A uniqueness result for a semipositone p-Laplacian problem on the exterior of a ball
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We consider steady state reaction diffusion equations on the exterior of a ball, namely, boundary value problems of the form: where source">Δpz:=div(|∇z|p−2∇z), source">1<p<n, λ   is a positive parameter, source">r0>0 and source">ΩE:={x∈Rn | |x|>r0}. Here the weight function source">K∈C1[r0,∞) satisfies source">K(r)>0 for source">r≥r0, source">limr→∞⁡K(r)=0, and the reaction term ac0b7dd83dfae450" title="Click to view the MathML source">f∈C[0,∞)∩C1(0,∞) is strictly increasing and satisfies source">f(0)<0 (semipositone), source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16303535&_mathId=si12.gif&_user=111111111&_pii=S0022247X16303535&_rdoc=1&_issn=0022247X&md5=1bae8bdbc77500934873d946bd58fe18">View the MathML <font color=source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16303535-si12.gif">, source">lims→∞⁡f(s)=∞, source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16303535&_mathId=si14.gif&_user=111111111&_pii=S0022247X16303535&_rdoc=1&_issn=0022247X&md5=d5f4bfc3f672426254e7940ee95f6cd2">View the MathML <font color=source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16303535-si14.gif"> and source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16303535&_mathId=si15.gif&_user=111111111&_pii=S0022247X16303535&_rdoc=1&_issn=0022247X&md5=f7ee135fde423808bc7ad01fc07568a7">View the MathML <font color=source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16303535-si15.gif"> is nonincreasing on source">[a,∞) for some source">a>0 and source">q∈(0,p−1). For a class of such steady state equations it turns out that every nonnegative radial solution is strictly positive in the exterior of a ball, and exists for source">λ≫1. We establish the uniqueness of this positive radial solution for source">λ≫1.

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