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Complex numbers
Definitions

Complex numbers Definitions

A complex number zz is specified by a pair of real numbers xx and yy and written as

z=x+iyz=x+i y

where ii is the imaginary unit which has the basic property

i2=1i^{2}=-1

The set of complex numbers is denoted by C\mathbb{C}. Two elements x+iyx+i y and u+ivu+i v are equal iffiff x=ux=u and y=vy=v. Given z=x+iyz=x+i y in C,x\mathbb{C}, x is the real part of xx and yy is the imaginary part,

x=Re(z),y=Im(z).x=\operatorname{Re}(z), \quad y=\operatorname{Im}(z) .

It is convenient to represent complex numbers geometrically as points of the complex plane known as the Argand diagram shown below.

Alternatively, use polar coordinates defined through x=rcosθ,y=rsinθx=r \cos \theta, y=r \sin \theta.

Modulus & argument

The modulus z|z| of z=x+iyz=x+i y is defined to be,

z=x2+y2=r|z|=\sqrt{x^{2}+y^{2}}=r

which is the distance from zz to the origin in the complex plane. The angle θ\theta in the polar form z=r(cosθ+isinθ)z=r(\cos \theta+i \sin \theta) is the argument of zz, denoted as argz\arg z. Note that the angle θ\theta is not unique: replacing θ\theta by θ+2π\theta+2 \pi yields the same zz (this is easy to see from the figures above). For example, z=0+i1z=0+i 1 which is normally written as ii has modulus 1 and argumentarg(i)=π/2\operatorname{argument} \arg (i)=\pi / 2 as well as π/2+2nπ\pi / 2+2 n \pi where nn is an integer.

To remove this ambiguity, we restrict the range of θ\theta to π<θπ-\pi<\theta \leq \pi (or another interval of length 2π2 \pi ). Then the principal value of the argument of zz (denoted Arg(z)\operatorname{Arg}(z), i.e. with upper case A) is the argument θ\theta for which π<θπ-\pi<\theta \leq \pi. Note that we use π<θπ-\pi<\theta \leq \pi and not πθπ-\pi \leq \theta \leq \pi to avoid multiplicity at the point θ=±π\theta= \pm \pi, which represents the same point on the plane. So, while Arg(z)\operatorname{Arg}(z) is single-valued, arg(z)\operatorname{single-valued,~} \arg (z) given by

arg(z)=Arg(z)+2nπ=θ+2nπ,\arg (z)=\operatorname{Arg}(z)+2 n \pi=\theta+2 n \pi,

is not. It is a multivalued function because for a given complex number z,arg(z)z, \arg (z) represents an infinite number of possibilities. Although multivalued, it becomes especially useful when we study the properties of the complex logarithm.

For example, if we wanted to calculate arg(z)\arg (z) and Arg(z)\operatorname{Arg}(z) where z=1i3z=1-i \sqrt{3}. The polar form is:

z=reiθ=r(cosθ+isinθ)z=r e^{i \theta}=r(\cos \theta+i \sin \theta)

where r=z=13=2r=|z|=|1-\sqrt{3}|=2. Now, comparing z=1i3z=1-i \sqrt{3}

rcosθ=1,rsinθ=3,r \cos \theta=1, \quad r \sin \theta=-\sqrt{3},

which gives tanθ=3\tan \theta=-\sqrt{3}.

The point (circle marker) on the Argand diagram above shows z=13z=1-\sqrt{3} and θ\theta is the angle taken anti-clockwise between the positive xx axis and the line segment. Now, Arg(z)\operatorname{Arg}(z) must be such that π<Arg(z)π-\pi<\operatorname{Arg}(z) \leq \pi; this gives

Arg(z)=π3\operatorname{Arg}(z)=-\frac{\pi}{3}

and

arg(z)=π3+2nπ\arg (z)=-\frac{\pi}{3}+2 n \pi

for integer nn. Note that we can show tan(π/3)=3\tan (\pi / 3)=\sqrt{3} using an equilateral triangle of side 2, separated into 2 right triangles as shown below. Using Pythagoras' theorem, the perpendicular has length 3\sqrt{3} and therefore tanθ=3\tan \theta=\sqrt{3}.

Algebra in the complex plane

The rules of addition are the same as for real numbers,

(x+iy)+(u+iv)=(x+u)+i(y+v).(x+i y)+(u+i v)=(x+u)+i(y+v) .

Multiplication rules are also the same but with the additional condition i2=1i^{2}=-1.,

(x+iy)(u+iv)=(xuyv)+i(xv+yu).(x+i y) \cdot(u+i v)=(x u-y v)+i(x v+y u) .

Note that

z1z2=z1z2\left|z_{1} z_{2}\right|=\left|z_{1}\right|\left|z_{2}\right|

for any z1,z2z_{1}, z_{2} in C\mathbb{C}. As for real numbers, we have the following commutative laws,

z1+z2=z2+z1z1z2=z2z1\begin{aligned} z_{1}+z_{2} & =z_{2}+z_{1} \\ z_{1} z_{2} & =z_{2} z_{1} \end{aligned}

and associative laws,

z1+(z2+z3)=(z1+z2)+z3,(z1z2)z3=z1(z2z3)\begin{aligned} z_{1}+\left(z_{2}+z_{3}\right) & =\left(z_{1}+z_{2}\right)+z_{3}, \\ \left(z_{1} z_{2}\right) z_{3} & =z_{1}\left(z_{2} z_{3}\right) \end{aligned}

for any z1,z2,z3z_{1}, z_{2}, z_{3} in C\mathbb{C}. For z=x+iyz=x+i y in C,z\mathbb{C},-z is defined to be (x)+i(y)(-x)+i(-y). Clearly, z+(z)=0z+(-z)=0.

Complex conjugation

The conjugate of a complex number z=x+iyz=x+i y in C\mathbb{C} is denoted by zˉ\bar{z} (or zz^{*} ) and is the complex number zˉ=xiy\bar{z}=x-i y, i.e. it is the original complex number with the sign of the imaginary part reversed. In polar form, zˉ=reiθ\bar{z}=r e^{-i \theta} if z=reiθz=r e^{i \theta}. In the Argand diagram, zˉ\bar{z} is the reflection of zz about the real axis. The following hold if z,z1,z2z, z_{1}, z_{2} are complex numbers:

  1. zˉ=z;\overline{\bar{z}}=z ;
  2. Re(z)=z+zˉ2,Im(z)=zzˉ2i\operatorname{Re}(z)=\frac{z+\bar{z}}{2}, \quad \operatorname{Im}(z)=\frac{z-\bar{z}}{2 i};
  3. z1+z2=z1+z2\overline{z_{1}+z_{2}}=\overline{z_{1}}+\overline{z_{2}};
  4. z1z2=z1z2\overline{z_{1} \cdot z_{2}}=\overline{z_{1}} \cdot \overline{z_{2}};
  5. zˉ=z|\bar{z}|=|z|.

Complex reciprocal

For z=x+iy0z=x+i y \neq 0, the reciprocal, 1/z1 / z (also written as z1z^{-1} ) is defined through

1z=xx2+y2iyx2+y2\frac{1}{z}=\frac{x}{x^{2}+y^{2}}-i \frac{y}{x^{2}+y^{2}}

To derive this result, start from the reciprocal of a complex number z=x+iyz=x+i y and multiply by zˉ/zˉ\bar{z} / \bar{z}, where zˉ\bar{z} is the conjugate:

1z=1zzˉzˉ\frac{1}{z}=\frac{1}{z} \frac{\bar{z}}{\bar{z}}

yielding a real denominator as

(x+iy)(xiy)=x2i2y2=x2+y2(x+i y)(x-i y)=x^{2}-i^{2} y^{2}=x^{2}+y^{2}

from which the result follows. Like real numbers, the reciprocal has the property

z1z=1z \cdot \frac{1}{z}=1

Note that

1z=1z\left|\frac{1}{z}\right|=\frac{1}{|z|}

To obtain the reciprocal in polar form, and starting from the equation, we have

1z=xx2+y2iyx2+y2=rcosθr2irsinθr2=cosθrisinθr\begin{aligned} \frac{1}{z} & =\frac{x}{x^{2}+y^{2}}-i \frac{y}{x^{2}+y^{2}} \\ & =\frac{r \cos \theta}{r^{2}}-i \frac{r \sin \theta}{r^{2}} \\ & =\frac{\cos \theta}{r}-i \frac{\sin \theta}{r} \end{aligned}

Or simply, by replacing in the polar form z=rcosθ+irsinθ,rz=r \cos \theta+i r \sin \theta, r with 1/r1 / r and θ\theta with θ-\theta.