Photoinduced Electron Transfer in Chormophores
J. Phys. Chem. B, Vol. 111, No. 24, 2007 6893
frames were oriented such that orthogonal wedges of reciprocal
space were surveyed. The data collection was carried out using
Mo KR radiation (graphite monochromator) with a frame time
of 5 s and a detector distance of 5.03 cm. A randomly oriented
region of reciprocal space was surveyed: four major sections
of frames were collected with 0.50° steps in ω at four different
φ settings and a detector position of -33° in 2θ. The intensity
data were corrected for absorption. Final cell constants were
calculated from the xyz centroids of 3975 strong reflections from
the actual data collection after integration. Additional crystal
and refinement information can be obtained from the CIF file
deposited as Supporting Information.
absence of quencher, τo is the excited-state lifetime in the
absence of quencher, I and τ are the corresponding values in
the presence of quencher, kq is the bimolecular quenching rate
constant, and [Q] is the molar concentration of the quencher.
Acknowledgment. This work is dedicated to Norman Sutin
for his leadership in electron transfer and recognition of the
potential of metal complex excited states for solar energy
conversion. We wish to thank the Division of Basic Sciences,
U.S. Department of Energy for financial support of this research
(Grant DE-FG02-90ER14125).
Supporting Information Available: X-ray crystallographic
data of complex 1 in CIF format. This material is available free
Quenching Experiments. For all of the quenching experi-
ments, stock solutions of the chomophores were made in
acetonitrile/water (2:3 v/v) containing 5 mg of the particular
complex. Samples with known quencher concentrations were
prepared by adding an appropriate amount of solid quencher to
10 mL volumetric flasks containing the diluted Pt chromophore
stock solutions (1.0 × 10-5 M). The solutions were deaerated
by three freeze-pump-thaw cycles. Steady-state luminescence
spectra were then collected for each sample. UV-vis spectra
were taken for each experiment to inspect potential photochemi-
cal products. In the simple bimolecular quenching reactions,
there was no evidence of any change in absorption spectra under
all experimental conditions. However, in the presence of both
TEOA and MV2+ reagents, visible excitation of the Pt chro-
mophore generated the blue methyl viologen radical cation,
which was detected by UV-vis spectra.
References and Notes
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To investigate concentration effects of the different Pt
chromophores, electron relays, the sacrificial donor, and the
solution pH, one of the reaction components was varied while
the others were held constant. General reaction conditions and
concentrations included 2.2 × 10-5 M Pt chromophore, 5.6 ×
10-3 M TEOA, 6.0 × 10-5 M Pt colloid, 3.1 × 10-4 M MV2+
or diquat, and pH 7. When examining the reductive quenching
effects on H2 production for chromophore 2, concentrations of
TEOA were varied in the range 5.6 × 10-3- 0.11 M. Likewise,
for oxidative quenching effects on H2 production for Pt
chromophore 2, concentrations of the electron relay DQ4 were
varied in the range 1 × 10-4- 6.2 × 10-3 M.
Determination of Rate Constants from Quenching Experi-
ments. In all samples, quenching rate constants (kq) were
evaluated from steady-state luminescence experiments. Addition
of quenchers to the Pt(II) compounds resulted in concentration-
dependent luminescence intensity quenching. Bimolecular quench-
ing was well-modeled by the Stern-Volmer equation46 (eq 2),
where Io is the integrated MLCT emission intensity in the