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Via a new inequality à la Gagliardo–Nirenberg, we prove the existence and nonexistence of solutions to \begin{equation*} \begin{cases} (-Δ)^s u + \fracμ{|y|^{2s}} u + λu = f(u), \quad ^N \ni x = (y,z) \in ^K \times ^{N-K}, \ \int_{^N} u^2 , x = ρ\end{cases} \end{equation*} in the mass-critical and mass-subcritical regimes, where , , belongs to a specific range, is given a priori, and is unknown. Additionally, we obtain similar results for the problem above with and as well as a related curl-curl equation. Finally, we provide a thorough insight into the threshold for that divides the scenarios of negative and zero least energy.

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