On the first eigenvalue of the generalized laplacian
Julian Fernandez Bonder, Ariel Salort
Abstract
In this work we investigate the energy of minimizers of Rayleigh-type quotients of the form $$ \frac{\int_ΩA(|\nabla u|)\, dx}{\int_ΩA(|u|)\, dx}. $$ These minimizers are eigenfunctions of the generalized laplacian defined as $Δ_a u = \text{div}\left(a(|\nabla u|)\frac{\nabla u}{|\nabla u|}\right)$ where $a(t)=A'(t)$ and the Rayleigh quotient is comparable to the associated eigenvalue. On the function $A$ we only assume that it is a Young function but no $Δ_2$ condition is imposed. Since the problem is not homogeneous, the energy of minimizers is known to strongly depend on the normalization parameter $α=\int_ΩA(|u|)\, dx$. In this work we precisely analyze this dependence and show differentiability of the energy with respect to $α$ and, moreover, the limits as $α\to 0$ and $α\to \infty$ of the Rayleigh quotient. The nonlocal version of this problem is also analyzed.
