Agmon's inequality

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In mathematical analysis, Agmon's inequalities, named after Shmuel Agmon,[1] consist of two closely related interpolation inequalities between the Lebesgue space L^\infty and the Sobolev spaces H^s. It is useful in the study of partial differential equations.

Let u\in H^2(\Omega)\cap H^1_0(\Omega) where \Omega\subset\mathbb{R}^3[vague]. Then Agmon's inequalities in 3D state that there exists a constant C such that

Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \displaystyle \|u\|_{L^\infty(\Omega)}\leq C \|u\|_{H^1(\Omega)}^{1/2} \|u\|_{H^2(\Omega)}^{1/2},


and

Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \displaystyle \|u\|_{L^\infty(\Omega)}\leq C \|u\|_{L^2(\Omega)}^{1/4} \|u\|_{H^2(\Omega)}^{3/4}.


In 2D, the first inequality still holds, but not the second: let u\in H^2(\Omega)\cap H^1_0(\Omega) where \Omega\subset\mathbb{R}^2. Then Agmon's inequality in 2D states that there exists a constant C such that

Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \displaystyle \|u\|_{L^\infty(\Omega)}\leq C \|u\|_{L^2(\Omega)}^{1/2} \|u\|_{H^2(\Omega)}^{1/2}.


For the n-dimensional case, choose s_1 and s_2 such that Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): s_1< \tfrac{n}{2} < s_2 . Then, if 0< \theta < 1 and Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \tfrac{n}{2} = \theta s_1 + (1-\theta)s_2 , the following inequality holds for any u\in H^{s_2}(\Omega)

Failed to parse (Missing <code>texvc</code> executable. Please see math/README to configure.): \displaystyle \|u\|_{L^\infty(\Omega)}\leq C \|u\|_{H^{s_1}(\Omega)}^{\theta} \|u\|_{H^{s_2}(\Omega)}^{1-\theta}


See also

Notes

  1. Lemma 13.2, in: Agmon, Shmuel, Lectures on Elliptic Boundary Value Problems, AMS Chelsea Publishing, Providence, RI, 2010. ISBN 978-0-8218-4910-1.

References

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