−4; it is indeed a solution.
Now the factorization. The complex roots of x4+4 are the four numbers above, and pairing conjugate roots produces quadratics with real coefficients.
Let θ be a real number that is not an integer multiple of 2π, and let n be a positive integer. Express ∑k=0n−1eikθ in closed form using the sum of a geometric progression, and deduce from it
k=0∑n−1coskθ,k=0∑n−1sinkθ.Solution
By hypothesis eiθ=1 (uniqueness in Remark 4.4). Since C is a field (Theorem 2.2) we may use the formula for the sum of a geometric progression, and (eiθ)k=eikθ by Theorem 5.1 (2), so
S:=k=0∑n−1eikθ=eiθ−1einθ−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⋅2isin2α
(we used eiβ−e−iβ=(cosβ+isinβ)−(cosβ−isinβ)=2isinβ). Applying this with α=nθ in the numerator and α=θ in the denominator, and noting sin(θ/2)=0 (since θ∈/2πZ),
which agrees with the left-hand side cos0+cosθ=1+cosθ. 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) 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?
Why the road stops at 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 quaternionsH — at the cost of abandoning commutativity of multiplication (ij=−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 are R, C and H, and among these only R and C are commutative. In other words, as long as one demands a commutative field containing R and finite-dimensional over R, nothing strictly larger than C exists. The complex numbers are special precisely because they are a dead end.
The fundamental theorem of algebra. The motive for introducing C was “to solve x2+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 1 with complex coefficients has a root in C. Adjoining the single element i 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→C defined on a domain Ω of the complex plane, the derivative