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Consider a random vector X with the coordinate distribution is uniformly distributed in the set $\{\sqrt{n}e_i : i = 1,..., n\}$, where $e_i$ denotes the n-element set of the canonical basis vectors in $R^n$. Show that $ \parallel X \parallel_{ \psi 2}\asymp \sqrt{\frac{n}{{ log n}}}.$

By the definition of the sub-gaussian norm of a random vector, $\parallel X\parallel_{ \psi_2}=\sup_{x∈S^{n−1}}\parallel <X, x>\parallel_{\psi 2} $, for all $x ∈ R^n$.

I tried to consider $\sup_{x∈S^{n−1}}\parallel <X, x>\parallel_{\psi 2}=\sup_{x∈S^{n−1}} \parallel \sum_{i=1}^n x_iX_i\parallel_{\psi_2}$, while I am not sure how to precede next? Thank you!

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  • $\begingroup$ Why do you say "show that"? Where do the question and the belief come from? $\endgroup$
    – user44143
    Commented Mar 2, 2020 at 14:34
  • $\begingroup$ This is a result I read from section 3.4.2 of book "high dimensional probability" by Vershynin. I am trying to prove this argument. $\endgroup$
    – Chen
    Commented Mar 2, 2020 at 14:40

1 Answer 1

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The subgaussian norm of a real-valued random variable $Y$ is $$\|Y\|:=\|Y\|_{\psi_2}:=\inf\{t>0\colon Ee^{Y^2/t^2}\le2\}.$$ If $Y$ is such that $P(Y=0)<1$ and $Ee^{Y^2/t^2}<\infty$ for all real $t>0$, then $Ee^{Y^2/t^2}$ continuously decreases in real $t>0$ from $\infty$ to $0$, so that $\|Y\|$ is the unique positive root of the equation $$Ee^{Y^2/\|Y\|^2}=2.$$

So, for $x=(x_1,\dots,x_n)\in S^{n-1}$ and $\nu_x:=\|X\cdot x\|$, where $X\cdot x:=\langle X,x\rangle$, we have $$2=E\exp\frac{(X\cdot x)^2}{\|X\cdot x\|^2} =\frac1n\,\sum_{i=1}^n\exp\frac{nx_i^2}{\nu_x^2} \le\frac1n\,\Big(n-1+\exp\frac n{\nu_x^2}\Big), \tag{1}$$ because $\sum_{i=1}^n\exp\frac{nu_i}{\nu_x^2}$ is convex in $u=(u_1,\dots,u_n)$ in the simplex that is the image of $S^{n-1}$ under the map $(x_1,\dots,x_n)\mapsto(x_1^2,\dots,x_n^2)$, and hence $\sum_{i=1}^n\exp\frac{nu_i}{\nu_x^2}$ attains its maximum on this simplex at one of the vertices of this simplex, which latter are the standard basis vectors $e_1,\dots,e_n$ in $\mathbb R^n$.

It follows from (1) that $$\nu_x\le\sqrt{\frac n{\ln(n+1)}}$$ for all $x\in S^{n-1}$, and this upper bound on $\nu_x$ is attained if $x$ is one of the $e_i$'s. Thus, $$\|X\|=\max_{x\in S^{n-1}}\nu_x=\sqrt{\frac n{\ln(n+1)}}\sim \sqrt{\frac n{\ln n}}$$ as $n\to\infty$, as desired.

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  • $\begingroup$ Thank you so much! $\endgroup$
    – Chen
    Commented Mar 2, 2020 at 18:29

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