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Note on the weak-strong uniqueness criterion for the β-QG in Morrey-Campanato space
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Consider the β  -quasi-geostrophic equations with the initial data class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0096300316305069&_mathId=si1.gif&_user=111111111&_pii=S0096300316305069&_rdoc=1&_issn=00963003&md5=574fcf83bdfe335998475550c9ca9da8" title="Click to view the MathML source">θ0∈L2(R2)class="mathContainer hidden">class="mathCode">θ0L2(R2). Let θ   and class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0096300316305069&_mathId=si2.gif&_user=111111111&_pii=S0096300316305069&_rdoc=1&_issn=00963003&md5=8138d08e3fa64d0d1cfbd2b662ffd1c0">class="imgLazyJSB inlineImage" height="18" width="13" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0096300316305069-si2.gif">class="mathContainer hidden">class="mathCode">θ˜ be two weak solutions with the same initial value θ0. If θ satisfies the energy inequality and if
class="formula" id="ueq0001">
where class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0096300316305069&_mathId=si4.gif&_user=111111111&_pii=S0096300316305069&_rdoc=1&_issn=00963003&md5=8fccb2dfb34549ba34236fa1d434a2e1">class="imgLazyJSB inlineImage" height="25" width="79" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0096300316305069-si4.gif">class="mathContainer hidden">class="mathCode">M.p,q(R2) denotes the homogeneous Morrey–Campanato space, then we have class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0096300316305069&_mathId=si5.gif&_user=111111111&_pii=S0096300316305069&_rdoc=1&_issn=00963003&md5=80ff903a36e47a957c4560d3dafeca7d">class="imgLazyJSB inlineImage" height="18" width="49" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0096300316305069-si5.gif">class="mathContainer hidden">class="mathCode">θ=θ˜. Due to the embedding relation class="mathmlsrc">title="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0096300316305069&_mathId=si6.gif&_user=111111111&_pii=S0096300316305069&_rdoc=1&_issn=00963003&md5=483c425b37dcbad7162f0e43f9851a2b">class="imgLazyJSB inlineImage" height="25" width="162" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0096300316305069-si6.gif">class="mathContainer hidden">class="mathCode">Lp(R2)M.p,q(R2) with 1 < p < q < ∞, we see that our result is an improvement of the corresponding result given by Zhao and Liu (2013).

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