C O M M U N I C A T I O N S
2
+
a d orbital of similar energy on Cu , where the absorbed energy
nonradiatively dissipates. The higher energy of the d orbitals in
supports our model of fluorescence enhancement synchronized with
radioactive decay. This new method of monitoring fluorescence
enhancement through the decay of radionuclides has a variety of
potential applications. For example, it may open new possibilities
for studying fundamental molecular transformations, such as
determining how quickly a molecule readjusts from one state to
another after radioactive decay. Furthermore, combining radionu-
clide decay with fluorescence enhancement could provide a unique
complementary signaling mechanism for radionuclear-optical
multimodal biological imaging. In fact, the new radiolabeled LS479
represents a paradigm-shifting strategy in multimodal molecular
2+
Ni compared with the π* orbitals precludes this transfer, allowing
the fluorescence of LS479 to occur naturally via a π* f π
transition. Indeed, the absorbance maximum in the visible spectra
2+
of Cu -DTPA was 740 nm, while that for Ni-DTPA was at a
shorter wavelength, 610 nm. A similar mechanism of quenching
might occur in porphyrin, which in its free form emits at ∼600 nm
but for which both Cu2 and Ni cause fluorescence quenching.
+
2+
15
6
4
2+
imaging because Cu and near-infrared fluorescent dyes such as
1
7
LS479 are routinely used in positron emission tomography and
1
8
optical imaging of living organisms, respectively. Moreover, the
strong correlation between fluorescence quenching and the presence
6
4
2+
of Cu chelation provides a dynamic method for studying the in
vivo stability of the radionuclide chelates, where fluorescence
enhancement reports demetalation of the radionuclide. Finally, the
new molecular construct and mechanism could be used to develop
visible radioactivity decay devices for environmental and nuclear
forensic applications. Future work will focus on these potential
applications.
Figure 3. Percent changes in 64Cu2+ concentration as a result of decay
calculated from exponential decay) and in relative fluorescence of Cu-
LS479 solution as a function of time. Unquenched LS479 (0.5 µM)
corresponded to a hypothetical zero-time point for fluorescence. Relative
fluorescence was measured as an area under the emission curve after addition
(
Acknowledgment. This study was support in part by the NIH
extramural grants R01 CA109754, R33 CA123537, R33 CA100972,
U54 CA136398, and U54 CA119342, the NIH Roadmap for
Medical Research as the funding source for the IPDC, and the
Intramural Research Program of Eunice Shriver NICHD.
64
of Cu solution divided by the area before the addition (λex ) 675 nm).
An overall increase in fluorescence intensity was seen as a function of time.
Supporting Information Available: Synthesis, experimental pro-
cedures, calculations, and optical spectra. This material is available
free of charge via the Internet at http://pubs.acs.org.
References
(
(
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(
(
Figure 4. Normalized emission of LS479 (λex ) 690 nm) and absorption
2+
2+
2+
spectra of Cu -DTPA, and Ni -DTPA and Zn -DTPA (the absorption
maximum for the Zn2 -DTPA complex was <450 nm). Substantial overlap
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+
1
28, 10.
(7) Chen, Y.; Rosenzweig, Z. Anal. Chem. 2002, 74, 5132.
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The fluorescence enhancement of LS479 observed upon com-
plexation with Zn suggests that the lack of a vacant d orbital
precludes ligand-to-metal charge transfer and the absence of
absorption bands prevents energy transfer. A distinguishing char-
acteristic of LS479 compared with HITC is the presence of a lone
electron pair on the conjugated amine group. Lone electron pairs
typically act as highly efficient fluorescence quenchers via an
2
223.
(11) Meallet-Renault, R.; Herault, A.; Vachon, J. J.; Pansu, R. B.; Amigoni-
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(
(
(
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1
6
(15) Dolphin, D., The Porphyrins; Academic Press: New York, 1978; Vol. 3, p
excited-state charge transfer (ESCT) mechanism. Indeed, the
quantum yield of LS479 (Φ ) 0.018) in unbuffered water was ∼6
times smaller than that of HITC (Φ ) 0.11). In addition, the
fluorescence lifetime of LS479 (τ ) 0.35 ns) was shorter than that
of HITC (τ ) 0.41 ns), further indicating the presence of a
fluorescence quenching process.
5
71.
(16) Atwood, J. L.; Steed, J. W. Encyclopedia of Supramolecular Chemistry;
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(
17) Anderson, C. J.; Connett, J. M.; Schwarz, S. W.; Rocque, P. A.; Guo, L. W.;
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1
992, 33, 1685.
(
18) Citrin, D.; Lee, A. K.; Scott, T.; Sproull, M.; Menard, C.; Tofilon, P. J.;
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The addition of 64CuCl
The net fluorescence enhancement upon Cu decay strongly
also resulted in fluorescence quenching.
2
64
2+
JA903685B
9
200 J. AM. CHEM. SOC. 9 VOL. 131, NO. 26, 2009