Electrocatalytic Proton Reduction
jacketed silver wire pseudo-reference electrode. The potential of
the silver electrode was referenced against the ferrocenium/ferrocene
couple, and all potentials are reported relative to the saturated
calomel electrode (SCE), where in THF E°′(Fc+/Fc) ) 0.53 V.32
The working electrode was polished with 0.3 µm alumina and
sonicated in THF between experiments. Acid titration experiments
were performed by measured addition of a THF solution of
p-toluenesulfonic acid (0.2 M) together with the complex and
supporting electrolyte at the same conditions as used in the initial
electrochemical experiment. Electrochemical simulations were
performed using DIGISIM version 3.0.18
and the front window consisted of a 25 µm thick film of Teflon-
coated Kapton. The 1/16 in. Teflon tubing used to transfer solutions
to/from the cell were press-sealed into holes in the Teflon block.
For electrochemically generated samples (TBA)PF6 (0.2 M) was
used as the supporting electrolyte. For solutions in acetonitrile the
data were in some instances affected by crystallinity leading to the
loss of data over a narrow k range for different of the detector
elements. This problem was ameliorated by rapidly freezing the
sample in isopentane (140 K) before storage in liquid nitrogen prior
to loading into the closed-cycle helium Displex cryostat (10 K).
The quality of the samples was established by IR spectroscopy
(Shimadzu Prestige FTIR) using an in-line system that included
both the fluorescence EXAFS cell and a solution IR cell. The
sample was frozen immediately after transfer to the EXAFS cell.
Infrared spectroelectrochemical (IR-SEC) measurements were
made using a purpose built high-pressure SEC cell capable of
operating at elevated gas pressure.33 In all experiments vitreous
carbon was used as the working electrode. Measurements were
generally conducted at gas pressures in the range 275-680 kPa.
Spectra of the thin film of solution (10-20 µm) in contact with
the working electrode were recorded during electrolysis at 1-2 s
intervals. Spectra are presented in absorbance mode where the
reference spectrum was recorded immediately before the application
of an oxidizing or reducing potential. A PAR model 362 potentiostat
was used to control the potential during SEC experiments.
The solution sample of 12- was generated by continuous-flow
electrosynthesis.34 The potential for these experiments was con-
trolled using a PAR 273A potentiostat. Samples of 1H- and C
W
were generated chemically. The sample of 1H-W was prepared by
reaction of a 3.5 mM solution of 1 in THF with 1 mol equiv of
Super-Hydride. IR spectroscopy was used to confirm that the
reaction proceeded quantitatively and with no significant formation
of side products. Exposure of this sample to CO resulted in its
conversion to C. Owing to the presence of Li+ the product contains
a mixture of ion-paired (35%) and non-ion-paired (65%) forms of
C. The sample used for EXAFS measurements contained a total
Continuous-flow electrosyntheses were performed using a pur-
pose built airtight cell based on a design reported previously.34 The
working and counter electrodes were fashioned from reticulated
vitreous carbon, and the reference electrode consisted of a jacketed
silver wire or a no-leak Ag/AgCl reference electrode (Cypress
Systems), which was inserted into a small cavity in the working
electrode. Standard liquid chromatography valves, gastight syringes,
and fittings (Hamilton) in conjunction with thick-walled 1/16 in.
Teflon tubing permitted anaerobic transfer of solution to and from
the cell. The flow of solution to the cell was controlled using a
syringe pump that was typically operated at a flow rate of 5 µL
s-1. The cell was jacketed, and the temperature could be maintained
at -50 °C for the duration of the experiment. IR spectra were
collected using a Bio-Rad FTS 175C spectrometer which utilized
a glowbar source, Ge/KBr beam splitter, and a liquid-nitrogen-
cooled MCT detector. NMR spectra were recorded using a Varian
Unity Plus 400 MHz instrument; chemical shifts of 31P NMR spectra
were referenced relative to H3PO4. Electrospray mass spectra were
recorded using a Micromass Quattro II mass spectrometer in
negative ion mode. Deoxygenated acetonitrile was used as the
mobile phase, and N2, as the drying and nebulizing gas. Sample
concentrations were approximately 0.4 µM.
of 5-10% 1 and 1H- (IR, Supporting information).
W
Data reduction of experimental X-ray absorption spectra was
performed using the program XFIT.27,28 The photon energy was
calibrated against the absorption edge of Fe foil, where the peak in
the first derivative was assigned an energy of 7111.2 eV. Back-
ground removal from the EXAFS data was performed both
automatically and manually using the AUTOBK algorithm35
(implemented within Athena36) and XFIT27,28 spline packages,
respectively. The use of both approaches provided an additional
check on the reliability of the EXAFS function.35,37 The model
structures were refined using the software package XFIT,27,28 which
incorporates ab initio FEFF 6.0138 MS curved-wave calculations.
The calculations included MS paths with Rmax ) 4 Å (maximum
effective path length of 8 Å) and up to four legs. The plane wave
and curved wave path filter thresholds were set at 2% and 3% of
the strongest MS path, respectively. A nonlinear least-squares fitting
is used to vary the model and concurrently optimize the fit of the
calculated to the observed EXAFS.27 The goodness of fit residual
parameter (RXAFS) has been defined28 where an RXAFS value around
20% is considered a good fit to the non-Fourier-transformed data,
while an RXAFS value greater than 40% is poor. The random
(statistical) errors (σr) in the Fe-L bond lengths due to noise in
the EXAFS data were estimated by Monte Carlo calculations.27,28
These were combined with the typical systematic errors (σs),
assigned a conservative consensus value of 0.02 Å,28 to give the
maximum root-mean-square (rms) error ([σr2 + σs2]1/2). A descrip-
tion of the models used for data analysis together with details of
X-ray fluorescence measurements were made at a temperature
of ca. 10 K using beamline 20B (bending magnet) at the KEK
Photon Factory, Tskuba, Japan. A channel-cut Si(111) monochro-
mator provided an energy resolution (∆E/E) of ca. 2.4 × 10-4
,
and higher order harmonics of the selected wavelength were rejected
by detuning the monochromator by a factor of a half. EXAFS
measurements were conducted at the Fe K-edge (7111.2 eV). Solid
samples were dispersed in boron nitride, and data were measured
in transmission mode using an ion chamber detector. Solutions were
measured in fluorescence mode using a 10-element Ge detector
and were prepared so as to give a concentration of 3-5 mM (i.e.
6-10 mM in iron) in either acetonitrile or THF. The fluorescence
cell consisted of a Teflon block with a 1.5 × 1.5 × 10 mm channel,
2
the symmetry constraints and restraints on E0, S0 , and σ2 is available
as Supporting Information.
(35) Newville, M.; Livins, P.; Yacoby, Y.; Rehr, J. J.; Stern, E. A. Phys.
ReV. B: Condens. Matter 1993, 47, 14126-14131.
(36) Ravel, B. Athena, 0.8.019; University of Washington: Seattle, WA,
2001.
(37) Bridges, F.; Booth, C. H.; Li, G. G. Physica B (Amsterdam) 1995,
208, 209, 121-124. Li, G. G.; Bridges, F.; Booth, C. H. Phys. ReV.
B: Condens. Matter 1995, 52, 6332-6348.
(38) Zabinsky, S. I.; Rehr, J. J.; Ankudinov, A.; Albers, R. C.; Eller, M. J.
Phys. ReV. B: Condens. Matter 1995, 52, 2995-3009.
(32) Chang, D.; Malinski, T.; Ulman, A.; Kadish, K. M. Inorg. Chem. 1984,
23, 817-24. Connelly, N. G.; Geiger, W. E. Chem. ReV. 1996, 96,
877-910.
(33) Borg, S. J.; Best, S. P. J. Electroanal. Chem. 2002, 535, 57-64.
(34) Bondin, M. I.; Foran, G.; Best, S. P. Aust. J. Chem. 2001, 54, 705-
709.
Inorganic Chemistry, Vol. 43, No. 18, 2004 5643