CiteExport$(function(){PrimeFaces.cw("TieredMenu","widget_formSmash_upper_j_idt184",{id:"formSmash:upper:j_idt184",widgetVar:"widget_formSmash_upper_j_idt184",autoDisplay:true,overlay:true,my:"left top",at:"left bottom",trigger:"formSmash:upper:exportLink",triggerEvent:"click"});}); $(function(){PrimeFaces.cw("OverlayPanel","widget_formSmash_upper_j_idt186_j_idt192",{id:"formSmash:upper:j_idt186:j_idt192",widgetVar:"widget_formSmash_upper_j_idt186_j_idt192",target:"formSmash:upper:j_idt186:permLink",showEffect:"blind",hideEffect:"fade",my:"right top",at:"right bottom",showCloseIcon:true});});

Boundary Estimates for Certain Degenerate and Singular Parabolic EquationsPrimeFaces.cw("AccordionPanel","widget_formSmash_some",{id:"formSmash:some",widgetVar:"widget_formSmash_some",multiple:true}); PrimeFaces.cw("AccordionPanel","widget_formSmash_all",{id:"formSmash:all",widgetVar:"widget_formSmash_all",multiple:true});
function selectAll()
{
var panelSome = $(PrimeFaces.escapeClientId("formSmash:some"));
var panelAll = $(PrimeFaces.escapeClientId("formSmash:all"));
panelAll.toggle();
toggleList(panelSome.get(0).childNodes, panelAll);
toggleList(panelAll.get(0).childNodes, panelAll);
}
/*Toggling the list of authorPanel nodes according to the toggling of the closeable second panel */
function toggleList(childList, panel)
{
var panelWasOpen = (panel.get(0).style.display == 'none');
// console.log('panel was open ' + panelWasOpen);
for (var c = 0; c < childList.length; c++) {
if (childList[c].classList.contains('authorPanel')) {
clickNode(panelWasOpen, childList[c]);
}
}
}
/*nodes have styleClass ui-corner-top if they are expanded and ui-corner-all if they are collapsed */
function clickNode(collapse, child)
{
if (collapse && child.classList.contains('ui-corner-top')) {
// console.log('collapse');
child.click();
}
if (!collapse && child.classList.contains('ui-corner-all')) {
// console.log('expand');
child.click();
}
}
PrimeFaces.cw("AccordionPanel","widget_formSmash_responsibleOrgs",{id:"formSmash:responsibleOrgs",widgetVar:"widget_formSmash_responsibleOrgs",multiple:true}); 2016 (English)In: Journal of the European Mathematical Society (Print), ISSN 1435-9855, E-ISSN 1435-9863, Vol. 18, no 2, p. 381-424Article in journal (Refereed) Published
##### Abstract [en]

##### Place, publisher, year, edition, pages

2016. Vol. 18, no 2, p. 381-424
##### Keyword [en]

Degenerate and singular parabolic equations; Harnack estimates; boundary Harnack inequality; Carleson estimate
##### National Category

Mathematical Analysis
##### Identifiers

URN: urn:nbn:se:uu:diva-186267DOI: 10.4171/JEMS/593ISI: 000370249100005OAI: oai:DiVA.org:uu-186267DiVA, id: diva2:572812
#####

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt648",{id:"formSmash:j_idt648",widgetVar:"widget_formSmash_j_idt648",multiple:true});
#####

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt657",{id:"formSmash:j_idt657",widgetVar:"widget_formSmash_j_idt657",multiple:true});
#####

PrimeFaces.cw("AccordionPanel","widget_formSmash_j_idt667",{id:"formSmash:j_idt667",widgetVar:"widget_formSmash_j_idt667",multiple:true});
Available from: 2013-02-12 Created: 2012-11-28 Last updated: 2017-12-07Bibliographically approved
##### In thesis

We study the boundary behavior of non-negative solutions to a class of degenerate/singular parabolic equations, whose prototype is the parabolic p-Laplace equation. Assuming that such solutions continuously vanish on some distinguished part of the lateral part S-T of a Lipschitz cylinder, we prove Carleson-type estimates, and deduce some consequences under additional assumptions on the equation or the domain. We then prove analogous estimates for non-negative solutions to a class of degenerate/singular parabolic equations of porous medium type.

1. Boundary Behavior of *p*-Laplace Type Equations$(function(){PrimeFaces.cw("OverlayPanel","overlay615186",{id:"formSmash:j_idt1080:0:j_idt1093",widgetVar:"overlay615186",target:"formSmash:j_idt1080:0:parentLink",showEvent:"mousedown",hideEvent:"mousedown",showEffect:"blind",hideEffect:"fade",appendToBody:true});});

doi
urn-nbn$(function(){PrimeFaces.cw("Tooltip","widget_formSmash_j_idt1974",{id:"formSmash:j_idt1974",widgetVar:"widget_formSmash_j_idt1974",showEffect:"fade",hideEffect:"fade",showDelay:500,hideDelay:300,target:"formSmash:altmetricDiv"});});

CiteExport$(function(){PrimeFaces.cw("TieredMenu","widget_formSmash_lower_j_idt2027",{id:"formSmash:lower:j_idt2027",widgetVar:"widget_formSmash_lower_j_idt2027",autoDisplay:true,overlay:true,my:"left top",at:"left bottom",trigger:"formSmash:lower:exportLink",triggerEvent:"click"});}); $(function(){PrimeFaces.cw("OverlayPanel","widget_formSmash_lower_j_idt2028_j_idt2030",{id:"formSmash:lower:j_idt2028:j_idt2030",widgetVar:"widget_formSmash_lower_j_idt2028_j_idt2030",target:"formSmash:lower:j_idt2028:permLink",showEffect:"blind",hideEffect:"fade",my:"right top",at:"right bottom",showCloseIcon:true});});