1638
R.D. Adams et al. / Journal of Organometallic Chemistry 693 (2008) 1636–1644
was heated to reflux for 3.5 h. The solvent was removed in
vacuo, and the products were then isolated by TLC by using
a 3:1 hexane/methylene chloride solvent mixture to yield in
order of elution the following: 4.8 mg (14% yield) of 6,
2.0 mg (4% yield) of mer-Re(Ph)(CO)3(SbPh3)2 (8), 1.1 mg
(3% yield) of Re2(CO)7(SbPh3)(l-SbPh2)2 (9), 2.0 mg (4%
yield) 7, 9.7 mg (31% recovered) of 4. Spectral data for 8.
from an octane/methylene chloride solvent mixture at room
temperature. Colorless single crystals of 5, 6, 9, 10 and 11
suitable for X-ray diffraction analyses were obtained by
slow evaporation of solvent from a hexane/methylene chlo-
ride solvent mixture at ꢀ25 °C. Colorless single crystals of
7 and 8 suitable for X-ray diffraction analyses were
obtained by slow evaporation of solvent from an octane/
benzene solvent mixture at room temperature. Each data
crystal was glued onto the end of a thin glass fiber. X-ray
intensity data were measured by using a Bruker SMART
APEX CCD-based diffractometer using Mo Ka radiation
IR mCO (cmꢀ1 in hexane): 1933(s), 1910(m) cmꢀ1 1H
.
NMR (CD2Cl2, in ppm) d = 7.15–7.67 (m, 30H, Ph),
6.52–6.93 (m, 5H, Ph–Re). Mass Spec. EI/MS m/z. 1054,
M+; 998, M+ꢀ2CO. The isotope pattern is consistent with
the presence of one rhenium atom. Spectral data for 9: IR
mCO (cmꢀ1 in hexane): 2072(m), 2024(w), 2008(vw),
1987(s), 1981(s), 1955(s), 1937(s), 1928(m). 1H NMR
(CD2Cl2, in ppm) d = 6.89–7.74 (m, 35H, Ph). EI/MS
m/z, 1474, M+, 1446, M+ꢀCO, 1418, M+ꢀ2CO, 1390,
M+ꢀ3CO. The isotope pattern is consistent with the pres-
ence of two rhenium atoms and three antimony atoms.
˚
(k = 0.71073 A). The raw data frames were integrated with
the SAINT+ program by using a narrow-frame integration
algorithm [6]. Correction for Lorentz and polarization
effects were also applied with SAINT+. An empirical absorp-
tion correction based on the multiple measurement of
equivalent reflections was applied using the program SAD-
ABS. All structures were solved by a combination of direct
methods and difference Fourier syntheses, and refined by
full-matrix least-squares on F2, using the SHELXTL software
package [7]. All non-hydrogen atoms were refined with
anisotropic displacement parameters. 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 Tables 1–3.
2.5. Reaction of 4 with H2
Compound 4 (44.5 mg, 0.0342 mmol) was dissolved in
25 mL of octane. While purging with H2 the reaction was
heated to reflux for 6.25 h. The solvent was removed in
vacuo, and the products were then isolated by TLC using
3:1 hexane/methylene chloride solvent mixture to yield in
order of elution the following: 9.4 (31% yield) Re2(CO)8-
(l-H)(l-SbPh2) (10), 3.7 mg (9% yield) Re2(SbPh3)(CO)7-
(l-SbPh2)(l-H) (11), 3.4 mg (7% yield) 9. Spectral data
for 10: IR mCO (cmꢀ1 in hexane): 2102(w), 2078(m),
Compounds 4, 5, 7, 10 and 11 all crystallized in the
ꢀ
triclinic crystal system. The space group P1 was assumed
Table 1
Crystallographic data for compounds 4 and 5
2009(s), 1997(s), 1971(s) cmꢀ1 1H NMR (CD2Cl2, in
.
Compound
4
5
ppm) d = 7.35–7.73 (m, 10 H, Ph), ꢀ16.341 (s, hydride,
1H). EI/MS m/z. 874, M+, 846, M+ꢀCO. The isotope pat-
tern is consistent with the presence of two rhenium atoms
and one antimony atom. Spectral data for 11: IR mCO
(cmꢀ1 in hexane): 2086(w), 2035(w), 2025(w), 1995(s),
Empirical formula
Formula weight
Crystal system
Re2Sb2O8C44H30
1302.58
Triclinic
ReSbO4C22H16
652.30
Triclinic
Lattice parameters
˚
a (A)
11.1865(4)
13.3720(5)
15.6059(6)
93.979(1)
95.802(1)
114.546(1)
2096.51(14)
9.5987(6)
10.9613(7)
11.1779(7)
71.178(1)
86.402(1)
84.894(1)
1108.04(12)
1959(m), 1940(m), 1931(m) cmꢀ1 1H NMR (CDCl3, in
.
˚
b (A)
˚
c (A)
ppm) d = 7.27–7.80 (m, Ph, 25H), ꢀ16.00 (s, hydride,
1H). EI/MS m/z.1198, M+, 1170, M+ꢀCO. The isotope
pattern is consistent with the presence of two rhenium
atoms and two antimony atoms.
a (°)
b (°)
c (°)
3
˚
V (A )
ꢀ
ꢀ
Space group
Z value
P1 ð#2Þ
P1 ð#2Þ
2
2
2.6. Detection of benzene formation
qcalc (g/cm3)
l (Mo Ka) (mmꢀ1
Temperature (K)
2Hmax (°)
Number of observed (I > 2r(I))
Number of parameters
Goodness-of-fit (GOF)
Maximum shift in cycle
Residualsa: R1; wR2
2.063
7.081
294(2)
56.64
8149
505
1.036
0.002
0.0289; 0.0597
Multi-scan,
1.000/0.810
1.349
1.955
6.699
294(2)
56.62
4720
257
1.044
0.001
0.0312; 0.0639
Multi-scan,
1.000/0.812
1.521
)
A 4.8-mg amount of 4 was dissolved in 0.6 mL of tolu-
ene-d8 in a 5 mm NMR tube. The NMR tube was evacuated
and filled with H2 five times. The NMR tube was heated in
an oil bath at 100 °C for 3 h. After this period of time the
NMR tube was taken out of the oil bath and cooled to
1
room temperature to acquire an H NMR spectrum. The
1H NMR spectrum of this solution showed a singlet at
Absorption correction,
maximum/minimum
d = 7.13 indicating the presence of benzene in solution.
Largest peak in final difference
ꢀ
3
˚
in map (e /A )
2.7. Crystallographic analyses
P
P
P
a
R = hkl(jjFobsj ꢀ jFcalcjj)/ hkljFobsj; Rw = [ hklw(jFobsj ꢀ jFcalcj)2/
P
P
1/2
hklwF2obs
]
;
w = 1/r2(Fobs); GOF = [ hklw(jFobsj ꢀ jFcalcj)2/(ndata
ꢀ
Colorless single crystals of 4 suitable for X-ray diffrac-
tion analyses were obtained by slow evaporation of solvent
nvari)]1/2
.