A Harnack inequality for solutions of elliptic-parabolic equations
Fabio Paronetto
TL;DR
This work develops a Harnack-type theory for strongly degenerate parabolic and elliptic-parabolic equations with a density $\uprho(x,t) \ge 0$, by introducing a parabolic De Giorgi class of order $2$, constructing an inhomogeneous parabolic Harnack for approximants, and passing to the limit to obtain a Harnack inequality for solutions in the degenerate regime. The analysis relies on an expansion of positivity, delicate energy estimates, and advanced covering and weight-theory tools to handle regions where $\uprho$ vanishes. A key outcome is Hölder continuity across the interface where $\uprho$ changes sign, and the results are extended to elliptic-parabolic mixtures by considering the elliptic behavior in the vanishing-density zones. The results have potential applications to diffusion and flow problems in heterogeneous media with phase interfaces.
Abstract
We want to prove a Harnack type inequality for solutions of strongly degenerate parabolic, or elliptic-parabolic, equations. To do that, we first define a De Giorgi class of order $p = 2$ that contains the solutions of evolution equations of the types $\uprho (x,t) u_t + A u = 0$ and $(\uprho (x,t) u)_t + A u = 0$, where $\uprho > 0$ almost everywhere and $A$ is a suitable elliptic operator. For functions belonging to this class we prove an inhomogeneous parabolic Harnack inequality, i.e. a Harnack inequality that takes into account the mean value of $\uprho$ in different regions of $Ω\times (0,T)$. \\ As a consequence, thanks to an approximation result and a delicate passage to the limit, we are able to get a Harnack inequality for solutions, and in these cases only for solutions, of strongly degenerating parabolic equations, i.e. when $\uprho \geqslant 0$. \\ As a byproduct one obtains Hölder continuity for solutions of a subclass of the first equation (i.e. $\uprho (x,t) u_t + A u = 0$): in particular the solutions of this subclass are Hölder continuous in the interface where $\uprho$ changes its sign, from positive to zero.
