Let me start by giving the formula
$$H_{n,l}(y_0,y_1,\dots,y_n)=\sum_{(k_1,k_2,\dots,k_{n-1})\in P_{n,l}}\frac{y_{0}}{l!}\prod_{j=1}^n (j+1-k_1-\cdots-k_j)\frac{y_{k_j}}{k_j!}$$
where, $P_{n.l}$ is the set of $(k_1,k_2,\dots,k_{n-1})\in \mathbb Z_{\geq 0}^{n-1}$ which satisfy $k_1+\cdots+k_{n-1}=n-l$ and $k_1+\cdots+k_i\le i$ for all $1\le i \le n$.
In this form this is due to L. Comtet:
L. Comtet, Une formule explicite pour les puissances successives de l'opérateur de dérivation de Lie, C. R. Acad. Sci. Paris Sér. A-B 276 (1973) A165–A168. Zbl 0252.05002
This has an OEIS entry, A139605, where you can find more references. In particular see Bergeron, F. and Reutenauer, C., Une interprétation combinatoire des puissances d'un opérateur différentiel linéaire, Ann. Sci. Math. Quebec. 11, 269–278 (1987) for a combinatorial interpretation in terms of forests of rooted trees.
The analogous expansion for the multivariable case is treated in "Universal expansion of the powers of a derivation" by M. Ginocchio. There are also generalizations to the non-commutative case that are described in his other article "On the Hopf algebra of functional graphs and differential algebras".
