Ion dynamics in alkali borohydrides, LiBH 4 , NaBH 4 , and KBH 4 , was studied by solid-state NMR. NMR spectra and spin−lattice relaxation times, T 1 , of 1 H and 11 B were measured and analyzed. The T 1 results of 1 H and 11 B indicated that two types of motions take place in the lowtemperature (LT) phase of LiBH 4 . The second moments of 1 H and 11 B NMR spectra suggested that the sum of the two types of motions resembles isotropic reorientation of the BH 4 unit. The T 1 minimum values of 1 H and 11 B supported that the C 3 rotation takes place at first. The second type of motion might be either C 3 rotation or C 2 rotation. The second moments of NMR spectra and the T 1 minimum values of 1 H and 11 B supported that the BH 4 unit reorients isotropically in NaBH 4 and KBH 4 .
INTRODUCTIONBorohydrides, alanates, and amides of alkali and alkaline-earth metals have recently received much attention due to their potentials as hydrogen storage materials and energy carriers for fuel cells. 1,2 Alkali borohydrides MBH 4 consist of alkali cations M + and tetrahedral [BH 4 ] − anions. The crystal structures and dynamics of the ions have been studied for a long time by means of various techniques: X-ray and neutron diffractions, 3−9 neutron scattering, 5,7,10−13 Raman spectroscopy, 4,14,15 nuclear magnetic resonance (NMR), 8,16−29 and theoretical calculations. 7,10,13,30,31 Among the various techniques, NMR is suitable to study ion dynamics. The tetrahedral BH 4 unit reorients very fast in the room-temperature phase of MBH 4 (M = Li, Na, K, Rb, and Cs). 8,[16][17][18][19][20][21][22]24,25,28,29 A slow hopping motion of lithium ion was suggested in the low-temperature (LT) phase of LiBH 4 . 25 Lithium ion diffuses very fast in the high-temperature (HT) phase of LiBH 4 . 23,25,27 Both hydrogen and boron atoms diffuse in the HT phase of LiBH 4 , 25 although a Raman study proposed diffusion of single hydrogen atoms. 15 No H exchange was observed between BH 4 units in molten LiBH 4 . 26 In solid LiBH 4 , intact BH 4 units diffuse instead of hydrogen atoms. 26,27 The spin−lattice relaxation time, T 1 , of nuclear spins can sensitively probe a motion with a rate of the order of Larmor frequency. BH 4 reorientation has frequently been studied by means of T 1 . The plot of T 1 as a function of inverse temperature (1/T) shows a V-shaped curve when the relaxation mechanism is originated from a single mode of motion. Analysis of the temperature dependence of T 1 produces the rate and the mode of motions. The rate of BH 4 reorientation was almost established for MBH 4 (M = Li, Na, K, Rb, and Cs). 8,24,28,29 The minimum values of T 1 as well as the line shapes are closely related with the crystal structure and the