Triammonium hydrogen diselenate, (NH,),H(SeO,),, undergoes a sequence of successive phase transitions: phase I (trigonal R3m) T,, = 332 K, phase I1 (trigonal R3) T,, = 302 K, phase I11 (triclinic P1) Tc3 = 275 K, phase IV (monoclinic) Tc4 = 181 K, and phase V (monoclinic) [l, 41. In the high temperature phases I and I1 the crystal exhibits a superionic conductivity of protonic type. The low temperature phase V is ferroelectric, whereas ferroelastic properties were found in phase 111. It was suggested that the phase transitions are related to order or disorder of SeOi-or NH: ions but the mechanisms for the transitions are still not recognized. Our interest in this particular system has been stimulated by recent cw and pulse EPR experiments performed in our laboratory. Thc purpose of these investigations is to examine the dynamical properties of NH; groups and to see which role, if any, they play in the phase transitions observed in this material.The spin-lattice relaxation times Tl have been measured with a SXP-4/100 Bruker pulse spcctrometer at 90 MHz within the temperature range 100 to 345 K. The temperatures were stabilized with an accuracy of f l K using a nitrogen gas flow unit and a minimum of 20 min was allowed for a sample to reach temperature equilibrium. The relaxation time T,was measured with the magnetization recovery method n -z -7c/2 on a polycrystalline sample. The time between the pulse sequence (the repetition time) was taken to be eight to ten times Tl. The recovery of magnetization was found to be exponential within the experimental error over the entire temperature range studied. The relaxation times exhibit two discontinuities in their temperature dependences (Fig. 1) at 302 and 275 K, respectively, due to the phase transitions of first-order character, consistent with the crystallographic work [ I , 21. The other two phase transitions in the triammonium hydrogen diselenate at 332 and 181 K, respectively, show a less distinct nature and are not pronounced in TI. I n the temperature region below 200 K we observe well resolved double minima due to two chcmically inequivalent ammonium ions NH: (1) and NH: (2). The ions form hydrogen bonds with the oxygen atoms. The NH: (1) ions appear to form the three stronger hydrogen bonds with Ro-H...o = 0.181, 0.194, and 0.198 nm whereas the N H l ( 2 ) ions are involved in two weaker hydrogen bonds with lengths of 0.255 and 0.211 nm, respectively. There are also differences in the average N-H bond lengths which are 0.100 and 0.078 nm for NH; ( I ) and NH,f (2), respectively. The ratio of the number of NH; (1) ions to N H l (2) in the crystal unit cell is equal to 2: 1.' ) Smoluchowskiego 17, PL-60-179 Poznan, Poland.