Next-order asymptotic expansion of the optimal Hardy weight in dimensions d ≥ 3
Establish the conjectured next-order asymptotic expansion of the optimal Hardy weight associated with the simple random walk on \(\mathbb{Z}^d\), \(d\geq 3\), namely \(w(x)=\frac{(d-2)^2}{8d|x|^2}+\frac{Q(\omega^x)}{|x|^4}+\mathcal{O}(|x|^{-6})\), where \(\omega^x=x/|x|\) and \(Q(z)=\frac{(d-2)^2}{16d}\left(\frac{5(d+2)^2}{8}\sum_{j=1}^d z_j^4-(2d+3)\right)\).
References
For the simple random walk, with the explicit formula of the higher-order term (see the Remark following Theorem~\ref{thm:UchiyamaFukai2}) it should be possible to derive the asymptotic expansion for w = \frac{\Delta G{1/2}}{G{1/2}} with one more higher order term. After consultation with AI we conjecture it to be
w_{\mu}(x) = \frac{(d-2)2}{8 d|x|2} + \frac{Q(\omega_ix)}{|x|4} + \mathcal{O}\big(|x|{-6}\big),
with Q given as
Q(z) = \frac{(d-2)2}{16d} \left( \frac{5(d+2)2}{8} \sum_{j=1}d z_j4 -(2d+3) \right).
It remains to determine exact pure-power constants in fixed dimensions $d\geq4$ and for nonlinear discrete $p$-energies.