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Suppose $uin dot{H}^1(mathbb{R}^n)$. In a seminal work, Struwe proved that if $ugeq 0$ and $|Delta u+u^{frac{n+2}{n-2}}|_{H^{-1}}:=Gamma(u)to 0$ then $dist(u,mathcal{T})to 0$, where $dist(u,mathcal{T})$ denotes the $dot{H}^1(mathbb{R}^n)$-distance of $u$ from the manifold of sums of Talenti bubbles. Ciraolo, Figalli and Maggi obtained the first quantitative version of Struwes decomposition with one bubble in all dimensions, namely $delta (u) leq C Gamma (u)$. For Struwes decomposition with two or more bubbles, Figalli and Glaudo showed a striking dimensional dependent quantitative estimate, namely $delta(u)leq C Gamma(u)$ when $3leq nleq 5$ while this is false for $ ngeq 6$. In this paper, we show that [dist (u,mathcal{T})leq Cbegin{cases} Gamma(u)left|log Gamma(u)right|^{frac{1}{2}}quad&text{if }n=6, |Gamma(u)|^{frac{n+2}{2(n-2)}}quad&text{if }ngeq 7.end{cases}] Furthermore, we show that this inequality is sharp.
Alexandrovs soap bubble theorem asserts that spheres are the only connected closed embedded hypersurfaces in the Euclidean space with constant mean curvature. The theorem can be extended to space forms and it holds for more general functions of the p
We prove sharp pointwise decay estimates for critical Dirac equations on $mathbb{R}^n$ with $ngeq 2$. They appear for instance in the study of critical Dirac equations on compact spin manifolds, describing blow-up profiles, and as effective equations
We establish an analog Hardy inequality with sharp constant involving exponential weight function. The special case of this inequality (for n=2) leads to a direct proof of Onofri inequality on S^2.
We prove that a plane domain which is almost isoperimetric (with respect to the $L^1$ metric) is close to a square whose sides are parallel to the coordinates axis. Closeness is measured either by $L^infty$ Haussdorf distance or Fraenkel asymmetry. I
In this paper, we derive some quantitative estimates for uniformly-rotating vortex patches. We prove that if a non-radial simply-connected patch $D$ is uniformly-rotating with small angular velocity $0 < Omega ll 1$, then the outmost point of the pat