By including the contribution of a bound electron to the potential to be screened, it is shown that the screening cloud around a Coulomb charge is repelled so as to enable the formation of a persistent localized state. This result is obtained either with Thomas-Fermi or Lindhard screening, and is applied to the determination of Mott's critical density.Introduction. -The bound states induced by a test charge screened by an electron gas have already been the subject of numerous papers. Their determination was primarily of interest in the study of the Metal-Insulator Transition (MIT) (see, e.g., [1][2][3][4]). Screened potentials are also known for exhibiting specific features such as Friedel oscillations, either in three-dimensional [5] or two-dimensional systems [6]. More recently, some authors also investigated the possibility of occurrence of a bound state in the attractive part of such oscillating potentials, either attractive or repulsive [7]. In all the cases I am aware of, an important property of such bound systems seems to have remained unnoticed: In contrast to the stationary states induced by an unscreened potential, as, for instance, with a hydrogen atom in vacuum or an impurity in a low-doped semiconductor, the potential felt by the trapped electron is not the same as the one which exists in the absence of such an electron. In other words, the screening of the test charge is also a function of the potential induced by the wave function of the bound particle. That the localized electron tends to repel the screening cloud should indeed be a trivial remark. But I wish to show that this may have major consequences, since this implies that the binding energy is not the same, depending on whether an electron was present or not in the site before switching on electron screening. Indeed, we shall see that even when the increase in electron density is such that there is no longer an empty state, the binding energy of the occupied state never vanishes. For the sake of clarity (and brevity), in this letter, I only intend to provide the simplest comprehensive example of such a phenomenon, in a three-dimensional system. I have therefore chosen to treat the case of an occupied bound state with a positive test charge, the screening of which is accounted for by introducing either the Lindhard or the Thomas-Fermi