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[parent] closure properties of Cauchy-Riemann equations (Theorem)

The set of solutions of the Cauchy-Riemann equations is closed under a surprisingly large number of operations. For convenience, let us introduce the notational conventions that $f$ and $g$ are complex functions with $f(x+iy) = u(x,y) + i v(x,y)$ and $g(x + iy) = p(x,y) + i q (x,y)$ . Let $D$ and $D'$ denote open subsets of the complex plane.

Theorem 1   If $f \colon D \to \mathbb{C}$ and $g \colon D \to \mathbb{C}$ satisfy the Cauchy-Riemann equations, so does $f + g$ . Furthermore, if $z\in \mathbb{C}$ , then $zf$ satisfies the Cauchy-Riemann equations.
Proof. This is an immediate consequence of the linearity of derivatives. $ \qedsymbol$
Theorem 2   If $f \colon D \to \mathbb{C}$ and $g \colon D \to \mathbb{C}$ satisfy the Cauchy-Riemann equations, so does $f \cdot g$ .
Proof. Letting $h$ and $k$ denote the real and imaginary parts of $f \cdot g$ respectively, we have
$\displaystyle {\partial h \over \partial x} - {\partial k \over \partial y}$ $\displaystyle = {\partial \over \partial x} \left( up - vq \right) - {\partial \over \partial y} \left( uq + vp \right)$    
  $\displaystyle = u {\partial p \over \partial x} + p {\partial u \over \partial ... ...\partial y} - v {\partial p \over \partial y} - p {\partial v \over \partial y}$    
  $\displaystyle = u \left( {\partial p \over \partial x} - {\partial q \over \par... ...left( {\partial u \over \partial y} + {\partial v \over \partial x} \right) = 0$    

and
$\displaystyle {\partial h \over \partial y} + {\partial k \over \partial x}$ $\displaystyle = {\partial \over \partial y} \left( up - vq \right) + {\partial \over \partial x} \left( uq + vp \right)$    
  $\displaystyle = u {\partial p \over \partial y} + p {\partial u \over \partial ... ...\partial x} + v {\partial p \over \partial x} + p {\partial v \over \partial x}$    
  $\displaystyle = u \left( {\partial p \over \partial y} + {\partial q \over \par... ...ft( {\partial u \over \partial x} - {\partial v \over \partial y} \right) = 0 .$    

$ \qedsymbol$
Theorem 3   If $f \colon D \to D'$ and $g \colon D' \to \mathbb{C}$ satisfy the Cauchy-Riemann equations, so does $f \circ g$ .
Proof. Letting $h$ and $k$ denote the real and imaginary parts of $f \circ g$ respectively, we have
$\displaystyle {\partial h \over \partial x} - {\partial k \over \partial y}$ $\displaystyle = {\partial \over \partial x} u(p(x,y),q(x,y)) - {\partial \over \partial y} v(p(x,y),q(x,y))$    
  $\displaystyle = {\partial u \over \partial p} {\partial p \over \partial x} + {... ...\over \partial y} - {\partial v \over \partial q} {\partial q \over \partial y}$    
  $\displaystyle = {\partial u \over \partial p} \left( {\partial p \over \partial... ...left( {\partial u \over \partial q} + {\partial v \over \partial p} \right) = 0$    

and
$\displaystyle {\partial h \over \partial y} + {\partial k \over \partial x}$ $\displaystyle = {\partial \over \partial y} u(p(x,y),q(x,y)) + {\partial \over \partial x} v(p(x,y),q(x,y))$    
  $\displaystyle = {\partial u \over \partial p} {\partial p \over \partial y} + {... ...\over \partial x} + {\partial v \over \partial q} {\partial q \over \partial x}$    
  $\displaystyle = {\partial u \over \partial p} \left( {\partial p \over \partial... ...left( {\partial u \over \partial q} + {\partial v \over \partial p} \right) = 0$    

$ \qedsymbol$
Theorem 4   If $f \colon D \to \mathbb{C}$ satisfies the Cauchy-Riemann equations, and has non-vanishing Jacobian, then $f^{-1}$ also satisfies the Cauchy-Riemann equations.
Proof. Let us denote the real and imaginary parts of $f^{-1}$ as $h$ and $k$ , respectively. Then, by definition of inverse function, we have
$\displaystyle u(h(x,y), k(x,y))$ $\displaystyle = x$    
$\displaystyle v(h(x,y), k(x,y))$ $\displaystyle = y .$    

Taking derivatives,
$\displaystyle {\partial u \over \partial h} {\partial h \over \partial x} + {\partial u \over \partial k} {\partial k \over \partial x}$ $\displaystyle = 1$    
$\displaystyle {\partial u \over \partial h} {\partial h \over \partial y} + {\partial u \over \partial k} {\partial k \over \partial y}$ $\displaystyle = 0$    
$\displaystyle {\partial v \over \partial h} {\partial h \over \partial x} + {\partial v \over \partial k} {\partial k \over \partial x}$ $\displaystyle = 0$    
$\displaystyle {\partial v \over \partial h} {\partial h \over \partial y} + {\partial v \over \partial k} {\partial k \over \partial y}$ $\displaystyle = 1$    

By the Cauchy-Riemann equations, $\partial u / \partial h = \partial v / \partial k$ and $\partial u / \partial k = - \partial v / \partial h$ . Using these relations to re-express the derivatives of $u$ as derivatives of $v$ , then subtracting the fourth equation form the first equation and adding the second and third equations, we obtain
$\displaystyle {\partial u \over \partial h} \left( {\partial h \over \partial x... ...k} \left( {\partial h \over \partial y} + {\partial k \over \partial x} \right)$ $\displaystyle = 0$    
$\displaystyle {\partial u \over \partial h} \left( {\partial h \over \partial y... ...k} \left( {\partial h \over \partial x} - {\partial k \over \partial y} \right)$ $\displaystyle = 0 .$    

With a little algebraic manipulation, we may conclude
$\displaystyle \left( \left( {\partial u \over \partial h} \right)^2 + \left( {\... ...t) \left( {\partial h \over \partial y} + {\partial k \over \partial x} \right)$ $\displaystyle = 0$    
$\displaystyle \left( \left( {\partial u \over \partial h} \right)^2 + \left( {\... ...t) \left( {\partial h \over \partial x} - {\partial k \over \partial y} \right)$ $\displaystyle = 0 .$    

Note that, by the Cauchy-Riemann equations, the Jacobian of $f$ equals the common prefactor of these equations: $$ {\partial (u,v) \over \partial (h,k)} = {\partial u \over \partial h} {\partial v \over \partial k} - {\partial u \over \partial k} {\partial v \over \partial h} = \left( {\partial u \over \partial h} \right)^2 + \left( {\partial u \over \partial k} \right)^2 $$ Hence, by assumptions, this quantity differs from zero and we may cancel it to obtain the Cauchy-Riemann equations for $f^{-1}$ . $ \qedsymbol$




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See Also: tangential Cauchy-Riemann complex of $C^{\infty)$-smooth forms, tangential Cauchy-Riemann complex of smooth forms


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Cross-references: algebraic, equation, relations, inverse function, Jacobian, imaginary parts, real, derivatives, consequence, complex plane, open subsets, complex functions, operations, number, closed under, Cauchy-Riemann equations, solutions

This is version 11 of closure properties of Cauchy-Riemann equations, born on 2008-01-12, modified 2008-05-06.
Object id is 10189, canonical name is ClosurePropertiesOfCauchyRiemannEquations.
Accessed 857 times total.

Classification:
AMS MSC30E99 (Functions of a complex variable :: Miscellaneous topics of analysis in the complex domain :: Miscellaneous)

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