Abstract A phenomenological theory of improper ferroelastic Phase Transition, that superionic hydrogen‐bonded Rb 3 H(SeO 4 ) 2 , crystals undergo at T c = 447 K, is presented. The temperature dependences of components of the spontaneous deformation tensor, elastic coefficient tensor, and electric conductivity in the vicinity of phase transition are calculated. A possible microscopic model of order–disorder type of the phase transition in the proton subsystem is discussed briefly.
M. PołomskaB. HilczerJ. WolakA. Pietraszko
Saburo YokotaYasuharu MakitaYutaka Takagi
Toshiki KishimotoToshio ÔsakaM. KomukaeYasuharu Makita
Ae Ran LimShin Gyoon HamJin‐Hae ChangM. Ichikawa