We build spaces of q.p. (quasi-periodic) functions and we establish some of
their properties. They are motivated by the Percival approach to q.p. solu
tions of Hamiltonian systems. The periodic solutions of an adequate partial
differential equation are related to the q.p. solutions of an ordinary dif
ferential equation. We use this approach to obtain some regularization theo
rems of weak q.p. solutions of differential equations. For a large class of
differential equations, the first theorem gives a result of density: a par
ticular form of perturbated equations have strong solutions. The second the
orem gives a condition which ensures that any essentially bounded weak solu
tion is a strong one.