R.D. Adams et al. / Journal of Organometallic Chemistry xxx (2014) 1e6
3
3
3
H
¼ 6 Hz, Ph), 8.30 (t, 1H, JH-H ¼ 6 Hz, Ph), 7.11 (t, 1H, JH-H ¼ 6 Hz,
3
Ph), 6.87 (t, 1H, JH-H ¼ 6 Hz, Ph). Mass Spec. EI/MS m/z: 1510.
3 9 3 6 4 3 2 4
Transformation of 2 into [Os (CO) (m -C H )(m-H)(m -Hg)] Os(CO) ,
4
1
4.2 mg (0.0058 mmol) of 2 was dissolved in cyclohexane. The
solution was heated to reflux for 70 min. The solvent was then
removed in vacuo. 1.5 mg (11% yield) of yellow [Os (CO)
)( -H)( -Hg)] Os(CO) , 4 was isolated by TLC on silica gel by
using a hexane/methylene chloride solvent mixture (4/1, v/v).
3
9 3
(m -
C
H
6 4
m
m
3
2
4
ꢀ
1
Spectral data for 4: IR nCO (cm in hexane): 2101(w), 2087(w),
2
080(m), 2070(s), 2052(s), 2024(w), 2017(m), 2012(w), 1996(m),
1
ꢁ
3
1989(m). H NMR (CD
2
Cl
2
, 25 C, TMS, in ppm)
d
¼ 7.93 (d, 1H, JH-
3
3
H
¼ 6 Hz, C
6
H
4
), 7.92 (d, 1H,
), 6.87 (d, 1H, JH-H ¼ 6 Hz, C
JH-H ¼ 6 Hz, C
6
H
4
), 6.88 (d, 1H,
J
H-
3
H
¼ 6 Hz, C
6
H
4
6
H
4
), -21.05 (s, 1H, hy-
dride); Mass Spec. EI/MS m/z: 2504.
Crystallographic analyses
Dark green single crystals of 2 and 3 suitable for X-ray diffrac-
tion analyses were obtained by slow evaporation of the solvent at
room temperature from solutions of the pure compound in hexane
solvent. Orange single crystals of 4 were obtained by slow evapo-
ration of solvent from a solution in hexane solvent at 5 C. The data
crystals were glued onto the end of thin glass fibers. X-ray intensity
Fig. 1. An ORTEP diagram of the molecular structure of [Os
showing 20% thermal ellipsoid probabilities. Hg is orange, I is purple, Os is blue and the
carbon atoms of the phenyl rings are colored red. Selected interatomic bond distances
3
(CO)10HgI(
m
-Ph)]
4
, 2
ꢁ
o
(Å) and angles ( ) are as follow: Os(1)
e
Os(2)
¼
2.8205(6) Å, Os(1) e
Os(3) ¼ 2.8761(6), Os(2) e Os(3) ¼ 2.8748(7), Os(1) e C(1) ¼ 2.309(12), Os(2) e
C(1) ¼ 2.285(12) Å, Os(1) e Hg(1) ¼ 2.7930(6) Å, Os(2) e Hg(1) ¼ 2.7978(7), Hg(1) e
data were measured by using a Bruker SMART APEX CCD-based
i
ii
I(1) ¼ 2.9112(8) Å, Hg(1) e I(1 ) ¼ 2.9645(8), Hg(1) e I(1 ) ¼ 3.524(1); Os(2) e Os(1) e
diffractometer using Mo K
a
radiation (
l
¼ 0.71073 Å). The raw
i
Os(3) ¼ 60.607(16), Os(1) e Hg(1) e Os(2) ¼ 60.596(15), I(1) e Hg(1) e I(1 ) ¼ 87.29(2),
i
data frames were integrated with the SAINTþ program by using a
narrow-frame integration algorithm [9]. Correction for Lorentz and
polarization effects were also applied with SAINTþ. An empirical
absorption correction based on the multiple measurement of
equivalent reflections was applied by using the program SADABS.
All structures were solved by a combination of direct methods and
difference Fourier syntheses and were refined by full-matrix least-
Hg(1) e I(1) e Hg(1 ) ¼ 91.11(2), Os(1) e C(1) e Os(2) ¼ 75.8(4). (For interpretation of
the references to color in this figure legend, the reader is referred to the web version of
this article.)
2
core having D symmetry. There are three independent Hg e I bond
i
distances: Hg(1) e I(1) ¼ 2.9112(8) Å, Hg(1) e I(1 ) ¼ 2.9645(8) Å
ii
and Hg(1) e I(1 ) ¼ 3.524(1) Å. Although transition metal halide
2
squares on F by using the SHELXTL software package [10]. All non-
cubanes are commonly found among the copper halide family of
complexes, they are rare among the Group IIB family of compounds
[11]. In fact, there has been only one previous structural verification
hydrogen atoms were refined with anisotropic displacement pa-
rameters. Hydrogen atoms were placed in geometrically idealized
positions and included as standard riding atoms during the least-
squares refinements. Crystal data, data collection parameters, and
results of the analyses are listed in Table 1. Compound 2 crystallized
in the orthorhombic crystal system. The space group Ccca was
indicated by the systematic absences in the data and confirmed by
the successful solution and refinement of the structure. The crystal
of a complex containing an Hg
complex anion [Hg I ]
8 20
4
I
4
cubane core. That was for the
[12]. The Hg e I distance in the cubane
core of this ion is 3.026(9) Å. Compound 2 contains four symmetry
equivalent Os (CO)10 -Ph) clusters. Each of which is linked to the
4
-
3
(m
cubane core via one bridging Hg atom. Each triosmium cluster in 2
contains ten linear carbonyl ligands and one edge-bridging phenyl
ligand. The latter which is analogous to the bridging phenyl ligand
in 1 serves as a 1-electron donor, B. Viewed as an uncharged
fragment the HgI group also serves as a 1-electron donor and
3
structure of 2 contains a significant void of 426 Å . The void
appeared to contain a highly disordered hexane molecule that was
cocrystallized from the crystallization solvent. Our efforts to devise
and refine a suitable disorder model were unsuccessful and the
void was ignored in the final refinements. Compound 3 crystallized
in the triclinic crystal system. The space group P-1 was confirmed
by the successful solution and refinement of the structure. Com-
pound 4 crystallized in the monoclinic crystal system. The space
group C2/c was indicated by the systematic absences in the data
and confirmed by the successful solution and refinement of the
structure. The Os e H distances in 4 were refined with distance
contraints of 1.80 Å.
3
therefore each Os cluster formally has only 46 valence electrons
instead of the expected 48 and is electronically unsaturated like
compound 1 [8a]. The unsaturation lies on the region of the
bridging phenyl ligand and the Os(1) e Os(2) bond, 2.8205(6) Å is
significantly shorter than the Os(1) e Os(3) ¼ 2.8761(6) Å and Os(2)
e Os(3) ¼ 2.8748(7) Å bonds. The analogous short bond in 1 is
significantly shorter, 2.7521(6) Å, than that in 2. The two inde-
pendent Os e Hg bond distances, Os(1) e Hg(1) ¼ 2.7930(6) Å,
Os(2) e Hg(1) ¼ 2.7978(7) Å, are slightly shorter than those found
to the bridging mercury atom in the compound [Os
3
(CO)10(m-
Results and discussion
Cl)] -Hg), 2.822(1) Å e 2.859(1) Å [13]. The Os e C distances to
2 4
(m
the bridging phenyl ligand are nearly equivalent, Os(1)
e
The reaction of Os
yielded the new compound [Os
yield. (Ph
Compound 2 was characterized by a single-crystal X-ray diffraction
analysis. An ORTEP diagram of the molecular structure of com-
pound 2 is shown in Fig. 1. Compound 2 is a tetramer of
3
(CO)10
(
m
ꢀ
h1ꢀPh)(
m
-AuPPh
3
), 1 with HgI
, 2 in 19%
2
C(1) ¼ 2.309(12) Å and Os(2) e C(1) ¼ 2.285(12) Å.
The bridging phenyl ligand in 1 was observed to undergo a
dynamical 2-fold rotation of the ring perpendicular to the Os e Os
3
(CO)10
(
m-Ph)( -HgI)]
m
4
3
P)AuI is the major colorless coproduct in this reaction.
1
bond on the H NMR timescale at elevated temperatures [8b].
Unfortunately, compound 2 is readily transformed thermally into
another product, see below, when heated so
a traditional
3 4 4
Os (CO)10(m-Ph)(m-HgI) that is held together by a cubane-like Hg I
temperature-dependent dynamic NMR investigation of 2 was not
Please cite this article in press as: R.D. Adams, et al., Journal of Organometallic Chemistry (2014), http://dx.doi.org/10.1016/
j.jorganchem.2014.08.009