Photocatalytic Hydrogen Evolution
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equipped with sub-nanosecond LED sources (280, 380, 460, and 600 nm,
500–700 ps pulse width) powered by a PicoQuant PDL 800-B variable
(2.5–40 MHz) pulsed power supply. The decays were analyzed by means
of PicoQuant FluoFit Global Fluorescence Decay Analysis Software.
action yields the reduced photosensitizer, which further
reacts bimolecularly with the catalyst, thereby triggering the
photocatalytic hydrogen production. Similar conclusions
have been recently reached by Eisenberg and coworkers
when comparing the photocatalytic efficiency of bound
versus free fluorescein/cobaloxime systems.[36]
A system similar to the one studied in this work has been
recently described by Sun and coworkers.[2d] It features the
same cobaloxime catalyst as used here, a zinc (instead of
aluminium) pyridyl porphyrin as sensitizer, and triethyla-
mine (instead of ascorbic acid) as sacrificial donor. In that
case, the mechanism was assumed to be unimolecular and
thought to consist of two consecutive steps: oxidative
quenching by the catalyst followed by hole transfer to the
sacrificial donor. From the viewpoint of hydrogen evolution,
that system (reported values in 80:20 THF/water, TON=22
in 5 h of irradiation)[2d] is considerably less efficient than the
present one.
In conclusion, a new noble-metal-free sacrificial donor/
photosensitizer/catalyst system for photochemical hydrogen
production, based on ascorbic acid, aluminium pyridyl por-
phyrin, and cobaloxime is presented. The hydrogen evolving
performance is good, particularly in terms of turnover fre-
quencies[48] (TOF=10.8 or 3.6 minꢀ1, with respect to the sen-
sitizer or the catalyst, respectively) and quantum yield (F=
4.6%, that is, 9.2% of maximum possible value). The turn-
over numbers (maximum TON=352 or 117, with respect to
the sensitizer or the catalyst, respectively) is limited by both
the permanent reduction of the sensitizer (formation of
chlorins) and the hydrogenation of the ligand of the cata-
lyst.
Ultrafast spectroscopy (UFS): Femtosecond time-resolved experiments
were performed by using a pump-probe setup based on the Spectra-Phys-
ics Hurricane Ti:sapphire laser source and the Ultrafast Systems Helios
spectrometer.[49] The 550 nm pump pulses were generated with a Spectra
Physics 800 OPA. Probe pulses were obtained by continuum generation
on a sapphire plate (useful spectral range: 450–800 nm). Effective time
resolution approximately 300 fs, temporal chirp over the white-light 450–
750 nm range approximately 200 fs, temporal window of the optical delay
stage 0–2000 ps. The time-resolved spectral data were analyzed with the
Ultrafast Systems Surface Explorer Pro software.
Nanosecond laser flash photolysis: Nanosecond transient measurements
were performed with a custom laser spectrometer comprised of a Contin-
uum Surelite II Nd:YAG laser (FWHM 6–8 ns) with frequency doubled,
(532 nm, 330 mJ) or tripled, (355 nm, 160 mJ) option, an Applied Photo-
physics xenon light source including a mod. 720 150 W lamp housing, a
mod. 620 power controlled lamp supply and a mod. 03-102 arc lamp
pulser. Laser excitation was provided at 908 with respect to the white
light probe beam. Light transmitted by the sample was focused onto the
entrance slit of a 300 mm focal length Acton SpectraPro 2300i triple gra-
ting, flat field, double exit monochromator equipped with a photomulti-
plier detector (Hamamatsu R3896) and a Princeton Instruments PIMAX
II gated intensified CCD camera, using a RB Gen II intensifier, a ST133
controller and a PTG pulser. An Edmund optics notch filter centered at
532 nm was used in order to avoid eventual scattered laser by the sample
to hit the detector. Signals from the photomultiplier (kinetic traces) were
processed by means of a LeCroy 9360 (600 MHz, 5 Gssꢀ1) digital oscillo-
scope.
Photolysis apparatus: The hydrogen evolution experiments were carried
out upon continuous visible-light irradiation with
a 175 W xenon
CERMAX arc-lamp (cut-off filter at 400 nm) of a reactor (a 10 mm path
length pyrex glass cuvette with head space obtained from a round-
bottom flask) containing the solution. The measuring cell was sealed
during the photoreaction: the head to which the cell is attached has
indeed four ports, closed with Swagelok connections, two of them are
part of a closed loop involving a GC gas inlet and a sample vent in order
to analyze the head space content without an appreciable gas consump-
tion, and the other two are for the degassing procedure (input and
output). Regarding the calculation of the photoreaction quantum yields
the irradiation was performed with an array of four high power Roithner
Lasertechnik orange (590 nm) 350 mA LEDs instead of white light (for
more details see the Supporting Information).
Experimental Section
Materials: Solvents for spectroscopic, photophysical, and photolysis
measurements were of spectroscopic grade, all the other chemicals were
of reagent grade quality, and were used as received.
Gas chromatography: The gas phase of the reaction vessel was analyzed
on an Agilent Technologies 490 microGC equipped with a 5 ꢃ molecular
sieve column (10 m), a thermal conductivity detector, and by using Ar as
carrier gas. An aliquot of 5 mL from the headspace of the reactor was
sampled by the internal GC pump and 200 nl were injected in the
column maintained at 608C for the separation and detection of gases.
The unused gas sample was then re-introduced in the reactor in order to
minimize its consumption along the whole photolysis. The amount of hy-
drogen was quantified through the external calibration method. This pro-
cedure was performed, prior to analysis, through a galvanostatic (typical-
ly 1 mA) electrolysis of a 0.1m H2SO4 solution in an analogous cell (same
volume) equipped with two Pt wires sealed in the glass at the bottom of
the cell. A 100% faradaic efficiency was assumed leading to a linear cor-
relation between the amount of H2 evolved at the cathode and the elec-
trolysis time.
NMR spectroscopy: 1H spectra were recorded at 400 MHz on a Bruker
Avance 400 QNP and at 500 MHz on a Bruker Avance 500. All spectra
were run at room temperature (298 K) in [D5]pyridine and [D3]acetoni-
trile. Proton peak positions were referenced to the peak of residual non-
deuterated solvent peaks.
Electrochemical measurements: Differential pulse voltammetry (DPV)
measurements were carried out with a PC-interfaced Eco Chemie Auto-
lab/Pgstat 30 potentiostat. Argon-purged 10ꢀ4 m sample solutions in THF,
containing 0.1m TBAPF6 (Fluka, electrochemical grade, 99%, dried in an
oven), were used. A conventional a three-electrode cell assembly was
adopted: a saturated calomel electrode (SCE Amel) and a platinum elec-
trode, both separated from the test solution by a glass frit, were used as
reference and counter electrodes, respectively; a glassy carbon electrode
was used as the working electrode. The thermodynamic reduction poten-
tials (half-wave potentials) were calculated from the relation E1/2
peak+DE/2, where DE is the pulse potential.
=
Hydrogen evolution experiments: In a typical experiment, samples of
5 mL were prepared in 20 mL scintillation vials starting from a solution
of AlP(OH) (1ꢂ10ꢀ4 m in water/organic solvent), and further adding
E
Steady-state absorption/emission measurements: UV/Vis absorption
spectra were recorded on a Jasco V-570 UV/Vis/NIR spectrophotometer.
Emission spectra were taken on a Horiba-Jobin Yvon Fluoromax-2 spec-
trofluorimeter, equipped with a Hamamatsu R3896 tube.
(H2O)] (small aliquots from a 3ꢂ10ꢀ2
AscH (as solid) and [CoACTHNUTRGENNU(G dmgH)ACHUTNGTRENNUNG m
mother solution in acetonitrile). The change in volume upon addition of
the latter can always be considered negligible (dilution ꢃ1%). The pH
of the final solution was adjusted (when required) upon further addition
of different aliquots of 1m NaOH or 1m HClO4 solution (total volume
Time-correlated single photon counting (TCSPC): Fluorescence lifetimes
were measured by using a TCSPC apparatus (PicoQuant Picoharp 300)
Chem. Eur. J. 2013, 19, 9261 – 9271
ꢁ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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