REVIEW 3 cited by
H\"older Continuity of the Gradient of Solutions to Doubly Non-Linear Parabolic Equations
Not yet reviewed by Pith; the record is open.
This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.
SPECIMEN: schema-true, not a live event
T0 review · schema-true
One-sentence machine reading of the paper's core claim.
pith:XXXXXXXX · record.json · timestamp
abstract
This paper is devoted to studying the local behavior of non-negative weak solutions to the doubly non-linear parabolic equation \begin{equation*} \partial_t u^q - \text{div}\big(|D u|^{p-2}D u\big) = 0 \end{equation*} in a space-time cylinder. H\"older estimates are established for the gradient of its weak solutions in the super-critical fast diffusion regime $0<p-1< q<\frac{N(p-1)}{(N-p)_+}$ where $N$ is the space dimension. Moreover, decay estimates are obtained for weak solutions and their gradient in the vicinity of possible extinction time. Two main components towards these regularity estimates are a time-insensitive Harnack inequality that is particular about this regime, and Schauder estimates for the parabolic $p$-Laplace equation.
Forward citations
Cited by 3 Pith papers
-
Parabolic De Giorgi classes with doubly nonlinear, nonstandard growth: local boundedness under exact integrability assumptions
A generalized parabolic De Giorgi class with unbalanced growth is shown to have locally bounded members under sharp integrability assumptions, with quantitative supremum estimates.
-
Integral Harnack estimates and the rate of extinction of singular fractional diffusion
Singular fractional p-Laplacian diffusion satisfies local integral Harnack estimates that imply finite-time extinction with (T*-t)^{1/(2-p)} decay.
-
Schauder estimates for parabolic $p$-Laplace systems
Bounded weak solutions to parabolic p-Laplace systems with Hölder continuous coefficients have locally Hölder continuous spatial gradients for every p > 1, with quantitative estimates in terms of the solution's oscillation.
Discussion (0). Continue with ORCID to comment.