Abstract

We investigate the existence and the boundary regularity of source-type self-similar solutions to the thin-film equation $h\_t=-(h^nh\_{zzz})z+(h^{n+3}){zz},$ $t>0,; z\in \mathbb{R};; h(0,z)= \omega \delta(z)$ where $n\in (3/2,3),; \omega > 0$ and $\delta$ is the Dirac mass at the origin. It is known that the leading order expansion near the edge of the support coincides with that of a traveling-wave solution for the standard thin-film equation: $h\_t=-(h^nh\_{zzz})\_z$. In this paper we sharpen this result, proving that the higher-order corrections are analytic with respect to three variables: the first one is just the {spatial} variable, whereas the second and the third (except for $n = 2$) are irrational powers of it. It is known that this third variable does not appear for the thin-film equation without gravity.

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