Organometallics
Article
the same (Figure S4, Supporting Information); the subtraction
spectrum did not show any ν(Ta−H) band.
flange, which was held to the top of the cross. The remaining two sides
of the cross were closed with KB flanges with holes where Kapton
windows were pasted at the center for X-rays to pass through. X-ray
absorption spectra were acquired at the National Synchrotron Light
Source (NSLS) (Beamline X-18b), at Brookhaven National Labo-
ratory, Upton, NY, USA, at room temperature at the tantalum LIII
edge, in the transmission mode with a double-crystal Si(111)
monochromator. The flux at X18b is 1 × 1010 photons/s at 100 mA
and 2.8 GeV, and the usable energy range is 5.8−40 keV. The
calibration was done using tantalum foil of 5 μm thickness. The
spectra were recorded between 9750 and 11000 eV with a 2.0 eV step.
The spectra analyzed were the result of the averaging of three such
acquisitions, and it was carefully checked that the results obtained were
comparable and reliable, since for each sample no evolution could be
detected by comparing the spectra between the first and last
acquisitions.
Ethylene Polymerization with 5. 5 (25 mg) and dry toluene (5
mL) were placed in a glass vial equipped with a magnetic stirrer. The
glass vial was sealed with a rubber cap under argon. Then the vial was
put into an ILS Premex parallel reactor system and stirred at 70 °C,
after the reactor was purged with N2 (99.999%) three times, ethylene
(99.95%) was introduced into the system with 50 bar pressure. After
the mixture was stirred for 1 h, the reaction was stopped and the
reactor was cooled to −5 °C to condense all the volatile components.
The liquid products were characterized by GC, and the PE produced
was isolated by filtration.
Reaction of 5 with 2-Pentyne. A 100 mg portion of 5 was placed in
a Schlenk flask with a septum, and the flask was evacuated to 10−5
mbar. Then, 10 μL of 2-pentyne was added by syringe. After standing
for 1 h at room temperature, 50 μL of H2O was added. The gas-phase
products in the flask were analyzed by GC; 55% of 2-pentyne
(corresponds to 1 equiv of the TaIII species) was consumed, and cis-2-
pentene and trans-2-pentene were found as the products in a ratio of
5:1.
XAS data were analyzed using the HORAE package, a graphical
interface to the AUTOBK and IFEFFIT code.37 XANES and EXAFS
spectra were obtained after performing standard procedures for pre-
edge subtraction, normalization, polynomial removal, and wave vector
conversion. Determination of the energy level (E0) was performed at
the first inflection point of the edge. For each atomic shell, the
following structural parameters were adjusted: coordination number
(N), bond length distance (R), and the so-called Debye−Waller factor
via the mean-square relative displacement (σ2) of the considered bond
length. The parameter ΔE0, which accounts for the difference between
the experimental absorption-edge energy and its estimate made by the
Solid-State Nuclear Magnetic Resonance. All of the solid-state
NMR spectra were recorded on a Bruker AVANCE III spectrometer
1
operating at 400, 100, and 162 MHz resonance frequencies for H,
13C, and 31P respectively, with a conventional double-resonance 4 mm
CPMAS probe. The samples were introduced under argon into
zirconia rotors, which were then tightly closed. The spinning
1
frequency was set to 17 kHz for H and 10 kHz for 13C and 31P
2
code, was also fitted. The amplitude factor (S0 ) was fitted to the
spectra. NMR chemical shifts are given with respect to TMS or H3PO4
as external references. For CP/MAS 13C NMR, the following sequence
was used: 90° pulse on the proton (pulse length 2.4 s), then a cross-
polarization step with a contact time of typically 1 ms, and finally
acquisition of the 13C signal under high-power proton decoupling. The
delay between scans was set to 5 s, to allow the complete relaxation of
the 1H nucleus, and the number of scans was 20000 for 1D 13C NMR.
An apodization function (exponential) corresponding to a line
broadening of 100 Hz was applied prior to Fourier transformation.
For CP/MAS 31P NMR, 90° pulse on the proton and a cross-
polarization step with a contact time of 2 ms were used. The delay
between the scans was set to 5 s, no spectral smoothing was employed
prior to Fourier transformation, and the number of scans was 15000
for phosphine. For 2D HETCOR multiple-quantum spectra were
recorded on a Bruker DSX-600 spectrometer with a conventional
double-resonance 3.2 mm CPMAS probe. 1H−13C heteronuclear
correlation solid-state NMR was performed according to the following
scheme: 90° proton pulse, t1 evolution period, cross-polarization (CP)
to carbon spins, and detection of carbon magnetization under TPPM
decoupling.34,35 For the cross-polarization step, a ramped radio
frequency (rf) field centered at 75 kHz was applied to the protons,
while the carbon rf field was matched to obtain the optimal signal. A
total of 32 t1 increments with 2000 scans each were collected. The
sample spinning frequency was 10 kHz. Two-dimensional double-
quantum (DQ) and triple-quantum (TQ) spectra were recorded with
the following scheme:36 excitation of DQ coherences, t1 evolution, Z
filter, and detection. The spectra were recorded in a rotor
synchronized fashion in t1; that is, the t1 increment was set equal to
one rotor period (4.545 μs). One cycle of the standard back-to-back
(BABA) recoupling sequence was used for the excitation and
reconversion period. Quadrature detection in w1 was achieved using
the States-TPPI method. A spinning frequency of 22 kHz was used.
The 90° proton pulse length was 2.5 μs, while a recycle delay of 5 s
was used. A total of 128 t1 increments with 32 scans each were
recorded.
EXAFS spectrum obtained for the tantalum(V) methoxide (Ta-
(OMe)5) reference compound, the molecular structure of the
compounds being a dimeric molecule with two [TaO6] octahedra
sharing a common edge.38 S0 was found to be equal to 1.04 (see the
2
Supporting Information).
ASSOCIATED CONTENT
* Supporting Information
■
S
Tables and figures giving IR, NMR, and other characterization
data. This material is available free of charge via the Internet at
AUTHOR INFORMATION
Corresponding Author
■
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
■
The authors are indebted to Prof. Lyndon Emsley for his
enthusiastic discussions and suggestions. We also thank King
Abdullah University of Science and Technology for generous
research support.
REFERENCES
■
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EXAFS Experiments. All of the manipulations for the sample
preparation were done inside a nitrogen-filled glovebox. Finely ground
surface organometallic samples were spread uniformly on Scotch tape
and folded multiple times to obtain the desired thickness. This sample
was then placed inside an airtight commercial cross equipped with
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flange, centering ring including the O-ring, and hinged clamps. A tray
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dx.doi.org/10.1021/om4012196 | Organometallics 2014, 33, 1205−1211