On critical systems involving fractional Laplacian
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Consider the following non-local critical system
class="formula" id="fm0010">
class="label">class="offscreen">equation0.1
class="mathml">class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si1.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=6645dc41739412aac3d2621bc9592666">class="imgLazyJSB inlineImage" height="88" width="418" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16305017-si1.gif">class="mathContainer hidden">class="mathCode">{(Δ)suλ1u=μ1|u|22u+αγ2|u|α2u|v|βin Ω,(Δ)svλ2v=μ2|v|22v+βγ2|u|α|v|β2vin Ω,u=0,v=0in RNΩ,class="temp" src="/sd/blank.gif">
where class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si2.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=ea3b687c18f5eb216fbba77d2574f914" title="Click to view the MathML source">(−Δ)sclass="mathContainer hidden">class="mathCode">(Δ)s is fractional Laplacian, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si3.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=7bc0b6d5f8bdce37d5a774f8e6130790" title="Click to view the MathML source">0<s<1class="mathContainer hidden">class="mathCode">0<s<1 and all class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si4.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=994a1a16789a2a3a408dee7c611f94e2" title="Click to view the MathML source">λ1212,γ>0class="mathContainer hidden">class="mathCode">λ1,λ2,μ1,μ2,γ>0, class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si13.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=f8e8a4269f2f1444426c8ac06fdeac3f">class="imgLazyJSB inlineImage" height="20" width="79" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16305017-si13.gif">class="mathContainer hidden">class="mathCode">2:=2NN2s is a fractional Sobolev critical exponent, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si6.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=2da5dffee4e444839c5c151e8e05d6e2" title="Click to view the MathML source">N>2sclass="mathContainer hidden">class="mathCode">N>2s, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si7.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=8da188a4fbb87f10989532b51f71cd60" title="Click to view the MathML source">α,β>1class="mathContainer hidden">class="mathCode">α,β>1, class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si14.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=98c94dc624225d21dcc252298fa714b5" title="Click to view the MathML source">α+β=2class="mathContainer hidden">class="mathCode">α+β=2, and Ω is an open bounded domain in class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16305017&_mathId=si147.gif&_user=111111111&_pii=S0022247X16305017&_rdoc=1&_issn=0022247X&md5=ce265466aa1c875411996ff59f1b5152" title="Click to view the MathML source">RNclass="mathContainer hidden">class="mathCode">RN with Lipschitz boundary. Under proper conditions, we establish the existence result of the ground state solution to system (0.1).

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