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arXiv 1402.0209math.FA
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关于各向同性凸体及其伴随的$L_p$ -质心体的平均宽度

On the mean-width of isotropic convex bodies and their associated $L_p$-centroid bodies

Emanuel Milman

摘要:

对于$\mathbb{R}^n$中任意原点对称凸体$K$,在各向同性位置,我们得到:\[ M^*(K) \leq C \sqrt{n} \log(n)^2 L_K ~, \]其中$M^*(K)$表示$K$的平均宽度的一半,$L_K$是$K$的各向同性常数,$C>0$是普适常数.这改进了先前最著名的估计值$M^*(K) \leq C n^{3/4} L_K$。直到$\log(n)$项和$L_K$项的幂,改进的边界是最好的可能,并且意味着各向同性位置是(直到$L_K$项)几乎$2$ -正则$M$ -位置。该界限扩展到任意位置,取决于协方差矩阵的特征值的某个加权平均。此外,该界限适用于$L_p$质心体的平均宽度,将$1 \leq p \leq \sqrt{n}$的Paouris的尖锐上限扩展到任意$p \geq \sqrt{n}$的几乎尖锐的界限。是否可以从新的边界中删除$L_K$项的问题本质上等同于$n$中对数因子内的切片问题。

英文摘要:

For any origin-symmetric convex body $K$ in $\mathbb{R}^n$ in isotropic position, we obtain the bound: \[ M^*(K) \leq C \sqrt{n} \log(n)^2 L_K ~, \] where $M^*(K)$ denotes (half) the mean-width of $K$, $L_K$ is the isotropic constant of $K$, and $C>0$ is a universal constant. This improves the previous best-known estimate $M^*(K) \leq C n^{3/4} L_K$. Up to the power of the $\log(n)$ term and the $L_K$ one, the improved bound is best possible, and implies that the isotropic position is (up to the $L_K$ term) an almost $2$-regular $M$-position. The bound extends to any arbitrary position, depending on a certain weighted average of the eigenvalues of the covariance matrix. Furthermore, the bound applies to the mean-width of $L_p$-centroid bodies, extending a sharp upper bound of Paouris for $1 \leq p \leq \sqrt{n}$ to an almost-sharp bound for an arbitrary $p \geq \sqrt{n}$. The question of whether it is possible to remove the $L_K$ term from the new bound is essentially equivalent to the Slicing Problem, to within logarithmic factors in $n$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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