Given an almost complex structure J in a cylinder of \documentclass[12pt]{minimal}
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\begin{document}$\mathbb{R}^{2p}$\end{document} (p > 1) together with a compatible symplectic form \documentclass[12pt]{minimal}
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\begin{document}$\omega$\end{document} and given an arbitrary J-holomorphic curve \documentclass[12pt]{minimal}
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\begin{document}$\Sigma $\end{document} without boundary in that cylinder, we construct an holomorphic perturbation of \documentclass[12pt]{minimal}
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\begin{document}$\Sigma $\end{document}, for the canonical complex structure J0 of \documentclass[12pt]{minimal}
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\begin{document}$\mathbb{R}^{2p}$\end{document}, such that the distance between these two curves in W1,2 and \documentclass[12pt]{minimal}
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\begin{document}$L^\infty$\end{document} norms, in a sub-cylinder, are controled by quantities depending on J, \documentclass[12pt]{minimal}
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\begin{document}$\omega$\end{document} and by the area of \documentclass[12pt]{minimal}
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\begin{document}$\Sigma $\end{document} only. These estimates depend neither on the topology nor on the conformal class of \documentclass[12pt]{minimal}
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\begin{document}$\Sigma $\end{document}. They are key tools in the recent proof of the regularity of 1-1 integral currents in [RT].