Is a Harmonic Function Constant if its Square is Also Harmonic?

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    2015
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SUMMARY

The discussion centers on the mathematical proof that if a harmonic function \( f : X \to \mathbb{R} \) is such that \( f^2 \) is also harmonic, then \( f \) must be a constant function. This conclusion is established through the properties of harmonic functions and their relationship with the Laplace operator. The solution was successfully provided by the user Opalg, demonstrating the application of harmonic function theory in complex analysis.

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  • Explore the implications of the maximum principle for harmonic functions
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Here is this week's POTW:

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Let $X$ be a domain in $\mathbb C$, and let $f : X \to \Bbb R$ be a harmonic function such that $f^2$ is harmonic. Prove $f$ is constant.

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This week's problem was correctly solved by Opalg. Here is his solution.
Writing $f_x,\;f_y$ for the partial derivatives, the condition for harmonicity is $f_{xx} + f_{yy} = 0.$

For the function $f^2$, $(f^2)_x = 2ff_x$ and $(f^2)_{xx} = 2(f_x)^2 + 2ff_{xx}.$ Similarly $(f^2)_{yy} = 2(f_y)^2 + 2ff_{yy}.$ Therefore $$(f^2)_{xx} + (f^2)_{yy} = 2\bigl((f_x)^2 + (f_y)^2\bigr) + 2f\bigl(f_{xx} + f_{yy}\bigr) = 2\bigl((f_x)^2 + (f_y)^2\bigr).$$ If $f^2$ is harmonic then this must be zero. But $(f_x)^2 + (f_y)^2 = 0$ implies $f_x = f_y = 0$. Therefore $f$ is constant. (Strictly speaking, if the partial derivatives vanish then $f$ is locally constant. But since a domain has to be connected it follows that $f$ must be globally constant.)
 

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