Angewandte
Chemie
shows reasonable TPA efficiency in nonaqueous protic media,
Q’ has a low TPEF cross-section in water. In contrast,
dendrimers G1–G3 maintain a significant TPA cross-section
in water, thereby confirming that the dendritic branches
indeed isolate the chromophoric core, thus preventing
aggregation and PL quenching. Interestingly, the TPA char-
acteristics appear to increase slightly with increasing gener-
ation. This effect could be related to the slight increase of
local polarity at the core with increasing generation due to the
nature of the dendritic branches, which provide a somewhat
polar environment.[14] Recent calculations and experiments[15]
have shown that increasing solvent polarity, in a certain range,
can lead to TPA enhancement.
Our results demonstrate that water-soluble, luminescent
two-photon markers can be obtained by incorporating a
lipophilic two-photon chromophoric unit within shielding
layers built by a dendritic approach. This covalent layer-by-
layer approach allows us to modulate the solubility by varying
the nature of the peripheral groups while isolating the core TP
chromophore from deleterious effects. This route allows us to
overcome the drawbacks encountered when solubilizing
groups are grafted directly onto a TP chromophore and
provides a unique modular approach. In particular, replacing
the core unit by more efficient TP chromophores[3] and taking
advantage of the polar environment provided by the dendritic
environment should lead to more efficient TP tracers, while
further surface functionalization opens up a route for further
functionality (such as recognition or targeting). This strategy
can, in principle, be applied to various lipophilic chromo-
phores that show high TPA cross-sections and large fluores-
cence quantum yields as long as phenol moieties can be
grafted onto them, thus allowing for the building of the
dendritic sheath.
This is of particular interest for biological applications due
to the low toxicity detected for phosphorus-based dendrim-
ers.[16] This is a major advantage—in addition to the accessi-
bility for both inner and surface functionalization using
covalent chemistry—over semiconductor quantum dots
(QD). These inorganic nano-objects have gained a lot of
popularity as photonic imaging agents[17] but their toxicity is
still a main concern. Taking into account potential risks is one
of the most important issues in nanoscience. With this aim in
mind, we have demonstrated that the organic-nanodots route
can provide a promising alternative in terms of two-photon
brilliance,[18] and that it allows us to maintain excellent PL
properties while conveying water solubility, which leads to
water-soluble tracers that can indeed be used for in vivo
imaging (Figure 2). This is an important step that establishes
that organic nanodots definitely merit consideration as an
alternative to semiconductor QDs for two-photon imaging,
although further studies focusing on toxicity and (photo)-
stability are needed. In this respect, it is important to add that
in preliminary experiments we have found that polycationic
phosphorus dendrimers bearing the same ammonium end
groups are stable for months towards hydrolysis and that the
photostability of dendrimers G1 and G2 is significantly higher
than that of chromophore Q’ in water, thus indicating that this
strategy is also of interest in terms of photostability improve-
ment.
Figure 2. Two-photon imaging of the vascular network in the dorsal
part of the rat olfactory bulb. Vessels were labeled after injecting
intravenously a small bolus of 500 mm of dendrimer G2 in water. The
fluorescence was excited at 710 nm, epi-collected, and band-pass
filtered (440/40 nm). The image was taken at a depth of about
200 mm. No obvious toxic effects were observed during the experiment
(for technical details, see reference [19]).
Received: March 30, 2006
Published online: June 21, 2006
Keywords: chromophores · contrast agents · dendrimers ·
.
fluorescence · two-photon absorption
[1] W. Denk, J. H. Strickler, W. W. Webb, Science 1990, 248, 73 – 76.
[2] C. Xu, W. W. Webb, J. Opt. Soc. Am. B 1996, 13, 481– 491.
[3] a) S.-J. Chung, K.-S. Kim, T.-C Lin, G. S. He, J. Swiatkiewicz,
P. N. Prasad, J. Phys. Chem. B 1999, 103, 10741 – 10745; b) L.
Ventelon, L. Moreaux, J. Mertz, M. Blanchard-Desce, Chem.
Commun. 1999, 2055 – 2056; c) M. Rumi, J. E. Ehrlich, A. A.
Heikal, J. W. Perry, S. Barlow, Z.-Y. Hu, D. McCord-Maughon,
T. C. Parker, H. Rꢀckel, S. Thayumanavan, S. R. Marder, D.
Beljonne, J.-L. Brꢁdas, J. Am. Chem. Soc. 2000, 122, 9500 – 9510;
d) B. R. Cho, K. H. Son, S. H. Lee, Y.-S. Song, Y.-K. Lee, S.-J.
Jeon, J. H. Choi, H. Lee, M. Cho, J. Am. Chem. Soc. 2001, 123,
10039 – 10045; e) O. Mongin, L. Porrꢂs, L. Moreaux, J. Mertz, M.
Blanchard-Desce, Org. Lett. 2002, 4, 719 – 722; f) W. J. Yang,
D. Y. Kim, C. H. Kim, M.-Y. Jeong, S. K. Lee, S.-J. Jeon, B. R.
Cho, Org. Lett. 2004, 6, 1389 – 1392; g) L. Porres, O. Mongin, C.
Katan, M. Charlot, T. Pons, J. Mertz, M. Blanchard-Desce, Org.
Lett. 2004, 6, 47 – 50; h) C. Le Droumaguet, O. Mongin, M. H. V.
Werts, M. Blanchard-Desce, Chem. Commun. 2005, 2802 – 2804.
[4] L. Ventelon, S. Charier, L. Moreaux, J. Mertz, M. Blanchard-
Desce, Angew. Chem. 2001, 113, 2156 – 2159; Angew. Chem. Int.
Ed. 2001, 40, 2098 – 2101.
[5] M. H. V. Werts, S. Gmouh, O. Mongin, T. Pons, M. Blanchard-
Desce, J. Am. Chem. Soc. 2004, 126, 16294 – 16295.
[6] M. Blanchard-Desce, C. R. Phys. 2002, 3, 439 – 448.
[7] H. Y. Woo, J. W. Hong, B. Liu, A. Mikhailovsky, D. Korystov,
G. C. Bazan, J. Am. Chem. Soc. 2005, 127, 820 – 821.
[8] J. Leclaire, Y. Coppel, A.-M. Caminade, J.-P. Majoral, J. Am.
Chem. Soc. 2004, 126, 2304 – 2305.
[9] TPEF measurements were performed by excitation with 150-fs
pulses from a Ti:sapphire laser, using the protocol of Xu and
Webb,[2] taking into account refractive index effects.[10]
Angew. Chem. Int. Ed. 2006, 45, 4645 –4648
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