Hurwitz integrality of the power series expansion of the sigma function for a telescopic curve

A telescopic curve is a certain algebraic curve defined by $m-1$ equations in the affine space of dimension $m$, which can be a hyperelliptic curve and an $(n,s)$ curve as a special case. The sigma function $\sigma (u)$ associated with the telescopic curve of genus $g$ is a holomorphic function on ${\mathbb{C}}^g$. For a subring $R$ of $\mathbb{C}$ and variables $u={}^t(u_1,\dots ,u_g)$, let $$R⟨⟨u⟩⟩=\left\{\sum _{i_1,\dots ,i_g\ge 0}{\kappa }_{i_1,\dots ,i_g}\frac{u_1^{i_1}\cdots u_g^{i_g}}{i_1!\cdots i_g!}\right|{\kappa }_{i_1,\dots ,i_g}\in R\}\mathrm{.}$$ If the power series expansion of a holomorphic function $f(u)$ on ${\mathbb{C}}^g$ around the origin belongs to $R⟨⟨u⟩⟩$, then $f(u)$ is said to be Hurwitz integral over $R$. In this paper, we show that the sigma function $\sigma (u)$ associated with the telescopic curve is Hurwitz integral over the ring generated by the coefficients of the defining equations of the curve and $\frac{1}{2}$ over $\mathbb{Z}$. Further, we show that $\sigma (u{)}^2$ is Hurwitz integral over the ring generated by the coefficients of the defining equations of the curve over $\mathbb{Z}$. Our results are a generalization of the results of Y. Ônishi for $(n,s)$ curves to telescopic curves.