In this paper, we consider a model problem arising from a classical planar Heisenberg ferromagnetic spin chain: −Δu+V(x)u−u1−u2Δ1−u2=c|u|p−2u,x∈RN,\documentclass[12pt]{minimal}
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\begin{document}$$ -\Delta u+V(x)u-\frac{u}{\sqrt{1-u^{2}}}\Delta \sqrt{1-u^{2}}=c \vert u \vert ^{p-2}u,\quad x\in \mathbb{R}^{N}, $$\end{document} where 2<p<2∗\documentclass[12pt]{minimal}
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\begin{document}$2< p<2^{*}$\end{document}, c>0\documentclass[12pt]{minimal}
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\begin{document}$c>0$\end{document} and N≥3\documentclass[12pt]{minimal}
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\begin{document}$N\geq 3$\end{document}. By the cutoff technique, the change of variables and the L∞\documentclass[12pt]{minimal}
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\begin{document}$L^{\infty}$\end{document} estimate, we prove that there exists c0>0\documentclass[12pt]{minimal}
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\begin{document}$c_{0}>0$\end{document}, such that for any c>c0\documentclass[12pt]{minimal}
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\begin{document}$c>c_{0}$\end{document} this problem admits a positive solution. Here, in contrast to the Morse iteration method, we construct the L∞\documentclass[12pt]{minimal}
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\begin{document}$L^{\infty}$\end{document} estimate of the solution. In particular, we give the specific expression of c0\documentclass[12pt]{minimal}
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\begin{document}$c_{0}$\end{document}.