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[Pt 2 (RCS 2 ) 4 ](R
Me, Et, n -Pr, n -Bu, n -Pen) can be stored without decomposition
for several months under an inert atmosphere in a freezer but gradually decompose
upon exposure to air.
The precursor complex [Pt 2 II (MeCS 2 ) 4 ] readily undergoes oxidative addition
with halogens in hot toluene, giving [Pt 2 III (MeCS 2 ) 4 X 2 ] containing platinum
atoms with formal oxidation state of
¼
þ
¼
3[ 28 ]. In the case of X
I, if the reaction
¼
is carried out with a ratio of [Pt 2 (MeCS 2 ) 4 ]:I
1:1, an MMX-chain compound
[Pt 2 (MeCS 2 ) 4 I] 1 (1) with formal oxidation state of
2.5 is isolated. This compound
can also be obtained from the reaction of [Pt 2 II (MeCS 2 ) 4 ] and [Pt 2 III (MeCS 2 ) 4 I 2 ]in
toluene under reflux [ 28 ]. As described in the next section, [Pt 2 (MeCS 2 ) 4 I] 1 (1)
undergoes an order-disorder type phase transition associated with the conformation
of two PtS 4 planes around 371-372 K [ 46 ]. One should be careful because the
disordered diplatinum unit of 1 will be partially formed in the crystal when the
crystals start to deposit above the transition temperature. [Pt 2 (RCS 2 ) 4 I] 1 (R
þ
Et (2),
n -Pr (3), n -Bu (4), and n -Pen (5)) can also be prepared by mixing equimolar
amounts of [Pt 2 II (RCS 2 ) 4 ] and [Pt 2 III (RCS 2 ) 4 I 2 ][ 32 - 35 ]. [Pt 2 ( n -BuCS 2 ) 4 I] 1 (4)
and [Pt 2 ( n -PenCS 2 ) 4 I] 1 (5) are prepared by cooling the corresponding toluene—
n -hexane or n -hexane solution down to 2 ~ 0 C, because the solubility of the MMX
compounds increases with elongation of the alkyl chains. These MMX-chain
compounds are relatively stable in air.
¼
9.2.2 Crystal Structures
Before describing the crystal structures, the transition temperature and the entropy
gain at the phase transition obtained by the heat capacity measurements of
[Pt 2 (RCS 2 ) 4 I] 1 (Me (1), Et (2), n -Pr (3), n -Bu (4), and n -Pen (5)) are listed in
Table 9.1 [ 47 - 52 ].
9.2.2.1
[Pt 2 (RCS 2 ) 4 I] 1 (R ¼ Me (1), Et (2))
Miyazaki et al. have reported the heat capacity of [Pt 2 (MeCS 2 ) 4 I] 1 (1) in which a
distinct heat capacity peak due to a phase transition was observed at T trs ¼
373.4 K,
indicating the presence of the room temperature (RT) and high-temperature (HT)
phases [ 48 ]. On the other hand, DSC measurements of [Pt 2 (EtCS 2 ) 4 I] 1 (2) do not
show any latent heat in the temperature range of 150-473 K [ 32 ]. [Pt 2 (RCS 2 ) 4 I] 1
(R
Me (1), Et (2)) crystallize in the same monoclinic space group C 2/ c and hence
have similar structures [ 28 , 32 ]. The crystal structure of 2 is shown in Fig. 9.2 .
The crystals of both compounds consist of neutral 1D chains with a repeating
-Pt-Pt-I- unit lying on the crystallographic twofold axis parallel to the b axis.
The crystal structure is exemplified with that of the compound 2 [ 32 ]. Two platinum
atoms of 2 are bridged by four dithiopropanato ligands with a Pt-Pt distance of
2.684 (1) ˚
¼
at 293 K, 0.189 ˚
shorter than the distance between the mean planes
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