Cauchy-Riemann Equations

The goal of this blog is for me to go through the derivation of Cauchy-Riemann Equations starting from derivability of a function on a complex variable. That said, this blog is aimed to improve my own understanding of the subject, and less aimed to convey the results to others, since I haven't mastered the concept.

Differentiability for R2→R2\mathbb{R}^2 \to \mathbb{R}^2 and C→C\mathbb{C} \to \mathbb{C}

Definition. Let f ⁣:Ω⊆R2→R2f \colon \Omega \subseteq \mathbb{R}^2 \to \mathbb{R}^2 be a continuous function, where Ω\Omega is an open set. We say that ff is differentiable at x0∈R2x_0 \in \mathbb{R}^2 if there exists a linear map df∣x0 ⁣:R2→R2\mathrm{d}f|_{x_0} \colon \mathbb{R}^2 \to \mathbb{R}^2 such that f(x0+h)=f(x0)+df∣x0(h)+o(h)f(x_0+h) = f(x_0) + \mathrm{d}f|_{x_0}(h) + \mathcal{o}(h) as ∥h∥→0\|h\| \to 0 (for any norm ∥⋅∥\|\cdot\|).

To motivate the definition for complex differentials, we want to replace the linear map df∣x0\mathrm{d}f|_{x_0} with a complex number df∣x0\mathrm{d}f|_{x_0}. This gives us the following definition.

Definition. Let f ⁣:Ω⊆C→Cf \colon \Omega \subseteq \mathbb{C} \to \mathbb{C} be a continuous function, where Ω\Omega is an open set. We say that ff is differentiable at z0∈Cz_0 \in \mathbb{C} (where we write z0=x0+iy0z_0 = x_0 + iy_0 so that x0,y0∈Rx_0, y_0 \in \mathbb{R}) if there exists a complex number df∣z0∈C\mathrm{d}f|_{z_0} \in \mathbb{C} such that f(z0+h)=f(z0)+df∣z0h+o(h)f(z_0+h) = f(z_0) + \mathrm{d}f|_{z_0}h + \mathcal{o}(h) as h→0h \to 0.

Well, then, suppose ff can be written as u+ivu + iv, so that f(x+iy)=u(x,y)+iv(x,y)f(x+iy) = u(x, y) + iv(x, y) for all x,y∈Rx, y \in \mathbb{R} such that x+iy∈Ωx+iy \in \Omega, and u,v ⁣:R2→Ru, v \colon \mathbb{R}^2 \to \mathbb{R}. Then what we see is that from f(z0+h)=f(z0)+df∣z0h+o(h),f(z_0 + h) = f(z_0) + \mathrm{d}f|_{z_0}h + \mathcal{o}(h), this means lim⁡h→0,h≠0f(z0+h)−f(z0)h=df∣z0\lim_{h \to 0, h \ne 0} \frac{f(z_0+h)-f(z_0)}{h} = \mathrm{d}f|_{z_0} so when we restrict hh to be real, we have lim⁡h→0,h≠0,h∈Rf(z0+h)−f(z0)h=df∣z0.\lim_{h \to 0, h \ne 0, h \in \mathbb{R}} \frac{f(z_0+h)-f(z_0)}{h} = \mathrm{d}f|_{z_0}. That is, lim⁡h→0,h≠0,h∈Ru(x0+h,y0)+iv(x0+h,y0)−u(x0,y0)−iv(x0,y0)h=df∣z0.\lim_{h \to 0, h \ne 0, h \in \mathbb{R}} \frac{u(x_0+h, y_0) + iv(x_0+h, y_0) - u(x_0, y_0) - iv(x_0, y_0)}{h} = \mathrm{d}f|_{z_0}. If we take the real part of both sides, we have lim⁡h→0,h≠0,h∈Ru(x0+h,y0)−u(x0,y0)h=ℜ(df∣z0).\lim_{h \to 0, h \ne 0, h \in \mathbb{R}} \frac{u(x_0+h, y_0) - u(x_0, y_0)}{h} = \Re(\mathrm{d}f|_{z_0}). This is precisely ∂xu(x0,y0)=ℜ(df∣z0)\partial_x u(x_0, y_0) = \Re(\mathrm{d}f|_{z_0}). Once we do the same for the imaginary part, we have ∂xv(x0,y0)=ℑ(df∣z0).\partial_x v(x_0, y_0) = \Im(\mathrm{d}f|_{z_0}). Now, instead of restricting hh to be real, let us restrict hh to be imaginary. We have lim⁡h→0,h≠0,h∈iRf(z0+h)−f(z0)h=df∣z0.\lim_{h \to 0, h \ne 0, h \in i\mathbb{R}} \frac{f(z_0+h)-f(z_0)}{h} = \mathrm{d}f|_{z_0}. or equivalently, lim⁡h→0,h≠0,h∈Ru(x0,y0+h)+iv(x0,y0+h)−u(x0,y0)−iv(x0,y0)ih=df∣z0.\lim_{h \to 0, h \ne 0, h \in \mathbb{R}} \frac{u(x_0, y_0+h) + iv(x_0, y_0+h) - u(x_0, y_0) - iv(x_0, y_0)}{ih} = \mathrm{d}f|_{z_0}. Now, using the fact that 1i=−i\frac{1}{i} = -i, we have lim⁡h→0,h≠0,h∈R−iu(x0,y0+h)+v(x0,y0+h)+iu(x0,y0)−v(x0,y0)h=df∣z0.\lim_{h \to 0, h \ne 0, h \in \mathbb{R}} \frac{-iu(x_0, y_0+h) + v(x_0, y_0+h) + iu(x_0, y_0) - v(x_0, y_0)}{h} = \mathrm{d}f|_{z_0}. Taking real part of this equation, we have ∂yv(x0,y0)=ℜ(df∣z0),\partial_y v(x_0, y_0) = \Re(\mathrm{d}f|_{z_0}), and the imaginary part gives −∂yu(x0,y0)=ℑ(df∣z0).-\partial_y u(x_0, y_0) = \Im(\mathrm{d}f|_{z_0}). Comparing these two the previous results, we have shown that ∂xu(x0,y0)=ℜ(df∣z0)=∂yv(x0,y0),\partial_x u(x_0, y_0) = \Re(\mathrm{d}f|_{z_0}) = \partial_y v(x_0, y_0), and ∂xv(x0,y0)=ℑ(df∣z0)=−∂yu(x0,y0).\partial_x v(x_0, y_0) = \Im(\mathrm{d}f|_{z_0}) = -\partial_y u(x_0, y_0). Translating these back into the notion of ff, we have that these two equations {∂xℜ(f(z0))=∂yℑ(f(z0))∂xℑ(f(z0))=−∂yℜ(f(z0))\begin{cases} \partial_x \Re(f(z_0)) = \partial_y \Im(f(z_0)) \\ \partial_x \Im(f(z_0)) = -\partial_y \Re(f(z_0)) \end{cases} hold true whenever ff is complex-differentiable at z0∈Ωz_0 \in \Omega.

These equations are, indeed, the Cauchy-Riemann equations.