MHB Is Every Solution to a Certain PDE on a Closed Manifold Constant?

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    2016
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Every smooth solution to the PDE fΔf = -α|∇f|² on a closed, connected Riemannian manifold M is constant. This result highlights the implications of the geometry of the manifold on the behavior of solutions to the PDE. The discussion emphasizes the significance of the closed manifold condition in deriving this conclusion. No responses were provided to the problem, indicating a potential challenge in solving it. The original poster has shared their solution for further insight.
Euge
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Here is this week's POTW:

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Let $M$ be a closed, connected Riemannian manifold. Prove that every $C^\infty(M;\Bbb R)$-solution of the PDE

$$f\Delta f = -\alpha |\nabla f|^2\quad (\alpha\in \Bbb R)$$ is constant.

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No one answered this week's problem. You can read my solution below.
Let $f$ be a solution of the PDE in $C^\infty(M;\Bbb R)$. Suppose $\alpha = 1$. Then

$\displaystyle \quad \Delta(f^2) = 2f\Delta f + 2|\nabla f|^2 = 0$.

Therefore $f^2$ is harmonic on $M$, and thus $f$ is constant.

Now suppose $\alpha \neq 1$. Then

$\displaystyle \text{div}(f\nabla f) = \frac{\Delta(f^2)}{2} = f\nabla f + |\nabla f|^2 = (1 - \alpha)|\nabla f|^2$.

Since $M$ is closed, the divergence theorem gives

$0 = \displaystyle \int_M \text{div}(f\nabla f)\, dV = (1 - \alpha) \int_M |\nabla f|^2\, dV$.

As $\alpha \neq 1$, it follows that

$\displaystyle \int_M |\nabla f|^2 \, dV = 0$

and thus $|\nabla f| = 0$. Hence $f$ is constant.