Least energy solutions for a weakly coupled fractional Schrödinger system
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In this paper, we consider the following system of two weakly coupled fractional nonlinear Schrödinger equations
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class="mathml">class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0362546X15003752&_mathId=si1.gif&_user=111111111&_pii=S0362546X15003752&_rdoc=1&_issn=0362546X&md5=04dd55e7175aec0f2c368f2ed9be44c1">class="imgLazyJSB inlineImage" height="51" width="382" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0362546X15003752-si1.gif">class="mathContainer hidden">class="mathCode">{class="cases">(Δ)su+u=(u2p+b(x)up1vp+1)uclass="quad">xRN(Δ)sv+ω2sv=(v2p+b(x)vp1up+1)vclass="quad">xRN.class="temp" src="/sd/blank.gif">
By use of the s-harmonic extension technique, we establish the existence of a nontrivial least energy solution of the system via variational methods. Especially, in the autonomous case i.e. class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0362546X15003752&_mathId=si2.gif&_user=111111111&_pii=S0362546X15003752&_rdoc=1&_issn=0362546X&md5=f403cd644fa2bde752c0d30f355dd419" title="Click to view the MathML source">b(x)≡bclass="mathContainer hidden">class="mathCode">b(x)b, a positive least energy solution with both nontrivial components is obtained.

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