1408
X. He et al.
Steck and Day,[12] cptcp and btcpc were synthesised by cou-
pling 1,10-phenanthroline-5,6-dione with 4-carbazol-9-yl-
benzaldehyde and 9-butyl-9H-carbazole-3,6-dicarbaldehyde,
respectively. Using a mixture of water and ethanol as solvent,
Ru1 and Ru2 were prepared by direct reaction of the precursor
complex cis-[Ru(phen)2Cl2]ꢀ2H2O with the appropriate mole
ratios of cptcp and btcpc, and were obtained in yields of 67 and
62 %, respectively. The desired RuII complexes were isolated as
their perchlorates and then purified by column chromatography
to afford satisfactory purity, which was verified by elemental
analysis, matrix-assisted laser desorption ionisation time-of-
flight (MALDI-ToF) mass spectrometry (Fig. S1 in the Sup-
plementary Material), and NMR spectroscopy (Fig. S2 in the
Supplementary Material).
The absorption spectra of Ru1 and Ru2 (Fig. S3 in the
Supplementary Material) in acetonitrile are very similar and
consist of three well resolved bands at ,460, 350, and 264 nm.
The bands at ,350 and 264 nm are attributed to intraligand (IL)
p - p* transitions.[13] The lowest energy band, at ,460 nm, is
assigned to a metal–ligand charge transfer (MLCT) transition,
which is attributed to Ru(dp) - cptcp or btcpc (p*) transitions.
In comparison to the spectra of other polypyridyl RuII
complexes, such as [Ru(phen)3]2þ (lmax 448 nm),[13] [Ru
(bpy)2(ip)]2þ (lmax 455 nm), [Ru(bpy)2(pip)]2þ (lmax 458 nm)
(where bpy ¼ 2,20-bipyridine, ip ¼ imidazo[4,5-f] [1,10]-
1.0
0.8
0.6
0.4
0.2
0
0.75
0.60
0.45
0.30
0.15
0
0
0.6 1.2 1.8 2.4 3.0 3.6 4.2
[DNA] ꢁ 105
250
300
350
400
450
500
550
600
Wavelength [nm]
1.0
0.8
0.6
0.4
0.2
0
1.50
1.25
1.00
0.75
0.50
0.25
0
phenanthroline,
and
pip ¼ 2-phenylimidazo[4,5-f]1,10-
0
0.5 1.0 1.5 2.0 2.5 3.0 3.5
phenanthroline),[14] the MLCT bands of Ru1 and Ru2 are
obviously red shifted, which may be due to the increased p
delocalisation and, thus, the p-acceptor capacity of the ligands
btcpc and cptcp, resulting in a decreased electron density on the
central RuII and, in turn, stabilisation of the metal dp orbital.
Complexes Ru1 and Ru2, upon dissolution in various
solvents, such as acetonitrile and water, could emit lumines-
cence in the absence of DNA at 258C. As shown in Fig. S4 in
the Supplementary Material, Ru1 and Ru2 showed emission
in acetonitrile with a maximum appearing at 597 and 585 nm,
respectively. Note that distinct red shifts around 12 nm were
observed for Ru1 and Ru2 in aqueous solution. In addition,
the emission spectra of Ru1 and Ru2 are somewhat solvato-
chromic, reflecting that the more polar the solvent, the smaller
the relative intensity.[15,16]
[DNA] ꢁ 105
250
300
350
400
450
500
550
600
Wavelength [nm]
Fig. 2. Absorption spectra of Ru1 (top) and Ru2 (bottom) in Tris–HCl
buffer upon addition of calf thymus (CT)-DNA. [Ru1] ¼ 10 mM, [Ru2] ¼
20 mM, [DNA] ¼ 0–34 mM. Arrow shows the absorbance changing upon the
increase of DNA concentration. Inserts: plots of (ea ꢃ ef)/(eb ꢃ ef) v. [DNA]
for the titration of DNA to complexes Ru1 and Ru2. ea, ef and eb are the
apparent, free, and bound metal complex extinction coefficients,
respectively.
Electronic Absorption Titration
The application of electronic absorption spectroscopy in DNA-
binding studies is one of the most useful techniques.[17] Upon
gradual addition of DNA, the electronic absorption spectros-
copy of the complex is perturbed due to the stacking interactions
between the aromatic chromophore of the intercalative ligand in
the complex and the base pairs of DNA. Therefore, binding of
the complex to DNA by intercalation usually results in hypo-
chromism and bathochromism. In general, the extent of the
hypochromism commonly parallels the intercalative binding
strength. The absorption spectra of Ru1 and Ru2 in the absence
and presence of calf thymus (CT)-DNA are given in Fig. 2. As
the concentrations of DNA are increased to saturation, for Ru1,
the hypochromism at 351 nm reaches as high as 14.1 % with
a red shift of 4 nm at a [DNA]/[Ru] ratio of 2.31; for Ru2, the
hypochromism at 367 nm reaches ,9.8 % with a red shift of
2 nm at a [DNA]/[Ru] ratio of 3.55. These spectroscopic char-
acteristics obviously suggest that both complexes can interact
with DNA, which most likely proceeds through a mode that
involves a stacking interaction between the aromatic chromo-
phore and the base pairs of DNA.
From the decrease of the absorbance of both complexes
(at 351 nm for Ru1 and 367 nm for Ru2), the intrinsic binding
constants Kb of Ru1 and Ru2 to DNA were determined as
(6.8 ꢁ 0.45) ꢂ 106 Mꢃ1 (s ¼ 0.67 ꢁ 0.15), and (4.61 ꢁ 0.22) ꢂ
106 Mꢃ1 (s ¼ 0.53 ꢁ 0.12), respectively. The Kb values of
the two complexes are comparable to that of [Ru
(bpy)2(pip)]2þ [14]
,
[Ru(bpy)2(ppd)]2þ (where ppd ¼ pteridino
[7,6-f][1,10]phenanthroline-1,13(10H,12H)-dione),[16] and the
known DNA intercalator ethidium bromide (EB).[18] However,
the Kb values of Ru1 and Ru2 are stronger than their parent
complexes, [Ru(bpy)3]2þ (4.7 ꢂ 103 Mꢃ1) and [Ru(phen)3]2þ
(5.4 ꢂ 103 Mꢃ1).[19] These data indicate that the size and the
shape of the intercalated ligand of the RuII complexes have a
significant effect on the strength of DNA binding, and the most
suitable intercalating ligand leads to the highest affinity of
complexes with DNA. Although the hydrophobicity of the
intercalative ligand in Ru2 is greater than that in Ru1, the steric
hindrance caused by a normal-butyl group is not advantageous
to the DNA-binding of Ru2, resulting in a lower DNA-binding
affinity. Therefore, synthetically considering these factors, the