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

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    2016
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SUMMARY

In the discussion regarding the problem of the week (POTW), it is established that for a closed, connected Riemannian manifold \( M \), every \( C^\infty(M;\mathbb{R}) \)-solution of the partial differential equation (PDE) \( f\Delta f = -\alpha |\nabla f|^2 \) (where \( \alpha \in \mathbb{R} \)) is constant. This conclusion is derived from the properties of Riemannian manifolds and the implications of the given PDE. The problem remains unsolved by participants, indicating a need for deeper exploration of the underlying mathematical principles.

PREREQUISITES
  • Understanding of Riemannian geometry
  • Familiarity with partial differential equations (PDEs)
  • Knowledge of the Laplace operator (\( \Delta \)) and gradient (\( \nabla \)) in differential geometry
  • Concept of smooth functions (\( C^\infty \)) on manifolds
NEXT STEPS
  • Study the properties of closed Riemannian manifolds
  • Explore the implications of the Laplace operator in Riemannian geometry
  • Investigate the role of gradient flow in PDEs
  • Learn about the maximum principle for solutions of PDEs
USEFUL FOR

Mathematicians, particularly those specializing in differential geometry and analysis, as well as students and researchers interested in the behavior of solutions to PDEs on manifolds.

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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Remember to read the http://www.mathhelpboards.com/showthread.php?772-Problem-of-the-Week-%28POTW%29-Procedure-and-Guidelines to find out how to http://www.mathhelpboards.com/forms.php?do=form&fid=2!
 
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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.
 

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