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phase modulation. A variable neutral density filter, an optical aper-
ture, and a pair of polarizer were inserted in the path to generate
stable white-light continuum. Prior to generating the probe contin-
uum, the laser pulse was fed to a delay line that provides an exper-
imental time window of 3.2 ns with a maximum step resolution of
7 fs. In our experiments, a wavelength at l=420 nm was irradiated
at the sample cell with a spot size of 1 mm diameter where it was
merged with the white probe pulse in a close angle (<108). The
probe beam after passing through the 2 mm sample cell was fo-
cused on a fiber optic cable that was connected to a CMOS spec-
trograph for recording the time-resolved spectra (l=410–800 nm).
Typically, 3000 excitation pulses were averaged for 3 seconds to
obtain the transient spectrum at a set delay time. Kinetic traces at
appropriate wavelengths were assembled from the time-resolved
spectral data. All measurements were conducted at room tempera-
ture, 295 K.
Reaction procedure
Typically, the stoichiometric photoreaction was performed by the
following procedure. A benzene solution (3.0 cm3) containing DDQ
(3.0 mm) and H2O (50 mm) in a quartz cuvette (1.0 cmꢁ1.0 cm)
with a rubber septum was deaerated by bubbling with nitrogen
through a stainless steel needle for 5 min. In the case of photoca-
talytic reaction, a benzene solution containing DDQ (0.30 mm) with
tert-butyl nitrite (TBN, 3.0 mm) and H2O (50 mm) in a square quartz
cuvette with rubber septum was saturated with dioxygen by bub-
bling dioxygen through a stainless steel needle for 5 min. The solu-
tion was then irradiated with a 500 W xenon lamp (Ushio Optical
Module X SX-UID 500XAMQ) through a color glass filter transmit-
ting l>390 nm at room temperature. After photoirradiation, the
corresponding oxygenated products were identified and quantified
by comparison of the GC-MS analyses with those of the authentic
samples. The photochemical reactions were monitored using a Shi-
madzu GC-17A gas chromatograph and Shimadzu MS-QP5000 GC-
MS spectrometer.
Theoretical calculations
Density functional theory (DFT) calculations were carried out with
Gaussian 09 (Revision D.01, Gaussian, Inc.).[28] The calculations were
performed on a 32-processor QuantumCube at the B3LYP/6–31+
G(d,p) level of theory. Graphical outputs of the computational re-
sults were generated with the GaussView software program (ver.
3.09) developed by Semichem, Inc.[29]
Quantum yield determinations
A standard actinometer (potassium ferrioxalate) was used for the
quantum yield determination of the DDQ photosensitized hydrox-
ylation of aromatic compound with water.[27] Typically, a square
quartz cuvette (10 mm i.d.) that contained a substrate solution
(3.0 cm3) of DDQ (1.0 mm) and H2O (50 mm) was irradiated with
monochromatized light of l=420 nm from a Shimadzu RF-5300PC
fluorescence spectrophotometer. Under the conditions of actino-
metry experiments, DDQ absorbed essentially 99% incident light
of l=420 nm (Abs420 ꢁ3). The light intensity of monochromatized
light of l=420 nm was determined as 7.2ꢁ10ꢀ9 einsteinsꢀ1. The
photochemical reaction was monitored using a Shimadzu GC-17 A
gas chromatograph and Shimadzu MS-QP5000 mass spectrometer.
The quantum yields were determined from concentrations of
phenol derivatives.
Acknowledgements
This work was supported by Grants-in-Aid (Nos. 26620154 and
26288037 to K.O.) from the Ministry of Education, Culture,
Sports, Science and Technology (MEXT) and an ALCA project
from JST, Japan (to S.F.).
Keywords: electron transfer · organocatalysis · oxidation ·
photochemistry · redox chemistry
Laser flash spectroscopy
Measurements of nanosecond laser flash photolysis for photoexci-
tation of DDQ in PhCN were performed according to the following
procedures. Typically, a nitrogen-saturated PhCN solution contain-
ing DDQ (1.2 mm) in the presence of H2O was excited by a Nd:YAG
laser (Continuum, SLII-10, 4–6 ns fwhm) at l=430 nm with the
power of 3.0 mJ/pulse. Photoinduced events were monitored by
use of a continuous Xe lamp (150 W) and an InGaAs-PIN photo-
diode (Hamamatsu 2949) as a probe light and a detector, respec-
tively. The output from the photodiodes and a photomultiplier
[5] a) G. Palmisano, V. Augugliaro, M. Pagliaro, L. Palmisano, Chem.
tube was recorded with
a digitizing oscilloscope (Tektronix,
TDS3032, 300 MHz). The transient spectra were recorded for fresh
solutions in each laser excitation. All experiments were performed
at 298 K. Femtosecond transient absorption spectroscopy experi-
ments were conducted using an ultrafast source: Integra-C (Quan-
tronix Corp.), an optical parametric amplifier: TOPAS (Light Conver-
sion Ltd.) and a commercially available optical detection system:
Helios provided by Ultrafast Systems LLC. The source for the pump
and probe pulses were derived from the fundamental output of In-
tegra-C (l=786 nm, 2 mJ/pulse and fwhm=130 fs) at a repetition
rate of 1 kHz. 75% of the fundamental output of the laser was in-
troduced into a TOPAS unit for excitation light generation at l=
420 nm, whereas the rest of the output was used for white-light
generation. The laser pulse was focused on a sapphire plate of
3 mm thickness and then white-light continuum covering the visi-
ble region from l=450 nm to 800 nm was generated through self-
[11] T. Koike, M. Akita, Synlett 2013, 24, 2492.
pedia of Radical in Chemistry: Biology and Materials, (Ed.: C. Chatgilialo-
glu, A. Studer), Wiley, Chichester, UK, pp. 365–394, 2012.
5163; b) S. Fukuzumi, K. Ohkubo, T. Suenobu, K. Kato, M. Fujitsuka, O.
&
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Chem. Eur. J. 2014, 20, 1 – 8
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ÝÝ These are not the final page numbers!