Table 3 Absorption and photophysical properties of complexes 4a-f
Entry
l4
labs (loge)/nma
l
em/nmb
l
em/nma (t/ns)
l
em/nma (t/ns)
(f)a,g
1
2
3
4
5
6
a
b
c
d
e
f
325 (4.37), 390 (4.03)
322 (4.40), 392 (3.96)
328 (4.32), 388 (4.06)
392 (4.18), 486 (3.86)
390 (4.20), 490 (3.78)
394 (4.14), 484 (3.90)
584
625
512
590
615
627
410c (2.7)
402c (2.5)
398c (1.6)
540d (3.9)
539d (3.1)
524d (6.9)
520e (1.6)
510e (2.6)
512e (7.2)
604f (6.5)
618f (7.6)
612f (< 1)
0.24
0.2
0.28
0.05
0.01
0.08
a aerated CHCl3 solution; b solid; c lex = 320 nm; d lex = 390 nm; e lex = 390 nm; f lex = 500 nm; g obtained for LLCT emission.
the microwave-assisted complexation of cyanobipyridine 3a-b,
a thiophenol and Zn(OAc)2 using a passive heating element.
The complexes display LLCT fluorescence in the solid-state,
but tunable dual emission in chloroform, arising from co-
emissive excited states. In general, the luminescence from the
complexes can be tuned through changes in bipyridine function-
ality and subtly modulated by changes in the ancillary thiolate
co-ligands.
We thank EPSRC for funding together with Cardiff University,
Professor C. Oliver Kappe for helpful discussions and Steve Singh
at Anton Paar Ltd (Hertford, UK) for the provision of the SiC
passive heating elements.
Fig. 3 Main: Emission profiles for 4a in CHCl3 (lex = 330 (blue), 350
(pink), 370 (yellow), 390 (turquoise), 400 (purple) and 410 (brown) nm.
Inset: excitation spectra for 4a lem = 410 nm (grey) and 520 nm (black).
Notes and references
1 (a) D. R. Kanis, M. A. Ratner and T. J. Marks, Chem. Rev., 1994, 94,
195; (b) M. M. M. Raposo, A. M. R. C. Sousa, G. Kirsch, P. Cardoso,
M. Belsley, E. D-, M. Gomes and A. M. C. Fonseca, Org. Lett., 2006,
8, 3681.
2 (a) A. D’Aleo, G. Pompidor, B. Elena, J. Vicat, P. L. Baldeck, L. Toupet,
R. Kahn, C. Andraud and O. Mauryr, ChemPhysChem, 2007, 8, 2125;
(b) J. H. Yu, D. Parker, R. Pal, R. A. Poole and M. J. Cann, J. Am.
Chem. Soc., 2006, 128, 2294.
3 M. C. Bagley, Z. Lin and S. J. A. Pope, Chem. Commun., 2009, 5165.
4 M. C. Bagley, Z. Lin and S. J. A. Pope, Tetrahedron Lett., 2009, 50,
6818.
5 (a) V. P. Rao, A. K-, Y. Jen and J. B. Caldwell, Tetrahedron Lett., 1994,
35, 3849; (b) A. Facchetti, L. Beverina, M. E. Van-der Boom, E. G.
Dutta, G. A. Pagani and T. J. Marks, J. Am. Chem. Soc., 2006, 128,
2142; and references cited therein.
6 Z. R. Grabowski, K. Rotkiewicz and W. Rettig, Chem. Rev., 2003, 103,
3899.
7 B. C. Thompson, K. A. About, J. R. Reynolds, K. Nakatani and
P. Audebert, New J. Chem., 2005, 29, 1128.
8 (a) S. Caddick and R. Fitzmaurice, Tetrahedron, 2009, 65, 3325; (b) C. O.
Kappe, Chem. Soc. Rev., 2008, 37, 1127; (c) C. O. Kappe, Angew. Chem.,
Int. Ed., 2004, 43, 6250; (d) C. O. Kappe, A. Stadler, Microwaves in
Organic and Medicinal ChemistryWiley-VCH: Weinheim, 2005.
9 P. Nilsson, K. Olofsson and M. Larhed, Top. Curr. Chem., 2006, 266,
103.
10 A. L. K. Shi Shun, E. T. Chernick, S. Eisler and R. R. Tykwinski,
J. Org. Chem., 2003, 68, 1339.
11 D. Venkataraman, R. K. Gujadhur and C. G. Bates, Org. Lett., 2001,
3, 4315.
associated with a unique excitation peak at ca. 400 nm, consistent
with the LLCT assignment in the corresponding absorption
spectra. Similar observations were noted for compounds 4d-f,
although with notable red-shifts in all cases. Time-resolved
luminescence lifetime measurements showed that each of the
emission peaks were relatively short-lived (< 10 ns) and indicative
of a fluorescence in each case, whilst the quantum yields of the low
energy emissions are significantly reduced for 4d-f.
Taken together with the data obtained for the corresponding free
ligands 3a-b, and the solid-state fluorescence (assigned to a LLCT
emitting state), these results indicate that the longer wavelength
emission in chloroform solution can again be attributed to the
LLCT excited state, but that the shorter wavelength band probably
arises from an intra-ligand charge transfer (ILCT) associated with
the cyanobipyridine. In this context, the extent of restricted motion
of the coordinated thiol can be invoked to explain disparities in
single (LLCT) or dual emission.20
The solvatochromic behaviour of 4f was probed and revealed
that the emission in acetonitrile (lem = 573 nm) and DMSO
(lem = 593 nm) was independent of excitation wavelength (390,
450 or 500 nm). A comparison with the free ligand 3b (lem
=
12 (a) T. J. Anderson, J. R. Scott, F. Millett and B. Durham, Inorg. Chem.,
2006, 45, 3843; (b) Y. Sun, M. L. Machala and F. N. Castellano, Inorg.
Chim. Acta, 2010, 363, 283; and references cited therein.
13 D. L. Greene and D. M. P. Mingos, Transition Met. Chem., 1991, 16,
71.
576 nm (MeCN); 580 nm (DMSO)) suggests that in polar
solvent the red-shifted emission of 4f is likely to be domi-
nated by (Zn(II)-perturbed) IL(bpy)CT character. This observation
is consistent with our previous studies into solvatochromic
cyanopyridines3 and related reports in the literature into classical
N,N-dimethylaminobenzonitrile (DMABN) species.6
´
14 A. De la Hoz, A. D´ıaz-Ortiz and A. Moreno, Chem. Soc. Rev., 2005,
34, 164.
15 For the use of passive heating elements in microwave-assisted organic
synthesis, see reference 16 and the following: (a) R. Hoogenboom,
T. F. A. Wilms, T. Erdmenger and U. S. Schubert, Aust. J. Chem., 2009,
In conclusion, a series of cyanobipyridine-derived Zn(II) bisthi-
olate complexes can be prepared rapidly and in high yield by
This journal is
The Royal Society of Chemistry 2010
Dalton Trans., 2010, 39, 3163–3166 | 3165
©