We consider the focusing inhomogeneous biharmonic nonlinear Schrödinger equation in H2(RN)\documentclass[12pt]{minimal}
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\begin{document}$$H^2(\mathbb {R}^N)$$\end{document}, iut+Δ2u-|x|-b|u|αu=0,\documentclass[12pt]{minimal}
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\begin{document}$$\begin{aligned} iu_t + \Delta ^2 u - |x|^{-b}|u|^{\alpha }u=0, \end{aligned}$$\end{document}when b>0\documentclass[12pt]{minimal}
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\begin{document}$$b > 0$$\end{document} and N≥5\documentclass[12pt]{minimal}
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\begin{document}$$N \ge 5$$\end{document}. We first obtain a small data global result in H2\documentclass[12pt]{minimal}
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\begin{document}$$H^2$$\end{document}, which, in the five-dimensional case, improves a previous result from Pastor and the second author. In the sequel, we show the main result, scattering below the mass-energy threshold in the intercritical case, that is, 8-2bN<α<8-2bN-4\documentclass[12pt]{minimal}
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\begin{document}$$\frac{8-2b}{N}< \alpha <\frac{8-2b}{N-4}$$\end{document}, without assuming radiality of the initial data. The proof combines the decay of the nonlinearity with Virial-Morawetz-type estimates to avoid the radial assumption, allowing for a much simpler proof than the Kenig-Merle roadmap.