C O M M U N I C A T I O N S
photophysics of metallodipyrrins, suggesting rational pathways to
fluorogenic dipyrrin-based chelators. These results open up pos-
sibilities for engaging metallodipyrrins in a variety of applications,
including construction of luminescent networks, electrooptical
materials, and biomedical imaging and sensing.
Acknowledgment. This work was supported by Grant 10-03-
01122a from RFBR and Grant EB007279 from NIH. S.A.V. is
grateful to Prof. R. M. Hochstrasser and Dr. L. E. Sinks for
invaluable discussions.
Supporting Information Available: Synthetic procedures, spec-
troscopic data, fluorescence lifetime data, and crystallographic data
(CIF). This material is available free of charge via the Internet at http://
pubs.acs.org.
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Figure 3. X-ray crystal structure (ORTEP) of the homoleptic Zn-2e
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solvation of the mono and bis complexes. The ratio of the oscillator
strengths (ML2 vs MLX) was found to be 1.92, which is very close
to the value predicted by the theory (2.0).9 Fast nonradiative
relaxation from the upper to the lower exciton state and slow
emission from the latter, consistent with the low oscillator strength
of the corresponding excitation, make intersystem crossing and
internal conversion the most likely causes for the loss of fluores-
cence in ML2. In toluene at 22 °C, ML2 exhibits a broad emission
(λmax ) 785 nm) with a negligible quantum yield (φfl < 0.01) and
an average lifetime of ∼1.6 ns (Figure S15).
The strong coupling of the transition dipoles suggests that the
mutual orientation of the dipyrrin units in ML2 deviates from strictly
orthogonal (D2h symmetry). The X-ray crystal structure (CCDC no.
749261) of ML2 complex Zn-2e (Figure 3) fully corroborates this
assumption. The angle between the mean-square planes of the
dipyrrins in Zn-2e is only 64.5°, which is smaller than that found
in the majority of known Zn-dipyrrin complexes.21 Similarly
flattened structures have been observed in Zn azadipyrrins
(63-39°)22 and Zn R-methoxydipyrrin (54.7°).23 Also noteworthy
is the quite significant ruffling of the dipyrrin ligands, which
resembles distortions of some nonplanar porphyrins.24
Notably, the computed structure [DFT/B3LYP/6-31G(d)] of
homoleptic Zn-2e (Figure 2c) was also found to be nonorthogonal,
although the angle between the mean-square planes was somewhat
larger (77°). This suggests that the distortion from the orthogonal
geometry is not induced by the crystal packing forces but is an
intrinsic property of the ML2 molecule, which is flattened because
of the propensity of the ligand π systems to align in coplanar
fashion.22 The nonorthogonal geometry may also facilitate interac-
tions between the metal and the proximate carbonyl oxygens, which
have been identified in some other homoleptic dipyrrin
complexes.19b Although the Zn-O distances in Zn-2e are quite
large (dZn-O ) 2.8-2.9 Å vs dZn-N ) 2.0 Å), the carbonyl groups
still could be implicated in the overall ligand-metal bond stabiliza-
tion.19
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Johansson, L. B. A. J. Am. Chem. Soc. 2002, 124, 196. (b) Tleugabulova,
D.; Zhang, Z.; Brennan, J. D. J. Phys. Chem. B 2002, 106, 13133.
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2008, 47, 766.
(22) Teets, T. S.; Partyka, D. V.; Updegraff, J. B.; Gray, T. G. Inorg. Chem.
2008, 47, 2338.
(23) Halper, S. R.; Stork, J. R.; Cohen, S. M. Dalton Trans. 2007, 1067.
(24) Senge, M. O. In The Porphyrin Handbook; Kadish, K. M., Smith, K. M.,
Guilard, R., Eds.; Academic Press: New York, 2000; Chapter 6.
In conclusion, the developed method of synthesis of fluorogenic
π-extended dipyrrins allows tuning of their optical bands across
the red/near-IR optical spectrum. Metal complexes of π-extended
metallodipyrrins are strongly fluorescent, and their fluorescence can
be switched on and off by changing the mode of metal coordination.
The molecular exciton theory9 provides a new insight into the
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