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trans-[Pt2Cl4(DMSO)2(LR)] (R = H for 1, R = F for 2), were
fully characterized, and the structure of open 2 was obtained
by single-crystal X-ray diffraction (see the Supporting Infor-
mation).
observed, especially for the closed complexes. The data
obtained thus show that the coordination compounds do
interact with the biomolecule, and most importantly, that
their open/closed forms exhibit drastically distinct behaviors.
The affinity of the compounds for DNA has been
evaluated and compared using the Stern–Volmer quenching
constant, KSV, by applying Equation (1).
A representation of the molecular structure of 2 is
depicted in Figure 1b. Crystallographic data, and selected
bond lengths, and angles are summarized in Tables S1 and S2
in the Supporting Information. As expected, 2 is a dinuclear
platinum(II) compound with two symmetry-related metal
centers, which exhibit a slightly distorted square-planar
geometry. It is notable that while the platinum precursor
has a cis configuration, the two metal ions in 2 display
a trans configuration. Such cis-to-trans isomerization has been
observed, and is due to the trans effect of S-bonded dimethyl
sulfoxide ligands.[16] The Pt–N, Pt–Cl, and Pt–S bond lengths
(see Table S2) are in normal ranges.[17] The slight distortion of
the square plane likely arises from steric hindrance induced
by the DMSO methyl groups. The analytical data for 1 suggest
that its structure is analogous to that of 2.
I0
I
ð1Þ
¼ 1 þ KSV ½complexꢀ
Herein, I0 and I are the emission intensities without and with
complex, respectively. A plot of I0/I vs. [complex] will give
a straight line whose slope is equal to KSV. The corresponding
plots for 1 and 2 (open/closed forms) are depicted in
Figure S4. The compound 1 displays a slightly better DNA
affinity than 2, with KSV = 6.6 ꢀ 103 ꢁ 0.8mꢂ1 (logKSV = 3.82)
for 1, while it is 4.8 ꢀ 103 ꢁ 0.9mꢂ1 (logKSV = 3.68) for 2. This
difference may be due to the fluorinated cyclopentenyl ring of
LF, whose fluorine atoms may induce unfavorable electro-
static repulsion with the phosphate backbone of the double
helix.[20] The most striking and important feature is the
significantly different behaviors of the open and closed forms
of both complexes; the KSV value for closed 1* is 42.5 ꢀ 103 ꢁ
0.6mꢂ1 (logKSV = 4.63), which is 6.5 times higher than that for
The switching properties of LH and LF, and the platinum
complexes 1 and 2, have next been examined by UV/Vis
spectroscopy. The corresponding spectra are shown in Figur-
es S1 (LH and LF), S2 (1), and S3 (2). Before UV irradiation at
l = 365 nm, strong absorption bands are observed below l =
400 nm (l = 230, 285 and 323 nm for LH; and l = 265, 275 and
300 nm for LF), and are due to p–p* transitions of the open
form of the ligands. Upon irradiation with UV light, two new
absorption bands are observed at l = 378 and 550 nm for LH,
and l = 381 and 592 nm for LF. These are ascribed to p–p*
transitions of the closed form of the ligands.[18] Upon
coordination to platinum, the p–p* transitions of both ligands
are red shifted. The solution (in dichloromethane) UV/Vis
spectrum of closed 1, that is 1*, exhibits characteristic p–p*
transition bands at l = 412 and 622 nm (Figure S2), and that
of 2* at l = 404 and 627 nm (Figure S3). Upon irradiation with
visible light, the initial spectra are recovered for 1 and 2 (as
for LH and LF), therefore indicating that the photocyclization
process is reversible. The stability of the closed forms of the
two coordination compounds has been also evaluated by UV/
Vis spectroscopy. Thus, solutions of 1 and 2 in CH2Cl2 have
been kept both in daylight and in the dark for 24 hours. UV/
Vis spectra have been subsequently recorded (Figures S2 and
S3), and show that the closed complexes are stable in the
absence of light. In contrast, in daylight, a clear decrease of
the p–p* transition bands of the closed compounds is
observed as a result of the partial opening of the coordinated
ligands LH and LF. The stability of the closed metal complexes
in the dark is of paramount importance regarding the study of
their potential DNA-interacting and cytotoxicity properties.
The potential interactions between DNA and the open/
closed forms of 1 and 2 have been investigated by fluores-
cence spectroscopy. Competitive binding studies using ethid-
ium bromide (EB) bound to calf thymus DNA (ct-DNA) have
been carried out. Displacement of EB from the fluorescent
EB-DNA adduct by a DNA-interacting molecule will induce
fluorescence quenching.[19] Fluorescence spectra have been
recorded at constant [ct-DNA] and [EB] (15 and 75 mm,
respectively), and using increasing amounts of 1 and 2 (in the
range 1–-25 mm). A clear decrease in emission intensity is
open 1. An analogous behavior is observed for 2* with KSV
=
26.8 ꢀ 103 ꢁ 0.9mꢂ1 (logKSV = 4.43), which is about 5.5 times
the value obtained for 2.
The greater interaction of the closed complexes with
duplex DNA may be explained structurally. The X-ray
structure of 2* could not be obtained, however, the structures
of the open/closed forms of one of the simplest members of
the 1,2-dithienylethene family, namely 1,2-bis[2,5-dimethyl(3-
thienyl)]-perfluorocyclopentene have been reported (see
Figure S5).[21] The open form is distinctly more voluminous
than the closed one (about 12% longer and 25% wider), and
the molecule is clearly more planar upon ring closure, with
a greater p conjugation. Consequently, it may be reasonable
to expect that the 1* and 2* will have an increased proficiency
to expel EB, owing to a sterically favored interaction with
DNA. Furthermore, the electronic changes taking place upon
ring closure will modify the coordination properties of the
ligand, and therefore affect the metal center (which may
modulate its DNA-binding properties).
It should be mentioned here that analogous studies with
the free ligands LH and LF could not be performed, since they
are not soluble in aqueous media or even buffer solutions
containing up to 10% DMSO. Therefore, the involvement of
the metal ions is crucial and the mechanism of action (of the
DNA interaction) is currently being investigated.
The interaction of the photoisomeric forms of 1 and 2 with
DNA has then been studied by agarose gel electrophoresis.
Electrophoretic-mobility measurements with pBR322 plas-
mid DNA were carried out, after a 24 hour incubation of
increasing quantities of 1/1* and 2/2* with the biomolecule in
the dark. The corresponding gels are depicted in Figure 2. The
free plasmid DNA is principally composed of form I, that is,
the normal supercoiled form, and some form II or relaxed
circular form (Figure 2, lanes 1). As reported earlier,[22] the
electrophoretic mobility of form II increases after incubation
2
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Angew. Chem. Int. Ed. 2015, 54, 1 – 6
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