Bis[(μ-iodo)iodo-η-cyclopentadienylruthenium(III)]
as the above binuclear form in its trans-configuration [13],
˚
Cr···Cr distances of 3.362(1) (295 K), 3.3447(8) A (203 K)
consistent with the presence of only limited metal···metal
bonding (cf. the aluminium and titanium analogues, Table
2). In the other example, the recently reported ru-
thenium(III)/chloride complex, the pairs of chloride and Cp
ligands lie cis with respect to the RuCl2Ru core which, here,
is disposed about a crystallographic 2-axis, rather than an
˚
inversion centre. Ru···Ru (2.7748(6) A) is much shorter than
Cr···Cr, despite M-Cl (bridging, x 2) which are very similar
˚
(2.3713(8), 2.3754(8) (M ϭ Cr); 2.3591(8), 2.3788(8) A
(M ϭ Ru). The M-Cl (terminal) distances differ appreci-
˚
ably: 2.2780(7), 2.3851(8) A, suggestive of much stronger
metal-metal bonding within the ruthenium complex, poss-
ibly the origin of and/or facilitated by the considerable
‘folding’ feature of the RuCl2Ru array across the Cl···Cl
line, a feature not possible if the dimer is truly centrosym-
metric as in many of the trans complexes and where the
formation of the cis form may be hindered by the Cp sub-
stituents.
The results of the present single crystal X-ray study are
fully consistent with the description of the present complex
as [CpIRu(μ-I)2RuICp], (Fig. 1), the structure being iso-
typic with the recently described chloride counterpart with
which its dimensions are compared in Table 1. The Ru···Ru
bond is somewhat longer in the iodide complex, consistent
with the presence of the much larger halogen atoms. The
latter perhaps dictate the decrease in ‘fold’ angle across the
the X···X line, concomitant with a distortion comprising a
twist about the intramolecular 2-axis and encompassing the
development of a differential between the Ru-I distances,
the bridging ones becoming shorter and one longer (mean
˚
˚
2.77 A), cf. the Ru-I (terminal) distance of 2.735(1) A (per-
haps a useful datum, since all three Ru-Cl distances in the
˚
chloride counterpart lie within a range of 0.026 A), with the
further constraint that the inner hydrogen atoms of the pair
˚
of Cp ligands contact (est. 2.3 A) within their van der Waals
sum. The molecules pack in sheets about z ϭ 0.25, 0.75 of
opposed polarity, as shown in Fig. 1(b).
Acknowledgement. We thank the ARC for support of this work and
Johnson Matthey plc, Reading, UK, for a generous loan of
RuCl3 ·nH2O.
Fig. 1 (a) Molecular projection of [CpIRu(μ-I)2RuICp]; the
crystallographic 2-axis lies quasi-vertical in the page. (b) Unit cell
contents projected down a.
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