es
Throughout ℂ stands for the set of all complex numbers. If z = x + ⅉy ∈ ℂ, its complex conjugate is denoted by z = x − ⅉy, where ⅉ or j denotes the imaginary unit, so ⅉ² = −1.

Holomorphic functions

We consider functions of complex variable z ∈ ℂ defined on some domain Ω ⊂ ℂ. We also expect that f(z) will in general take values in &Co pf; as well.

If f(z) = u + ⅉv, then the function u(x, y) is called the real part of f and v(x, y) is called the imaginary part of f. Of course, it will not in general be possible to plot the graph of f(z), which will lie in ℂ², the set of ordered pairs of complex numbers, that is the set {(z,w) ∈ ℂ² : w = f(z)}. The graph can also be viewed as the subset of ℝ4 given by {(x, y, s, t): s = u(x, y), t = v(x, y)}. In particular, it lies in a four-dimensional space.

If z = x + ⅉy, then a function f(z) is simply a function f(x, y) = u(x, y)+ ⅉv(x, y) of the two real variables x and y. As such, it is a function (mapping) from ℝ² to ℝ². The usual operations on complex numbers extend to complex functions: given a complex function f(z) = u + ⅉv, we can define functions Re f(z = u (the real part is also denoted by ℜ), Im f(z = v (the imaginary part is also denoted by ℑ), complex conjugate f(z = u − ⅉv, \( \displaystyle \quad |f(z)| = \sqrt{u^2 + v^2} . \quad \) Likewise, if g(z) is another complex-valued function, we can define f(z) g(z) and f(z)/g(z) provided g(z) ≠ 0.

Limits and continuity

The absolute value measures the distance between two complex numbers. Thus, z₁ and z₂ are close when |z₁ − z₂| is small. We can then define the limit of a complex-valued function f(z) as follows: we write

\[ \lim_{z\to c} \ f(z) = C , \]
where c and C are understood to be complex numbers, if the distance from f(z) to C, |f(z) − C|, is small whenever |zc| is small. More precisely, if we want |f(z) − C| to be less than some small specified positive real number ε, then there should exist a positive real number δ such that, if |zc| < δ, then |f(z) − C| < ε. Note that, as with real functions, it does not matter if f(c) = C or even that f(z) be defined at c. It is easy to see that, if c =(c₁, c₂), C = 𝑎 + ⅉb and f(z) = u + ⅉv is written as real and imaginary parts, then \( \displaystyle \quad \lim_{z \to c} \ f(z) = C \quad \) if and only if \( \displaystyle \quad \lim_{(x,y) \to (c_1 ,c_2 )}\ u(x,y) = a \quad\mbox{and} \quad \lim_{(x,y) \to (c_1 ,c_2 )}\ v(x,y) = b . \quad \) Thus, the story for limits of functions of a complex variable is the same as the story for limits of real valued functions of the variables x, y. However, a real variable x can approach a real number c only from above or below (or from the left or right, depending on your point of view), whereas there are many ways for a complex variable to approach a complex number c.

Sequences, limits of sequences, convergent series and power series can be defined similarly.

As for functions of a real variable, a function f(z) is continuous at c if

\[ \lim_{z\to c} \ f(z) = f(c) . \]
In other words, the limit exists, f(·) is defined at z = c, and its value at c is the limiting value. A function f(·) is continuous in some domain Ω ⊆ ℂ if it is continuous at all points z ∈ Ω. It means that a function f(z) = u + ⅉv is continuous if and only if its real and imaginary parts are continuous; so that the usual functions z, z, Rez, Imz, |z|, ez are continuous. z are continuous

Cauchy--Riemann equations

arx = Graphics[{Black, Thickness[0.01], Arrowheads[0.09], Arrow[{{-0.3, 0}, {1.5, 0}}]}]; ary = Graphics[{Black, Thickness[0.01], Arrowheads[0.09], Arrow[{{0, -0.15}, {0, 1.1}}]}]; tr = Graphics[{Blue, Thickness[0.008], Line[{{0.4, 0.3}, {1.1, 0.3}, {1.1, 0.8}}]}]; ar = Graphics[{Blue, Thickness[0.008], Arrowheads[0.05], Arrow[{{0.4, 0.3}, {1.1, 0.8}}]}]; txt = Graphics[{Black, Text[Style[x, 14], {1.6, 0.16}], Text[Style[y, 14], {-0.1, 1.1}], Text[Style[\[CapitalDelta]x, 14], {0.8, 0.2}], Text[Style[\[ImaginaryJ] \[CapitalDelta]y, 14], {1.25, 0.5}], Text[Style[\[CapitalDelta]z, 14], {0.7, 0.65}]}]; Show[arx, ary, ar, tr, txt, PlotRange -> {{-0.5, 2}, {-0.5, 1.2}}] /
Approximation of derivative.

The derivative of a complex-valued function 𝑓(z), denoted 𝑓′(z), is defined by
\[ \lim_{\Delta z \to 0} \ \frac{f(z + \Delta z) - f(z)}{\Delta z} , \]
if it exists. Here z = 𝑥 + ⅉy is a complex number and ⅉ or j is the imaginary unit in the complex plane ℂ, so ⅉ² = −1. In Δz = Δ𝑥 + ⅉΔy, Δ𝑥 and Δy are independent of each other.
Now if 𝑓(z) = u(𝑥, y) + ⅉv(𝑥, y), then
\begin{align*} f' (z) &= \lim_{\substack{\Delta z \to 0 \\ y\mbox{ is fixed}}} \ \frac{u(x + \Delta x, y) + \mathbf{j}\,v(x+ \Delta x, y) - u(x,y) - \mathbf{j}\,v(x,y)}{\Delta x} \\ &= \frac{\partial u}{\partial x} + \mathbf{j}\,\frac{\partial v}{\partial x} . \end{align*}
Similarly, when x is fixed, we have
\begin{align*} f' (z) &= \lim_{\substack{\Delta z \to 0 \\ x\mbox{ is fixed}}} \ \frac{u(x, y + \Delta y) + \mathbf{j}\,v(x, y+ \Delta y) - u(x,y) - \mathbf{j}\,v(x,y)}{\mathbf{j}\,\Delta y} \\ &= \frac{1}{\mathbf{j}}\,\frac{\partial u}{\partial y} + \frac{\partial v}{\partial y} = - \mathbf{j}\, \frac{\partial u}{\partial y} + \frac{\partial v}{\partial y} . \end{align*}
Thus, approaching 0 along horizontal and vertical directions has given two different expressions. Equating real and imaginary parts, we see that: if a function f(z) = u + ⅉv is complex differentiable, then its real and imaginary parts satisfy the Cauchy-Riemann equations:
\begin{equation} \label{EqCR.1} \frac{\partial u}{\partial x} = \frac{\partial v}{\partial y} , \qquad\quad \frac{\partial u}{\partial y} = -\frac{\partial v}{\partial x} . j \end{equation}
The Cauchy–Riemann equations first appeared in the work of Jean le Rond d'Alembert. Later, Leonhard Euler connected this system to the analytic functions. Augustin-Louis Cauchy then used these equations to construct his theory of functions. Bernhard Riemann's dissertation on the theory of functions appeared in 1851.

   
Example 1:    ■
End of Example 1

 

 

  1. Apostol, T.M., Calculus, Vol. 2: Multi-Variable Calculus and Linear Algebra with Applications to Differential Equations and Probability, Wiley; 2nd edition, 1991; ISBN-13: ‎ 978-0471000075.