arXiv2019
Let $Π_n^d$ denote the space of spherical polynomials of degree at most $n$ on the unit sphere $\mathbb{S}^d\subset \mathbb{R}^{d+1}$ that is equipped with the surface Lebesgue measure $dσ$ normalized by $\int_{\mathbb{S}^d} \, dσ(x)=1$. This paper establishes a close connection between the asymptotic Nikolskii constant, $$ \mathcal{L}^\ast(d):=\lim_{n\to \infty} \frac 1 {\dim Π_n^d} \sup_{f\in Π_n^d} \frac { \|f\|_{L^\infty(\mathbb{S}^d)}}{\|f\|_{L^1(\mathbb{S}^d)}},$$ and the following extremal problem: $$ \mathcal{I}_α:=\inf_{a_k} \Bigl\| j_{α+1} (t)- \sum_{k=1}^\infty a_k j_α \bigl( q_{α+1,k}t/q_{α+1,1}\bigr)\Bigr\|_{L^\infty(\mathbb{R}_+)} $$ with the infimum being taken over all sequences $\{a_k\}_{k=1}^\infty\subset \mathbb{R}$ such that the infinite series converges absolutely a.e. on $\mathbb{R}_+$. Here $j_α$ denotes the Bessel function of the first kind normalized so that $j_α(0)=1$, and $\{q_{α+1,k}\}_{k=1}^\infty$ denotes the strict increasing sequence of all positive zeros of $j_{α+1}$. We prove that for $α\ge -0.272$, $$\mathcal{I}_α= \frac{\int_{0}^{q_{α+1,1}}j_{α+1}(t)t^{2α+1}\,dt}{\int_{0}^{q_{α+1,1}}t^{2α+1}\,dt}= {}_{1}F_{2}\Bigl(α+1;α+2,α+2;-\frac{q_{α+1,1}^{2}}{4}\Bigr). $$ As a result, we deduce that the constant $\mathcal{L}^\ast(d)$ goes to zero exponentially fast as $d\to\infty$: \[ 0.5^d\le \mathcal{L}^{*}(d)\le (0.857\cdots)^{d\,(1+\varepsilon_d)} \ \ \ \ \ \text{with $\varepsilon_d =O(d^{-2/3})$.} \]