In the ferroelectric phase of two KTa1−xNbxO3 (x = 0.022 and x = 0.027) samples, we have measured the variation of the real and imaginary parts of the complex dielectric constant ε just after an isothermal evolution of duration t pl at the temperature T pl (plateau). We have found that the temperature derivative dε dT (T, t pl ) has not the same value for T = T pl +0 and T = T pl − 0 if t pl is not zero; this means that ε(T, t pl ) is not derivable with respect to T . Return to disorder is carefully defined. Its occurrence after a temperature plateau at T pl has been studied for fixed T pl as a function of t pl and of measurement frequency.Introduction. -Aging is a widespread phenomenon. Noticed on the elastic compliance of polymers a long time ago [1], it has also been observed in many solids: on the magnetic susceptibility χ of spin-glasses (SG) [2-5], on the elastic constant c and on the dielectric constant ε of disordered dielectrics [6][7][8]. Aging is said to occur when the evolution is nonstationary and depends on the thermal history; it may lead to ergodicity breaking [7]. This is a consequence of disorder and frustration.Recently, a surprising effect was observed in some materials after isothermal aging at the fixed temperature T pl (or plateau). Aging manifests itself by the decrease of some susceptibility (indeed, its real part and its imaginary part). This evolution tends necessarily towards more stability and thus more order. It may happen that upon cooling at the end of the plateau an immediate increase (generally of the imaginary part) is observed, thus indicating some return to disorder, although temperature is lowered. A memory effect is often associated with return to disorder [9][10][11].Return to disorder was observed in various compounds: in the ferroelectric lock-in phase of Rb 2 ZnCl 4 [12], in the SG phase of CdCr 1.7 In 0.3 S 4 [9] and in Cu:Mn [9, 10] which is a metallic SG, in the two phases (SG and ferromagnetic) of CdCr 1.9 In 0.1 S 4 [13], in the disordered dielectric KTa 1−x Nb x O 3 (KTN) [11] but not in K 1−y Li y TaO 3 (KLT) [14], which is also a disordered dielectric.In this letter, we present a precise definition of return to disorder and we report new dielectric measurements performed just at the end of isothermal aging. They provide quantitative data on two types of results: i) the derivatives of the complex dielectric constant with respect ( * ) Associated with the Centre National de la Recherche Scientifique (UMR 7603).