R.D. Adams et al. / Journal of Organometallic Chemistry 751 (2014) 475e481
477
2003(m), 1986(m), 1942(w). 1H NMR (CD2Cl2,
d
in ppm) at 25 ꢁC:
also applied with SAINTþ. An empirical absorption correction
based on the multiple measurement of equivalent reflections was
applied using the program SADABS [16]. All structures were solved
by a combination of direct methods and difference Fourier syn-
theses, and refined by full-matrix least-squares on F2 by using the
SHELXTL software package [17]. All non-hydrogen atoms were
refined with anisotropic thermal parameters. The hydride ligand in
compound 6 was refined on its positional parameters with a fixed
isotropic thermal parameter. Compound 3 crystallized in ortho-
rhombic system. The space group Pna21 was indicated by the sys-
tematic absences in the data and confirmed by the successful
solution and refinement for the structure. Efforts to solve the
structure of 3 in the alternative centrosymmetric space group Pnma
were unsuccessful. Compounds 4, 6 and 7 crystallized in mono-
clinic system. The space groups P21/c in compound 4 and P21/n for
compounds 6 and 7 were uniquely identified by the systematic
absences in the data and were subsequently confirmed by the
successful solutions and refinements for the structures in each case.
Crystal data, data collection parameters, and results of these ana-
lyses are listed in Table 1.
d
¼ 7.22e7.84 (m, 10H, Ph). EI/MS m/z. 1034 (Mþ). Spectral data for
6. IR vCO (cmꢀ1 in hexane): 2126(w), 2089(m), 2082(m), 2073(s),
2056(w), 2044(vs), 2020(m), 2015(m), 2009(m), 2850(w). 1H NMR
(CD2Cl2,
d
in ppm) at 25 ꢁC:
d
¼ 6.59e7.08 (m, 4H, C6H4), ¼ ꢀ14.54
d
(s, hydride). EI/MS m/z. 1988 (Mþ).
3. Thermal transformations of 4
A 7.4 mg (0.0072 mmol) amount of 4 was dissolved in 10 mL of
hexane in a 50 mL three neck flask. The solution was heated up to
reflux for 5 h. After cooling, the solvent was removed in vacuo, and
the products were then isolated by TLC by using a 6/1 hexane/
methylene chloride elution solvent mixture to yield in order of
elution: 0.7 mg of 3 (10.5% yield); 3.2 mg of Os3(CO)10(m-h
2-O]
CPh)2, 7 [15] (42% yield). Spectral data for 7: IR vCO (cmꢀ1 in hex-
ane): 2099(w), 2068(vs), 2048(m), 2016(vs), 2005(s), 1998(m),
1989(w), 1983(m), 1975(w), 1954(vw). Mass Spec. EI/MS m/z. 1062
(Mþ).
3.1. Crystallographic analyses
3.2. Computational details
Yellow single crystals of 3 and orange single crystals of 4 suitable
for X-ray diffraction analysis were obtained by slow evaporation of
solvent from solutions in hexane/methylene chloride solvent
mixtures at ꢀ30 ꢁC. Dark green single crystals of 6 suitable for X-ray
diffraction analyses was obtained by slow evaporation of solvent
from a solution of the pure compound in a hexane/methylene
chloride solvent mixture at room temperature. Yellow single crys-
tals of 7 suitable for X-ray diffraction analyses was obtained by slow
evaporation of solvent from solutions in hexane solvent mixtures
at ꢀ30 ꢁC. Each data crystal was glued onto the end of a thin glass
fiber. X-ray diffraction intensity data were measured by using a
Density functional theory (DFT) calculations were performed
with the Amsterdam Density Functional (ADF) suite of programs
[18] by using the PBEsol functional [19] with Slater-type valence
quadruple-
z
þ 4 polarization function, relativistically optimized
(QZ4P) basis sets for osmium and valence triple-
z
þ 2 polarization
function (TZ2P) basis sets for carbon, oxygen, and hydrogen atoms
with small frozen cores and a scalar relativistic ZORA (Zeroth-Order
Regular Approximation) correction. The molecular orbitals for 3
and their energies were determined by a geometry-optimized gas-
phase calculation that was initiated with the structure as found in
the solid state. Electron densities at the bond critical points around
the C6 ring were calculated by using the Bader Quantum Theory of
Atoms In a Molecule (QTAIM) model and the AIMAll software
package [20,21].
Bruker SMART APEX CCD-based diffractometer by using Mo K
a
ꢀ
radiation (
l
¼ 0.71073 A). The raw data frames were integrated with
the SAINT þ program by using a narrow-frame integration algo-
rithm [16]. Corrections for Lorentz and polarization effects were
Table 1
Crystallographic data for compounds 3, 4, 6 and 7.
Compound
3
4
6
7
Empirical formula
Formula weight
Crystal system
Os3O10C16H4
926.79
Orthorhombic
Os3O11C23H10
1032.91
Monoclinic
Os6BiO17C29H10
1987.48
Monoclinic
Os3O12C24H10
1060.92
Monoclinic
Lattice parameters
ꢀ
a (A)
13.9465(3)
8.9230(2)
15.2811(3)
90.00
90.00
90.00
1901.65(7)
Pna21, no.33
4
3.237
20.048
294(2)
56.06
3363
263
1.035
0.001
0.0190, 0.0326
Multi-scan
1.000/0.749
0.496
10.9741(10)
28.833(3)
8.4711(8)
90.00
110.460(2)
90.00
2511.3(4)
P21/c, no.14
4
2.732
15.200
294(2)
50.06
4429
334
1.070
0.000
0.0423, 0.0759
Multi-scan
1.000/0.703
1.369
9.6005(4)
24.3314(10)
16.4283(7)
90.00
102.0420(10)
90.00
3753.1(3)
P21/n, no.14
4
3.517
24.977
294(2)
50.06
6624
475
1.090
0.001
0.0637, 0.1201
Multi-scan
1.000/0.523
2.935
16.766(3)
9.4626(14)
16.991(3)
90
99.243(3)
90
2660.6(7)
P21/n, no.14
4
2.649
14.354
294(2)
50.06
4689
352
1.071
0.001
0.0368, 0.0793
Multi-scan
1.000/0.646
1.387
ꢀ
b (A)
ꢀ
c (A)
a
b
g
(deg)
(deg)
(deg)
3
ꢀ
V (A )
Space group
Z value
rcalc (g/cm3)
m
(Mo Ka) (mmꢀ1
)
Temperature (K)
Qmax (ꢁ)
No. Obs. (I > 2
No. Parameters
2
s
(I))
Goodness of fit GOFa
Max. shift in cycle
Residualsa: R1; wR2
Absorption
Correction, Max/min
Largest peak in Final Diff. Map (eꢀ/A )
3
ꢀ
GOF ¼ [Shklw (rFobsr ꢀ rFcalcr)2/(ndata e nvari)]1/2
.
a
R ¼ Shkl(rrFobsr ꢀ rFcalcrr)/ShklrFobsr; Rw ¼ [Shklw(rFobsr ꢀ rFcalcr)2/ShklwF2
]
s
1/2; w ¼ 1/ 2(Fobs).
obs