S. Nagata et al., METAL-INSULATOR-TRANSITION IN THE SPINEL-TYPE CUIR2(S1-XSEX)(4) SYSTEM, Physical review. B, Condensed matter, 58(11), 1998, pp. 6844-6854
The thiospinel CuIr2S4 exhibits a temperature-induced metal-insulator
(M-l) transition around 226 K, showing hysteresis on heating and cooli
ng, that manifests itself as a gap in the electronic density of state
with increasing electrical resistivity at low temperatures. Conversely
, CuIr2Se4 remains metallic down to 0.5 K. We have successfully synthe
sized the spinel-type compound CuIr2(S1-xSex)(4) system. In order to s
ee the effect of substitutions of Se at the S sites, we have carried o
ut a systematic experimental study of structural, electrical, and magn
etic properties of CuIr2(S1-xSex)(4). Mossbauer spectroscopy measureme
nts of Ir-193 have been performed for CuIr2S4 and CuIr2Se4. The M-I tr
ansition of CuIr2(S1-xSex)(4) for x less than or equal to 0.15 is acco
mpanied by a structural transformation from tetragonal (low-temperatur
e insulating phase) to cubic (high-temperature metallic phase) symmetr
y. With increasing Se concentration x, the sharp M-l transition shifts
to lower temperature. The resistivity shows a monotonous increase wit
h decreasing temperature for 0.17 less than or equal to x less than or
equal to 0.78 between 4.2 and 300 K, and the metallic state is recove
red for x greater than or equal to 0.80. Magnetic susceptibility measu
rements show the jump at the M-I transition temperature with hysteresi
s on heating and cooling. The high-temperature metallic phase of CuIr2
S4 shows Pauli paramagnetism, having a density of states at the Fermi
level, D(epsilon(F))= 0.67 states/eV atom. The insulating phase at low
temperatures exhibits diamagnetism, and there is no localized magneti
c moment. The Arrhenius regime is observed for the conductivity with a
thermally activated process for 0 less than or equal to x less than o
r equal to 0.70 in the insulating phase. There is a general trend towa
rd increasing metallicity with increasing x, which is consistent with
the magnetic susceptibility results. A possibility of a two-site model
of different valence states for Ir ions in the insulating phase of Cu
Ir2S4 will be discussed on the basis of the Mossbauer data. A phase di
agram of temperature versus Se concentration x will be proposed for th
e CuIr2(S1-xSex)(4) system. The mechanism of the M-l transition remain
s enigmatic and is far from a complete picture.