6382 Organometallics, Vol. 29, No. 23, 2010
Tong et al.
Table 2. Calculated log K for 1 and 2 with Thiol Substrates (1:1
binding) in Aerated 8:2 DMF/Tris Buffer (pH 7.2)
human diseases such as neurotoxicity, growth problems,
and cardiovascular and Alzheimer’s diseases.27
thiol substrate
1
2
Summary
cysteine
homocysteine
1-octanethiol
log K = 4.90 ( 0.01
log K = 3.65 ( 0.06
log K = 2.93 ( 0.03
log K = 3.80 ( 0.07
log K = 3.42 ( 0.11
log K = 2.94 ( 0.03
Compared with our recent report employing terpyridine-
Pt(II) moieties, the present work describes a host system
containing the highly emissive [N,C,N-Pt(II)] luminophore.
The new complexes have been fully characterized, and their
photophysical properties and potential to act as selective
phosphorescent probes have been investigated. By utilizing
the known propensity for terminal thiols to coordinate to
Pt(II), we have integrated the [N,C,N-Pt(II)] and carboxylate
binding sites to afford a crowded molecular framework that
displays unusual preferential binding for Cys over Hcy, while
no binding is detected for methionine. In this regard, the
preorganized, shape-persistent binding pocket maintained by
the rigid xanthene backbone undoubtedly plays a critical role in
differentiating the thiol-containing species, and the enhanced
binding with Cys is attributed to the superior ditopic spatial
fit and greater complementarity. Insight into the nature of
the host-guest interaction has also been obtained from the
binding behavior of the ester congener. While we are not
advocating this system as a practical sensor for distinguishing
biological thiols (the sensing media are not biocompatible),
we consider that the development of this design approach,
based on congested ditopic hosts bearing responsive phos-
phorescent reporting units, is worthwhile.
and 2, and the above Coulombic argument is again invoked
to rationalize the significantly higher log K for 1, as predicted
by the DFT calculations described above.
Previously reported luminescent and colorimetric probes
for biological thiols are often nondiscriminating,23,24 or
selectivity for Hcy over Cys is obtained (due to steric
reasons).25 Indeed, sensors capable of Cys-over-Hcy selec-
tivity are rare.26 In this context, the noticeably higher log K
for the binding of 1 to Cys compared with Hcy is intriguing.
Even though the selectivity for Cys over Hcy (KCys/KHcy
=
17.8) is modest, we suggest that the binding cavity in 1
affords a superior ditopic spatial fit and enhanced comple-
mentarity for the shorter Cys. Hence, we consider the pre-
ferential binding of 1 to the more sterically hindered Cys over
Hcy to be the initial realization of the crowded ditopic
phosphorescent host concept postulated in this work. The
selective recognition of biomolecules and their structural
motifs is appealing for, inter alia, probing biological path-
ways and designing new therapeutic agents. The detection of
Cys and Hcy is important because abnormal levels of these
biological thiols are associated with a wide spectrum of
Experimental Section
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Jiang, S.; Warner, I. M.; Dawan, F. B.; Lian, K.; Strongin, R. M. J. Am.
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M.; Gao, Y.; Li, L.; Liu, Z.; Zhang, J.; Zhang, D.; Yi, T.; Huang, C. J. Am.
Chem. Soc. 2007, 129, 10322. (f) Sreejith, S.; Divya, K. P.; Ajayaghosh, A.
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T. M.; Weissleder, R.; Hilderbrand, S. A. Org. Lett. 2008, 10, 37. (h) Lee,
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W.; Yuan, L.; Cao, Z.; Feng, Y.; Long, L. Chem.;Eur. J. 2009, 15, 5096. (j)
Yao, Z.; Feng, X.; Li, C.; Shi, G. Chem. Commun. 2009, 5886. (k) Huo, F.-J.;
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(l) Shao, N.; Jin, J.; Wang, H.; Zheng, J.; Yang, R.; Chan, W. H.; Abliz, Z. J. Am.
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Zhong, X.; Zhao, C.; Zhu, L. Chem. Commun. 2010, 46, 2971.
(24) Phosphorescent examples: (a) Chow, C.-F.; Chiu, B. K.-W.;
Lam, M. H.-W.; Wong, W.-Y. J. Am. Chem. Soc. 2003, 125, 7802. (b)
Huang, K.; Yang, H.; Zhou, Z.; Chen, H.; Li, F.; Yi, T.; Huang, C. Inorg.
Chim. Acta 2009, 362, 2577.
(25) For example: (a) Wang, W.; Escobedo, J. O.; Lawrence, C. M.;
Strongin, R. M. J. Am. Chem. Soc. 2004, 126, 3400. (b) Lee, K.-S.; Kim,
T.-K.; Lee, J. H.; Kim, H.-J.; Hong, J.-I. Chem. Commun. 2008, 6173. (c)
Shiu, H.-Y.; Chong, H.-C.; Leung, Y.-C.; Wong, M.-K.; Che, C.-M. Chem.;
Eur. J. 2010, 16, 3308. Phosphorescent: (d) Chen, H.; Zhao, Q.; Wu, Y.; Li,
F.; Yang, H.; Yi, T.; Huang, C. Inorg. Chem. 2007, 46, 11075.
(26) Colorimetric: (a) Han, M. S.; Kim, D. H. Tetrahedron 2004, 60,
11251. (b) Wang, W.; Rusin, O.; Xu, X.; Kim, K. K.; Escobedo, J. O.;
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Sun, S.; Sun, P.; Peng, X. Chem. Commun. 2009, 5904. Circular dichroism
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General Considerations. All reactions were performed under a
nitrogen atmosphere, and solvents for syntheses (analytical
grade) were used without further purification. Solvents for
photophysical measurements were purified according to con-
ventional methods. 1H NMR spectra were obtained on a Bruker
DRX 400 FT-NMR spectrometer (ppm) using Me4Si as internal
standard. ESI mass spectra were measured on a Perkin-Elmer
Sciex API 150EX mass spectrometer. IR spectra were recorded
on a Perkin-Elmer 1600 series FT-IR spectrophotometer. Ele-
mental analyses were performed on an Elementar Analysensys-
teme GmbH Vario EL elemental analyzer.
Photophysical Measurements. UV-vis absorption spectra
were obtained on an Agilent 8453 diode array spectrophot-
ometer. Steady-state emission spectra were recorded on a SPEX
FluoroLog 3-TCSPC spectrophotometer equipped with a Ha-
mamatsu R928 PMT detector, and emission lifetime measure-
ments were conducted using NanoLed sources in the fast MCS
mode and checked using the TCSPC mode. Low-temperature
(77 K) emission spectra for glasses and solid-state samples were
recorded in 5 mm diameter quartz tubes, which were placed in a
liquid nitrogen Dewar equipped with quartz windows. Unless
otherwise stated, 298 K emission spectra were recorded using
aerated solutions. The emission quantum yield was measured28
by using [Ru(bpy)3](PF6)2 in degassed acetonitrile as the stan-
dard (Φr = 0.062) and calculated by Φs = Φr(Br/Bs)(ns/nr)2(Ds/
Dr), where the subscripts s and r refer to sample and reference
standard solution respectively, n is the refractive index of the
solvents, D is the integrated intensity, and Φ is the luminescence
quantum yield; sample and standard solutions for this pur-
pose were degassed with at least three freeze-pump-thaw
cycles. The quantity B is calculated by the equation B = 1 - 10-AL
,
where A is the absorbance at the excitation wavelength and L is
the optical path length. Errors for λ ((1 nm), τ ((10%), and
Φ ((10%) are estimated. For the UV-vis absorption and emission
(28) Demas, J. N.; Crosby, G. A. J. Phys. Chem. 1971, 75, 991.