Fractional p-Laplacian evolution equations
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In this paper we study the fractional p-Laplacian evolution equation given by
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mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si2.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=64f0c3f8d802475f336f62be4503afbe" title="Click to view the MathML source">0<s<1, mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si3.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=f04350c14ac9d8fdd5a040fc11234e69" title="Click to view the MathML source">p≥1. In a bounded domain Ω we deal with the Dirichlet problem by taking mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si4.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=96f60e0bf640aa064717943b03558c8f" title="Click to view the MathML source">A=RN and mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si5.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=9ea824c6c0ddc085a443ea5f08c57553" title="Click to view the MathML source">u=0 in mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si6.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=1cf7ca07b806341955811338e8ee6e78" title="Click to view the MathML source">RN∖Ω, and the Neumann problem by taking mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si7.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=e44ff624e6336358f8722a9a4e5ee8f9" title="Click to view the MathML source">A=Ω. We include here the limit case mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si8.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=c3aac8f5d6a6967b4bb92f6e97fa49e6" title="Click to view the MathML source">p=1 that has the extra difficulty of giving a meaning to 2416000052&_mathId=si18.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=184a2613fd56463e2205e45160164a57">View the MathML source2416000052-si18.gif"> when mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si10.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=bb1e8434752bd7146f42bece8128e94b" title="Click to view the MathML source">u(y)=u(x). We also consider the Cauchy problem in the whole mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si11.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=f01da517382f3574056c1ba10ad2bb6e" title="Click to view the MathML source">RN by taking mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si12.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=b7c7a7e312cb28ac3981997d2d739557" title="Click to view the MathML source">A=Ω=RN. We find existence and uniqueness of strong solutions for each of the above mentioned problems. We also study the asymptotic behaviour of these solutions as mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si13.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=4211d8e6042fd199d796a45d57f216cb" title="Click to view the MathML source">t→∞. Finally, we recover the local p  -Laplacian evolution equation with Dirichlet or Neumann boundary conditions, and for the Cauchy problem, by taking the limit as mulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0021782416000052&_mathId=si14.gif&_user=111111111&_pii=S0021782416000052&_rdoc=1&_issn=00217824&md5=8e349b44ac2382def3abc6efe7c17aea" title="Click to view the MathML source">s→1 in the nonlocal problems multiplied by a suitable scaling constant.

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