Sulfide Radical Cations in Electron Transfer
A R T I C L E S
Patterson methods and refined by least-squares techniques adapting the
An alternative mechanism to that shown in Scheme 10
involves thermodynamically unfavorable formation of super-
oxide (E°(O2/O2-•) ) -0.87 V vs SCE in CH3CN)51 by
pyrylium radical (TPP•, 2MeOTPP•, and 2MeOSTPP•) reduction
of oxygen that is driven by its rapid reaction with sulfide radical
cation, or its formation by decomposition of 7SOO• and 8SOO•,
and its subsequent reaction via steps 3 and 4 in the Baciocchi
mechanism2 (Scheme 8). This would provide a rationale for the
observed quenching by benzoquinone. However, the absence
of the diagnostic superoxide product 6 formed in the NMQ+-
catalyzed reaction of 1 (eq 2) precludes this alternative pos-
sibility.
full-matrix weighted least-squares scheme, w-1 ) σ2Fo2 + (0.0596P)2
+ 0.17P, where P ) (Fo + 2Fc2)/3, on F2 using the SHELXTL
2
program.57,58
C14H12S2O2 crystallizes in the centrosymmetric triclinic space group
P1h. The asymmetric unit consists of a compound molecule. The
molecules are well ordered and well separated. All non-hydrogen atoms
were located in the difference maps during successive cycles of least-
squares and refined anisotropically. All of the hydrogen atoms except
for one were located in the Fourier maps and refined isotropically. One
of the hydrogen atoms was placed in a calculated position and refined
isotropically using a riding model. The final refinement parameters were
R1 ) 0.0364 and wR2 ) 0.1015 for data with F > 4σ(F), giving a
data-to-parameter ratio of 12. The refinement data for all of the data
were R1 ) 0.0403 and wR2 ) 0.1050.
Conclusion
We have demonstrated that electron-transfer photooxygen-
ations of sulfides are far more complex than previously assumed.
Although the experimental data suggests that NMQ+ functions
as a simple outer sphere electron shuttle between the sulfide
and oxygen, and pyrylium cations function by a less passive
inner sphere mechanism. We also introduced a new technique,
the photooxygenation of 2d4, to detect the absence of a
persulfoxide in electron-transfer-catalyzed oxygenations and
illustrated its use with the pyrylium cation sensitizer, 2MeOT-
PP+.
Laser Flash Photolysis. Nanosecond laser flash photolysis experi-
ments were conducted using an excitation wavelength of 355 nm (5-
20 mJ/pulse) from a Nd:YAG laser. The transient spectra were recorded
with a point-point technique with 5-10 nm intervals from 350 to 700
nm. The kinetic decays were the average of at least 10 shots. Samples
were degassed by either three freeze-pump-thaw cycles or by bubbling
with argon. The optical densities were adjusted to between 0.3 and 0.6
at the excitation wavelength. When oxygen was needed, the sample
was saturated with oxygen for 20 min. Several solvents were used
including methylene chloride, 1,2-dichloroethane, and acetonitrile. In
general, the most intense peaks were observed in 1,2-dichloroethane.
The singlet-oxygen experiments were done with oxygen-saturated
solutions using either the 355 or 532 nm output of a 10 Hz Nd:YAG
laser. The kinetic apparatus consisted of a germanium (Judson 5 mm
φ) diode detector/customized preamplifier and various optics: A 10
nm narrow band-pass non-fluoresceing filter centered at 1.27 µm placed
just ahead of the detector, a 500 MHz LeCroy transient digitizer/signal
averager interfaced to a computer, and an energy meter. Because the
experimental decay is a convolution of the detector response (fwhm of
approximately 10 ps for the 5 mm φ detector) and the sample decay,
it was necessary to implement a numerical deconvolution analysis to
accurately extract measured lifetimes 100 µs g τ g 2 ms from the
recorded data. The numerical deconvolution analysis of Demas59 for
exponential decays corrects artifacts caused by scattered excitation light
that may reach the detector that was used. This analysis was
implemented on our laboratory computer using a general scientific/
engineering analysis/data acquisition program called Lifetime. Signal
averaging 100 experiments, each with laser pump energies e5 mJ gave
8192-point decay curves, each of which produced pseudo first-order
rate constants with correlation coefficients (square root) better than 0.99.
Experimental Section
Sulfides 1, 2,10 2SO,10 2SOd4,10 2d4,10 3,25 4,25 5,25 6,25 and
NMQ+BF4
were all synthesized as reported in the literature.
-53
Commercial samples of TPP, and 2MeOTPP were used as received
for the photochemical reactions and purified by recrystallization from
ethanol for the electrochemical studies.
2-(p-Methoxyphenyl)-4,6-diphenyl-thiapyrylium Tetrafluorobo-
rate. 2-MeO-STPP was synthesized using a modified procedure of
Suld54 and Wizinger.55 A 2.5 mL H2O solution of sodium sulfide
nonahydrate (250 mg, 1.04 mmol) was added to a solution of 2MeOTPP
(0.21 g, 0.5 mmol) in 10 mL of acetone. After the addition was
complete, the mixture was stirred for 0.5 h, then acidified with 2.5 mL
of 48% HBF4, diluted with 10 mL of H2O, stirred for 2 h, and then
filtered. The crude product was recrystallized twice from ethanol. Yield
11%. 1H NMR (CD3CN) δ 3.96 (s, 3H), 7.27(d, J ) 8.7 Hz, 2H), 7.70-
7.81(m, 6H), 8.07-8.17(m, 6H), 8.80(d, J ) 14.7 Hz, 2H).
Radical Cation Preparation. Solutions of 1 and 2 were prepared
in a specially designed two-compartment cell with one compartment
filled with 0.1 M substrate and the second compartment with 1 equiv
of sublimed (220 °C) NOBF4 in acetonitrile. Both compartments were
subjected to a series of three freeze-pump-thaw cycles and then mixed
at room temperature under vacuum. The UV-vis spectra of 2+• was
collected immediately. The yellow color of 1+• disappeared too rapidly
to allow measurement of its UV-vis spectrum at room temperature.
Crystallographic Data for 5. X-ray diffraction data were collected
for C14H12S2O2 on a Bruker P4 Diffractometer equipped with a
molybdenum tube and a graphite monochromator at 25 °C. A colorless
rectangular prismatic crystal of approximate dimensions 0.52 × 0.36
× 0.24 mm3 glued to a glass fiber was used for data collection. A total
of 2812 (Rint ) 0.0226) independent reflections were gathered in the
2θ range of 4.04 to 55° with the data collected having -1 e h e 9,
-10 e k e 10, -13 e l e 13 using the XSCANS program.56 Three
standard reflections measured after every 97 reflections exhibited no
significant loss of intensity. The data were corrected for Lorentz-
polarization effects and absorption. The structure was solved by
Stern-Volmer Studies. All Stern-Volmer studies were done using
acetonitrile as the solvent and sensitizer concentrations of [NMQ+] )
1.5 × 10-5 M, [TPP+] ) 4 × 10-6 M, and [2MeOTPP+] ) 4 × 10-6
M. In the TPP+ quenching studies, the concentrations of 1 were varied
over the range of 5.16 × 10-4 to 9.82 × 10-3 M, the concentrations of
2 over the range of 5.7 × 10-4 to 5.7 × 10-3 M, and utilized an
excitation wavelength of 405 nm and slit widths of 2.5 nm on the
excitation side and 5 nm on the emission side. In the 2MeOTPP+
quenching studies, the concentrations of 1 were varied over the range
of 2.0 × 10-3 to 8.7 × 10-3 M, the concentrations of 2 over the range
of 6.6 × 10-4 to 7.9 × 10-3 M, and utilized an excitation wavelength
of 447 nm and slit widths of 5.0 nm on both the excitation side and
emission side. In the NMQ+ quenching studies, the 1 concentrations
were varied over the range of 2.5 × 10-4 to 1.5 × 10-3 M, and utilized
an excitation wavelength of 317 nm and slit widths of 2.5 nm on the
excitation side and 5 nm on the emission side. All slopes of the Stern-
(53) Donovan, P. F.; Conley, D. A. J. Chem. Eng. Data 1966, 11, 614-615.
(54) Suld, G.; Price, C. C. J. Am. Chem. Soc. 1962, 84, 2090-2094.
(55) Wizinger, R.; Ulrich, P HelV. Chim. Acta 1956, 39, 207-216.
(56) Bruker XSCANS, ver. 2.31; Bruker AXS: Madison, WI, 1993.
(57) Bruker SHELXTL, ver. 5.10; Bruker AXS: Madison, WI, 1997.
(58) Sheldrick, G. M. SHELXS97 and SHELXL97, University of Go¨ttingen:
Go¨ttingen, Germany, 1997.
(59) Love, J. C.; Demas, J. N. Anal. Chem. 1984, 56, 82.
9
J. AM. CHEM. SOC. VOL. 130, NO. 12, 2008 4067