“…As far as we know, in all other relevant results related to our inverse problem, that can be found for instance in the articles [9,12,21,28,30], the determination of the quasilinear term a has been considered from Neumann boundary measurements restricted to an open subset of ∂Ω associated with Dirichlet excitations lying in an infinite dimensional space. In Theorem 2.1 and 2.2, we improve these results by restricting the Dirichlet excitations to the space of affine functions of R n taking values in R, which is a space of dimension n + 1, and we consider Neumann measurements restricted to at most n points for the determination of general quasilinear terms depending simultaneously on the solutions and the gradient of the solutions of (1.3).…”