TY - JOUR
T1 - Li self-diffusion in garnet-type Li7La3Zr 2O12 as probed directly by diffusion-induced Li7 spin-lattice relaxation NMR spectroscopy
AU - Kuhn, A.
AU - Narayanan, S.
AU - Spencer, L.
AU - Goward, G.
AU - Thangadurai, V.
AU - Wilkening, M.
PY - 2011/3/15
Y1 - 2011/3/15
N2 - Li self-diffusion in garnet-type Li7La3Zr 2O12, crystallizing with tetragonal symmetry at room temperature, is measured by temperature-variable Li7 spin-spin as well as spin-lattice relaxation (SLR) nuclear magnetic resonance (NMR) spectroscopy. The SLR NMR rates which were recorded in both the laboratory and the rotating frame of reference pass through characteristic diffusion-induced rate peaks allowing for the direct determination of Li jump rates τ-1, which can be directly converted into self-diffusion coefficients Dsd. The NMR results are compared with those obtained from electrical impedance spectroscopy measurements carried out in a large temperature and wide frequency range. Taken together, the long-range diffusion process, being mainly responsible for ionic conduction at ambient temperature, is characterized by an activation energy of approximately 0.5 eV, with τ0-1×1014 s-1 being the pre-exponential factor of the underlying Arrhenius relation.
AB - Li self-diffusion in garnet-type Li7La3Zr 2O12, crystallizing with tetragonal symmetry at room temperature, is measured by temperature-variable Li7 spin-spin as well as spin-lattice relaxation (SLR) nuclear magnetic resonance (NMR) spectroscopy. The SLR NMR rates which were recorded in both the laboratory and the rotating frame of reference pass through characteristic diffusion-induced rate peaks allowing for the direct determination of Li jump rates τ-1, which can be directly converted into self-diffusion coefficients Dsd. The NMR results are compared with those obtained from electrical impedance spectroscopy measurements carried out in a large temperature and wide frequency range. Taken together, the long-range diffusion process, being mainly responsible for ionic conduction at ambient temperature, is characterized by an activation energy of approximately 0.5 eV, with τ0-1×1014 s-1 being the pre-exponential factor of the underlying Arrhenius relation.
U2 - 10.1103/PhysRevB.83.094302
DO - 10.1103/PhysRevB.83.094302
M3 - Article
AN - SCOPUS:79960982820
SN - 1098-0121
VL - 83
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 9
M1 - 094302
ER -