We prove a localization theorem for continuous ergodic Schrödinger operators Hω := H 0 +Vω, where the random potential Vω is a nonnegative Anderson-type perturbation of the periodic operator H 0 . We consider a lower spectral band edge of σ(H 0 ), say E = 0, at a gap which is preserved by the perturbation Vω. Assuming that all Floquet eigenvalues of H 0 , which reach the spectral edge 0 as a minimum, have there a positive definite Hessian, we conclude that there exists an interval I containing 0 such that Hω has only pure point spectrum in I for almost all ω.Since 0 is in the support of the density of ω 0 it follows that 0 ∈ σ(H ω ). In this case we say that 0 is a lower band edge of the periodic operator, which is preserved by the positive random perturbation V ω .