Mw. Barsoum et al., Electrical conductivity, thermopower, and hall effect of Ti(3)AIC(2), Ti(4)AIN(3), and Ti3SiC2, PHYS REV B, 62(15), 2000, pp. 10194-10198
In this paper we report on the thermopower and electrical conductivities of
Ti4AlN2.9 and Ti3Al1.1C1.8 in the 300-850 K temperature range. We also mea
sured the room temperature Hall effect in Ti3SiC2 Ti4AlN2.9, and Ti3Al1.1C1
.8. Based on these results we conclude that holes are the majority carriers
at room temperature in Ti3Al1.1C1.8 and Ti4AlN2.9. At higher temperatures
free electrons contribute to the transport properties. Ti3SiC2 is a mixed c
onductor wherein the concentrations and mobilities of the free electrons ar
e, respectively, equal to those of the holes over an extended temperature r
ange. The high conductivity of Ti3SiC2 is due to the presence of a large co
ncentration of charge carriers. The lower conductivity of Ti3Al1.1C1.8 is d
ue to a dearth of charge carriers. The even lower conductivity of Ti4AlN2.9
is attributed to a reduced mobility, most probably due to vacancy scatteri
ng of the charge carriers.