Composite copper chalcogenide halides: Neutron powder diffraction of CuClCu2TeS3 and electrical properties of CuClCu2TeS3, (CuI)(2)Cu3SbS3, and (CuI)(3)Cu2TeS3
A. Pfitzner et al., Composite copper chalcogenide halides: Neutron powder diffraction of CuClCu2TeS3 and electrical properties of CuClCu2TeS3, (CuI)(2)Cu3SbS3, and (CuI)(3)Cu2TeS3, J SOL ST CH, 147(1), 1999, pp. 170-176
The crystal structure of CuClCu2TeS3 was refined from TOF neutron powder di
ffraction data in order to verify the distribution of chlorine and sulfur,
It is a novel derivative of the zincblende type with an ordered distributio
n both of the cations Cu+ and Te4+ and of the anions Cl- and S2-, The compo
und crystallizes in the rhombohedral system, space group R3m (No. 160) with
a=7.3502(1) Angstrom, c=10.3873(2) Angstrom, V= 485.99 and Z= 3. The struc
ture refinement converged to R-wp=0.039 and R-Bragg = 0.032, From the neutr
on data it can be derived that there is no significant disorder of Cl- and
S atoms, Impedance spectroscopic measurements in the temperature range 140-
280 degrees C reveal that CuClCu2TeS3 is a semiconductor with an activation
energy of 0.75 eV (T< 200 degrees C) and 1.25 eV (Tr 200 degrees C), respe
ctively. On the other hand (CuI)(3)Cu2TeS3 and (CuI)(2)Cu3SbS3 exhibit high
copper ion conductivity with activation energies of 0.2 and 0.35 eV, respe
ctively, but a negligible electronic conduction. (C) 1999 Academic Press.