Chemistry Reference
In-Depth Information
Fig. 9.11 (a) Temperature dependence of the electrical conductivity of a single-crystal
[Pt
2
(MeCS
2
)
4
I]
1
(1) parallel to the chain axis
b
[
31
]. (b) Temperature dependence of the electrical
resistivity of a single-crystal of 1 parallel to the chain axis
b
type phase transition concerning conformation change of the two PtS
4
planes has
been observed at 365-375 K. The HT disordered phase is also metallic.
9.2.5.2
[Pt
2
(EtCS
2
)
4
I]
1
(2)
The room temperature electrical conductivity of [Pt
2
(EtCS
2
)
4
I]
1
(2)is5-30Scm
1
,
which is of the same order as that reported for 1 [
32
]. The temperature dependence of
electrical resistivity of crystal 2 along the 1D chain is represented in Fig.
9.12a
.On
decreasing temperature, the electrical resistivity increases and reaches a maximum
around 235 K and then decreases down to a minimum at 205 K. Below 205 K, the
electrical resistivity behaves as a semiconductor with an activated energy of
110 meV. To confirm whether the electrical conducting behavior is metallic or not,
the thermoelectric power
S
has been measured (Fig.
9.12b
). Above room temperature,
the
S
takes the temperature-independent small negative value,
VK
1
. Upon
cooling, the
S
slightly increases and shows a slight swelling around 260-205 K and
then changes its sign and increases rapidly. If the MMX units form a metallic band, it
is an effective half-filled band mainly composed of a Pt-Pt d
15
m
*-I pz combination
since the present compound has formally an unpaired electron per an MMX unit. For
the tight-binding approximation, the thermoelectric power of the half-filled band
(
s
1) would give the temperature-independent value, zero [
62
-
64
]. The observed
temperature-independent behavior of
S
above room temperature is consistent with the
r ΒΌ
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