Communications
Experimental Section
BODIPY derivatives were synthesized according to literature proce-
dures with some modifications (see Supporting Information for
details)[20]
Microsized anatase TiO2 crystals with dominant (001) facets were
prepared by the hydrothermal method from titanium sulfate and
hydrofluoric acid according to literature procedures (see Supporting
Information for details).[21]
Steady-state UV/Vis absorption spectra were measured by a
Shimadzu UV-3100 UV/Vis/NIR spectrophotometer. Steady-state
fluorescence spectra were measured by a Hitachi 850 or HORIBA
FluoroMax-4 fluorescence spectrophotometer. Cyclic voltammetry
(CV) measurements were carried out at room temperature with an
electrochemical analyzer (ALS, 660A) with a standard three-elec-
trode configuration.
The experimental setup for single-particle experiments was based
on an Olympus IX71 inverted fluorescence microscope.[4] The details
of the experimental setup are described in the Supporting Informa-
tion. The position of the TiO2 particles immobilized on the cover glass
was determined from the transmission image obtained by illuminating
the sample from above with a halogen lamp (Olympus, U-LH100L-3).
Circularly polarized light emitted from a CW Ar ion laser (Melles
Griot, IMA101010BOS; 488 nm, 0.1 kWcmꢀ2 at the glass surface) was
reflected by a first dichroic mirror (Olympus, RDM450) toward a
second dichroic mirror (Olympus, DM505). The laser light passing
through an objective lens (Olympus, UPLSAPO 100XO; 1.40 NA,
100 ꢀ ) after the reflection at the second dichroic mirror was totally
reflected at the cover glass/methanol interface, which generated an
evanescent field, making it possible to detect a single fluorescence dye
molecule. For excitation of the TiO2 particles, the 365 nm light
emitted by an LED (OPTO-LINE, MS-LED-365) and passing
through a neutral density (ND) filter was passed through the
objective. The fluorescence emission from the fluorescent products
generated over a single TiO2 particle on the cover glass was collected
by using the same objective, magnified by a 1.6 ꢀ built-in magnifi-
cation changer, passed through a bandpass filter (Semrock, FF01-531/
40-25) to remove the undesired scattered light, and then imaged by an
electron-multiplying charge-coupled device (EM-CCD) camera
(Roper Scientific, Cascade II:512). The images were recorded at a
frame rate of 20 framessꢀ1. All experimental data were obtained at
room temperature.
Confocal fluorescence images were taken by using an objective-
scanning confocal microscope system (PicoQuant, MicroTime 200)
coupled to an Olympus IX71 inverted fluorescence microscope. The
samples were excited through an oil-immersion objective lens
(Olympus, UAPON 150XOTIRF; 1.45 NA, 150 ꢀ ) with a 485 nm
pulsed laser (PicoQuant, LDH-D-C-485; 2 kWcmꢀ2 at the glass
surface) controlled by a PDL-800B driver (PicoQuant). The emission
from the sample was collected by the same objective and detected by
a single-photon avalanche photodiode (Micro Photon Devices, PDM
50CT) through a dichroic beam splitter and bandpass filter (Semrock,
FF01-531/40-25).
Figure 4. A) Structure of anatase TiO2 crystal with preferential (001)
facets. Transmission (B) of a single TiO2 crystal on the cover glass and
fluorescence (C) images of the same crystal in Ar-saturated 2.0 mm
DN-BODIPY solution under 488 nm laser and UV irradiation
(30 mWcmꢀ2 at the glass surface). The red and blue dots in image B)
indicate the fluorescence bursts located on the (101) and (001)
surfaces, respectively, observed during 3 min irradiation. The precise
positions at which fluorescent products were generated were deter-
mined by centroid analysis. The arrow in image C) indicates the
fluorescence spot.
found to be preferentially located on the (101) surface of the
crystal (see red dots in image B). A similar tendency was
observed for more than five individual crystals examined. The
average counting rates of single dye molecules were roughly
estimated to be (53 ꢃ 10) and (17 ꢃ 4) molecules mmꢀ2 minꢀ1
for (101) and (001) surfaces, respectively; this strongly
indicates the effect of crystal facets on the photocatalytic
activity, which is not evident in the bulk measurement.[18] Our
finding is generally consistent with previous studies and may
be explained by differences in surface energy levels of the
conduction and valence bands, surface structures, and
adsorption energies of substrates on the exposed crystal
faces.[19] However, further work is needed to clarify the
detailed mechanism of the face-selective photocatalytic
reaction.
Received: August 10, 2010
In conclusion, we propose novel single-molecule fluores-
cence probe DN-BODIPY for studying the reduction process
involved in ET on the TiO2 surface. Single-molecule kinetic
and imaging analyses of the fluorescence bursts emitted from
the products revealed the temporal dynamics of molecular
interactions and interfacial ET, and heterogeneous distribu-
tions of reactive sites on individual catalyst particles. Our
methodology should provide a suitable approach to exploring
the electron-transport characteristics in various semiconduc-
tor (photo)catalysts as well as metal–semiconductor and
semiconductor–semiconductor nanocomposites.
Published online: October 4, 2010
Keywords: electron transfer · fluorescent probes · nanoparticles ·
.
photochemistry · single-molecule studies
[1] Electron Transfer in Chemistry, Vols. 1–5 (Ed.: A. Balzani),
Wiley-VCH, Weinheim, 2001.
[2] a) M. R. Hoffmann, S. T. Martin, W. Choi, D. W. Bahnemannt,
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2010, 49, 8593 –8597