Pottasium iodate, KIO 3 , belongs to the perovskite structure and undergoes successive phase transitions at T 1 = 212 • C, T 2 = 72.5 • C, T 3 = −15 • C, T 4 = −160 • C and T 5 = −240 • C, respectively. The temperature dependences of the dielectric, elastic and piezoelectic properties have been measured in the temperature range from −263 • C to 330 • C. The superionic conductivity was found in the temperature range above T 2 . Pronounced dielectric dispersions in the frequency range below 10 kHz were observed around −160 • C and −240 • C and the data were analyzed by fitting to the Davidson-Cole and Havriliak-Negami dispersion formulas, respectively. Both dielectric anomalies are ascribed to the taional glass-transitions. The piezoelectric and elastic properties have been investigsated by the resonance-antiresonance method. The piezoelectric and elastic anomalies were observed at T 2 and T 3 .Pottasium iodate, KIO 3 , is one of the most facinating member of the perovskite family owing to its non-linerar optical properites. 1) It undergoes successive phase transitions at T 1 = 212 • C, T 2 = 72.5 • C, T 3 = −15 • C and T 4 = −160 • C and T 5 = −240 • C, respectively, and is ferroelectric in all phases below 212 • C. 2) The phases are denoted here I, II, III, IV, V and VI-phases in decending order of the temperature.It has been reported that the space group in each phase is R3m(C 5 3v ) (T > T 1 ), Cm(Cs 3 ) (T 1 > T > T 2 ), and P1(C 1 1 ) (T 2 > T > T 3 ), respectively.3) The results of structural studies on KIO 3 until 1971 were summarized by Crane. 4) The structural details of the I-, II-and III-phases and their relation to the cubic prototype were discussed by Hamid. 2) The structural changes induced by the transitions at T 3 = −15 • C, T 4 = −160 • C and T 5 = −240 • C are not yet known. The phase transition at T 5 was found in the present investigastion. The phase transition at 130 • C reported by several authors is still questionable. 4)Investigations on the physical properties such as dielectric, 2, 5) elelctro-optical, 6, 7) piezoelectric properties, 6, 7) NQR 2) and Raman scatterng experiments 8, 9) of KIO 3 have been reported. Although much data have been reported especially on the temperature dependences of dielectric constants, still there has been some discrepancies between them. The ferroelectric properties of KIO 3 crystals at the successive phase transitions have been investigated in detail by Herlach 2) and Helg, 5) however, the behavior of KIO 3 has not been fully understood. Systematic measurements on the physical properties of KIO 3 have been required to understand the origin of the as 267 successive phase trnsitions.In this paper, dielectric, elastic and piezoelectric measurements have been performed in the temperature range between −263 • C and 330 • C and the mechanism of the successive phase transition has been investigated. §2. ExperimentalThe KIO 3 single crystals used in our experiment were grown from the aqueous solution containg KIO 3 and HIO 3 by the temperature lowering method. 10, ...