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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=182709"><dc:title>High and low perturbations of the critical Choquard equation on the Heisenberg group</dc:title><dc:creator>Bai,	Shujie	(Avtor)
	</dc:creator><dc:creator>Repovš,	Dušan	(Avtor)
	</dc:creator><dc:creator>Song,	Yueqiang	(Avtor)
	</dc:creator><dc:subject>perturbations</dc:subject><dc:subject>critical Choquard equation</dc:subject><dc:subject>Heisenberg group</dc:subject><dc:description>We study the following critical Choquard equation on the Heisenberg group: $\begin{cases} {-\Delta_H u }={\mu} |u|^{q-2}u+\int_{\Omega} \frac{|u(\eta)|^{Q_{\lambda}^{\ast}}} {|\eta^{-1}\xi|^{\lambda}} d\eta|u|^{Q_{\lambda}^{\ast}-2}u &amp; \mbox{in}\ \Omega, \\ u=0 &amp; \mbox{on}\ \partial\Omega, \end{cases}$ where $\Omega\subset \mathbb{H}^N$ is a smooth bounded domain, $\Delta_H$ is the Kohn-Laplacian on the Heisenberg group $\mathbb{H}^N$, $1 &lt; q &lt; 2$ or $2 &lt; q &lt; Q_\lambda^\ast$, $\mu &gt; 0$, $0 &lt; \lambda &lt; Q=2N+2$, and $Q_{\lambda}^{\ast}=\frac{2Q-\lambda}{Q-2}$ is the critical exponent. Using the concentration compactness principle and the critical point theory, we prove that the above problem has the least two positive solutions for $1 &lt; q &lt; $ in the case of low perturbations (small values of $\mu$), and has a nontrivial solution for $2 &lt; q &lt; Q_\lambda^\ast$ in the case of high perturbations (large values of $\mu$). Moreover, for $1 &lt; q &lt; 2$, we also show that there is a positive ground state solution, and for $2 &lt; q &lt; Q_\lambda^\ast$, there are at least $n$ pairs of nontrivial weak solutions.</dc:description><dc:date>2024</dc:date><dc:date>2026-05-21 10:03:32</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>182709</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
