Sobolev-BMO and fractional integrals on super-critical ranges of Lebesgue spaces
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In this article, we explore the mapping and boundedness properties of linear and bilinear fractional integral operators acting on Lebesgue spaces with large indices. The prototype ν  -order fractional integral operator is the Riesz potential class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si1.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=8e07cf170075e093857e2fac110ee52e" title="Click to view the MathML source">Iνclass="mathContainer hidden">class="mathCode">Iν, and the standard estimates for class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si1.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=8e07cf170075e093857e2fac110ee52e" title="Click to view the MathML source">Iνclass="mathContainer hidden">class="mathCode">Iν are from class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si2.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=75faae3c94ea2f4c169ab8b9d78be339" title="Click to view the MathML source">Lpclass="mathContainer hidden">class="mathCode">Lp into class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si3.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=f3cdd959a191d1f5b61df2383d595453" title="Click to view the MathML source">Lqclass="mathContainer hidden">class="mathCode">Lq when class="mathmlsrc">itle="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si4.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=e9e6c000b85fd9bd767a409f221053a0">class="imgLazyJSB inlineImage" height="18" width="71" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022123616303196-si4.gif">class="mathContainer hidden">class="mathCode">1<p<nν and class="mathmlsrc">itle="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si32.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=5965d40a472d112f022525becde64ccb">class="imgLazyJSB inlineImage" height="22" width="73" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022123616303196-si32.gif">class="mathContainer hidden">class="mathCode">1p=1q+νn. We show that a ν  -order linear fractional integral operator can be continuously extended to a bounded operator from class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si2.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=75faae3c94ea2f4c169ab8b9d78be339" title="Click to view the MathML source">Lpclass="mathContainer hidden">class="mathCode">Lp into the Sobolev-BMO   space class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si54.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=b95ab6851a303e49a0aa16b7b09c57ed" title="Click to view the MathML source">Is(BMO)class="mathContainer hidden">class="mathCode">Is(BMO) when class="mathmlsrc">itle="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si7.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=f8d572a69a02d03fe733edcb49a579b0">class="imgLazyJSB inlineImage" height="17" width="80" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022123616303196-si7.gif">class="mathContainer hidden">class="mathCode">nνp< and class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si8.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=f312c8b3339a849ec7e3d09273afcf06" title="Click to view the MathML source">0≤s<νclass="mathContainer hidden">class="mathCode">0s<ν satisfy class="mathmlsrc">itle="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si58.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=fc8182b771c8cf17c2eaa6320d3645a2">class="imgLazyJSB inlineImage" height="22" width="59" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022123616303196-si58.gif">class="mathContainer hidden">class="mathCode">1p=νsn. Likewise, we prove estimates for ν  -order bilinear fractional integral operators from class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si10.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=bf874ff9081478b59b6451ec436a2ab6" title="Click to view the MathML source">Lp1×Lp2class="mathContainer hidden">class="mathCode">Lp1×Lp2 into class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si54.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=b95ab6851a303e49a0aa16b7b09c57ed" title="Click to view the MathML source">Is(BMO)class="mathContainer hidden">class="mathCode">Is(BMO) for various ranges of the indices class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si11.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=002fae8aa964dabde87c643f0155f61d" title="Click to view the MathML source">p1class="mathContainer hidden">class="mathCode">p1, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si12.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=c530fad0e79aa63a6786fd8d9bad09b6" title="Click to view the MathML source">p2class="mathContainer hidden">class="mathCode">p2, and s   satisfying class="mathmlsrc">itle="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022123616303196&_mathId=si103.gif&_user=111111111&_pii=S0022123616303196&_rdoc=1&_issn=00221236&md5=4693c118743e88503574a05eb50fa113">class="imgLazyJSB inlineImage" height="22" width="102" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022123616303196-si103.gif">class="mathContainer hidden">class="mathCode">1p1+1p2=νsn.

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