to the intraparticle energy transfer which combines donor–
acceptor emissions apparently into a single peak, as discussed
above. The two-photon excitation of OSNP at 780 nm also
produces a similar fluorescence spectrum and pH-dependence,
except that the peak position and the intensity are slightly different
at every measured pH, due to the different two-photon
absorptivity of the NVP component between the neutral and the
protonated states. Despite a lack of noticeable dual emission, the
spectral evolution of one- and two-photon fluorescence of OSNP
enables ratiometric probing in the range of pH 4–8 at room
temperature, as shown in Fig. 2d. The intensity ratio of emissions
at 580 and 460 nm varies with pH, by one order of magnitude
under one-photon excitation and 3.4 times under two-photon
excitation. Importantly, OSNP, which includes a less proton-
sensitive pyridine-based dye, shows a greater response in the weak
acidic range by virtue of the improved proton sensitivity. From the
fitting of the titration curves, the same pKa values (y 6.4) were
extracted by both one- and two-photon excitation, which are
similar to the values obtained by a carboxyfluorescein probe, often
used for near-physiological pH measurement.2
In summary, the basic dye-concentrated nanoparticle structure
has been shown to improve the proton sensing ability, in terms of
fluorescence, through nanoscopic intraparticle energy transfer
from the neutral inner part to the protonated surface. We
anticipate that our approach, based on the dye-concentrated
ORMOSIL nanoparticle, will provide a promising pathway to
near-physiological intracellular pH monitoring, due to its advan-
tages which include water dispersibility, biocompatibility, and
appropriate pKa, as well as two-photon activity. Further, the
surface silanol groups of ORMOSIL nanoparticles can be
modified for targeted delivery, without affecting the intrinsic
properties of sensor molecules.
Fig. 2 pH-dependent spectral evolution of the OSNP dispersion: one-
photon absorption (a) and PL (b, excited at 370 nm), and two-photon
excited PL (c, excited at 780 nm). (d) Ratiometric plots of fluorescence
intensities at 580 and 460 nm by one- (circle, excited at 370 nm) and two-
(triangle, excited at 780 nm) photon excitations. The solid lines are the
fitting results for experimental data by using Eqn. (1) in ESI{.
NVP monomer emission at 460 nm, suggesting the occurrence of
energy transfer within OSNP. It is noted that, due to a partial
overlap in Fig. 1a, only the shorter-wavelength side of the neutral
NVP emission is transferred to the protonated one and the longer-
wavelength energy is left, resulting in a red shift of the neutral
component. Moreover, by virtue of energy transfer, the emission
from the protonated NVP on the surface, in spite of there being a
minimal amount, exhibits amplified intensity, comparable to the
excess neutral component, validating our nanoparticle-based
design strategy for improving proton sensitivity. The similarity in
the excitation spectra below 400 nm for both emission components
(at 450 and 600 nm, respectively) is evidence of intraparticle energy
transfer, indicating protonated emission generated by neutral
excitation (Fig. S4 in ESI{). Overall, the NVP-concentrated OSNP
emits greenish mixed fluorescence even under neutral conditions,
between the neutral blue and the protonated yellow ones of the
NVP monomer.
This work was supported in part by a DURINT grant from the
Chemistry and Life Sciences Directorate of the Air Force Office of
Scientific Research and in part by the Post-doctoral Fellowship
Program of Korea Science & Engineering Foundation (KOSEF).
Notes and references
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The spectral evolution and the ratiometric behavior of OSNP
under one- and two-photon excitation are shown in Fig. 2. The
absorption and the emission spectra of OSNP show practically
instantaneous responses to the pH change. The pH-dependence of
the one-photon absorption in Fig. 2a displays a dual-absorption
behavior, typical of ratiometric probes, with an isosbestic point at
ca. 370 nm, indicating the ground-state conversion from neutral to
protonated species. Upon excitation at 370 nm, however, OSNP
emits no normal dual emission, but broad, single-peak fluorescence
at every experimental pH, which becomes narrower and red-
shifted with decreasing pH. This unusual behavior, different from
dual emission of the NVP monomer (Fig. S2 in ESI{), is attributed
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