TY - JOUR
T1 - Stoichiometry dependence of the transport properties of TiS2
AU - Klipstein, P. C.
AU - Bagnall, A. G.
AU - Liang, W. Y.
AU - Marseglia, E. A.
AU - Friend, R. H.
PY - 1981
Y1 - 1981
N2 - Transport and Raman data are presented for samples of Ti 1+xS2 with carrier densities, determined from the Hall coefficient, ranging from approximately 1020 cm-3 to approximately 3*1021 cm-3. No dependence on carrier concentration, n, is observed for the frequency of the A1g Raman-active phonon, whereas a strong variation is seen in the non-linear temperature dependence of resistivity, rho (T), between 4.2K and 290K. Fitting the resistivity to a power law, rho (T)- rho (o) varies as Tp, in the range 110K to 290K, the authors find p=2.3 for n approximately 1020 cm-3 and p=1.6 for n approximately *1021 cm -3. For samples with carrier concentrations above approximately 7*1020 cm-3 a stronger temperature dependence is observed below 100K. The temperature-dependent part of the resistivity is proportional to n-0.74 at room temperature and n-0.60 at 150K. It is argued that the scattering mechanism in TiS2 is with both optical and acoustic phonons. Below the Debye temperature the form and variation with carrier concentration of the temperature dependence may be described by a model involving both intra- and inter-valley scattering by acoustic phonons.
AB - Transport and Raman data are presented for samples of Ti 1+xS2 with carrier densities, determined from the Hall coefficient, ranging from approximately 1020 cm-3 to approximately 3*1021 cm-3. No dependence on carrier concentration, n, is observed for the frequency of the A1g Raman-active phonon, whereas a strong variation is seen in the non-linear temperature dependence of resistivity, rho (T), between 4.2K and 290K. Fitting the resistivity to a power law, rho (T)- rho (o) varies as Tp, in the range 110K to 290K, the authors find p=2.3 for n approximately 1020 cm-3 and p=1.6 for n approximately *1021 cm -3. For samples with carrier concentrations above approximately 7*1020 cm-3 a stronger temperature dependence is observed below 100K. The temperature-dependent part of the resistivity is proportional to n-0.74 at room temperature and n-0.60 at 150K. It is argued that the scattering mechanism in TiS2 is with both optical and acoustic phonons. Below the Debye temperature the form and variation with carrier concentration of the temperature dependence may be described by a model involving both intra- and inter-valley scattering by acoustic phonons.
UR - https://www.scopus.com/pages/publications/36149042142
U2 - 10.1088/0022-3719/14/28/009
DO - 10.1088/0022-3719/14/28/009
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AN - SCOPUS:36149042142
SN - 0022-3719
VL - 14
SP - 4067
EP - 4081
JO - Journal of Physics C: Solid State Physics
JF - Journal of Physics C: Solid State Physics
IS - 28
M1 - 009
ER -