Electronic Journal of Differential Equations, Vol. 2004(2004), No. 76, pp. 1-32. Title: Variational methods for a resonant problem with the p-Laplacian in $\mathbb{R}^N$ Authors: Benedicte Alziary (Univ. Toulouse 1, France) Jacqueline Fleckinger (Univ. Toulouse 1, France) Peter Takac (Univ. Rostock, Germany) Abstract: The solvability of the resonant Cauchy problem $$ - \Delta_p u = \lambda_1 m(|x|) |u|^{p-2} u + f(x) \quad\hbox{in } \mathbb{R}^N ;\quad u\in D^{1,p}(\mathbb{R}^N), $$ in the entire Euclidean space $\mathbb{R}^N$ ($N\geq 1$) is investigated as a part of the Fredholm alternative at the first (smallest) eigenvalue $\lambda_1$ of the positive $p$-Laplacian $-\Delta_p$ on $D^{1,p}(\mathbb{R}^N)$ relative to the weight $m(|x|)$. Here, $\Delta_p$ stands for the $p$-Laplacian, $m\colon \mathbb{R}_+\to \mathbb{R}_+$ is a weight function assumed to be radially symmetric, $m\not\equiv 0$ in $\mathbb{R}_+$, and $f\colon \mathbb{R}^N\to \mathbb{R}$ is a given function satisfying a suitable integrability condition. The weight $m(r)$ is assumed to be bounded and to decay fast enough as $r\to +\infty$. Let $\varphi_1$ denote the (positive) eigenfunction associated with the (simple) eigenvalue $\lambda_1$ of $-\Delta_p$. If $\int_{\mathbb{R}^N} f\varphi_1 \,{\rm d}x =0$, we show that problem has at least one solution $u$ in the completion $D^{1,p}(\mathbb{R}^N)$ of $C_{\mathrm{c}}^1(\mathbb{R}^N)$ endowed with the norm $(\int_{\mathbb{R}^N} |\nabla u|^p \,{\rm d}x)^{1/p}$. To establish this existence result, we employ a saddle point method if $1 < p < 2$, and an improved Poincar\'e inequality if $2\leq p< N$. We use weighted Lebesgue and Sobolev spaces with weights depending on $\varphi_1$. The asymptotic behavior of $\varphi_1(x)= \varphi_1(|x|)$ as $|x|\to \infty$ plays a crucial role. \end{abstract} Submitted March 19, 2004. Published May 26, 2004. Math Subject Classifications: 35P30, 35J20, 47J10, 47J30 Key Words: p-Laplacian; degenerate quasilinear Cauchy problem; Fredholm alternative; (p-1)-homogeneous problem at resonance; saddle point geometry; improved Poincare inequality; second-order Taylor formula.