Ekaterina V.
Svezhentseva
ab,
Anastasiya O.
Solovieva
c,
Yuri A.
Vorotnikov
a,
Olga G.
Kurskaya
d,
Konstantin A.
Brylev
ab,
Alphiya R.
Tsygankova
ab,
Mariya V.
Edeleva
e,
Svetlana N.
Gyrylova
d,
Noboru
Kitamura
f,
Olga A.
Efremova
*g,
Michael A.
Shestopalov
*abcd,
Yuri V.
Mironov
ab and
Alexander M.
Shestopalov
d
aNikolaev Institute of Inorganic Chemistry SB RAS, 3 Acad. Lavrentiev Ave., 630090 Novosibirsk, Russian Federation. E-mail: shtopy@niic.nsc.ru; Fax: +7 383 330 94 89; Tel: +7 383 330 92 53
bNovosibirsk State University, 2 Pirogova Str., 630090 Novosibirsk, Russian Federation
cScientific Institute of Clinical and Experimental Lymphology, 2 Timakova Str., 630060 Novosibirsk, Russian Federation
dResearch Institute of Experimental and Clinical Medicine, 2 Timakova Str., 630060 Novosibirsk, Russian Federation
eVorozhtsov Novosibirsk Institute of Organic Chemistry SB RAS, 9 Acad. Lavrentiev Ave, 630090 Novosibirsk, Russian Federation
fDepartment of Chemistry, Faculty of Science, Hokkaido University, 060-0810 Sapporo, Japan
gDepartment of Chemistry, University of Hull, Cottingham Road, Hull, HU6 7RX, UK. E-mail: o.efremova@hull.ac.uk; Tel: +44 (0)1482 465417
First published on 5th January 2017
The development of water-soluble forms of octahedral molybdenum clusters {Mo6X8}4+ (X = Cl, Br, I) is strongly motivated by the tremendous potential that these complexes have for biological applications, namely as agents for bioimaging and photodynamic therapy. In this work, we report the first water-soluble hybrid materials, which represent sodium polystyrene sulfonate doped by molybdenum clusters, and the evaluation of their photophysical and biological properties (dark and photoinduced cytotoxicity and cellular uptake) with the use of cervical cancer (HeLa) and human epidermoid larynx carcinoma (Hep-2) cell-lines as models.
![]() | ||
Fig. 1 The general structure of octahedral cluster complexes [{Mo6X8}L6]n, where X is either Cl, Br or I and L is either an organic or inorganic terminal ligand. |
In order to tackle this obstacle we recently developed an approach, in which hexamolybdenum cluster complexes were supported by inert matrices, such as SiO2 nanoparticles,11–14 polystyrene microparticles7,15–17 and metal–organic frameworks,9,18,19 which are known to build stable suspensions in water.
Such an approach allowed us to study some biological properties (e.g. dark cytotoxicity and photoinduced cytotoxicity) of Mo6 cluster containing polymer materials. It is obvious though that the above approach does not produce materials, where hexamolybdenum cluster anions would be dissolved in water, which could be valuable in the context of increasing singlet oxygen generation efficiency and corresponding photoinduced toxicity. Indeed, in our previous work we showed that the efficiency of singlet oxygen generation was strongly dependent on the size of the particles: the higher specific surface area, the more efficient the singlet oxygen generation.11
In this work, we demonstrate a new approach to deliver hexamolybdenum cluster complexes in an aqueous phase. In this method, highly water-soluble anionic polymer sodium polystyrene sulfonate (PSS) was used to bind the {Mo6X8}4+ (X = Cl, Br or I) cluster complexes in order to dissolve them in aqueous media. The cytotoxicity of the obtained hybrid materials {Mo6X8}@PSS was studied by MTT assay in cervical cancer (HeLa) and human epidermoid larynx carcinoma (Hep-2) cells, while the internalisation of the cluster complexes from the solutions into HeLa cells was traced by flow cytometry.
Cluster complexes of composition [{Mo6X8}(NO3)6]2− (X = Cl, Br or I) were selected as convenient sources of {Mo6X8}4+ due to their well-recognised lability associated with easy substitution of apical NO3− ligands by other groups. Indeed, this ability of the nitrato cluster complexes was earlier exploited to develop new complexes17 as well as hybrid materials with thiol-functionalised polystyrene15,17 and silica particles.11,12
The PSS polymer of high molecular weight was obtained according to a standard free radical polymerisation reaction of 4-styrenesulfonic acid sodium salt in an aqueous solution initiated by sodium peroxodisulfate. According to elemental analysis the obtained polymer contained two water molecules per monomeric unit. The molecular mass (Mn) of PSS determined by size exclusion chromatography (SEC) was found to be 2.2 MDa.
Water-soluble molybdenum cluster doped materials {Mo6X8}n@PSS (where n = 1, 5, 10 and 100 refers to the loading of cluster complexes (Bu4N)2[{Mo6X8}(NO3)6] (X = Cl, Br or I) in milligrams per 100 mg of initial PSS) were obtained by impregnation of solid PSS with acetone solutions of (Bu4N)2[{Mo6X8}(NO3)6] at concentrations of 0.2, 1, 2 or 20 mg mL−1. After the reactions, the yellow-coloured solids (namely light yellow, yellow and dark yellow for X = Cl, Br and I, respectively) were separated by centrifugation, washed with an excess of acetone to remove any unbounded metal cluster complex and dried in air. A UV-vis study of {Mo6X8}n@PSS aqueous solutions has indeed shown enhanced absorbance in the wavelength region 270–450 nm (Fig. S1–S3, ESI†) due to the presence of the yellow metal cluster complexes.
The data of the FTIR and elemental (CHNS) analyses of {Mo6X8}n@PSS hybrids showed that all NO3− ligands and tetra-n-butyl ammonium cations were removed upon the reactions of (Bu4N)2[{Mo6X8}(NO3)6] with PSS (Fig. S4–S7, ESI†). This observation suggests that nitrato ligands were substituted by the sulfonate groups present in PSS and water molecules and removed as NaNO3 and Bu4NNO3. Such substitution of nitrato ligands in the impregnation reaction of a polymer material with a solution of (Bu4N)2[{Mo6X8}(NO3)6] was previously observed on thiol-functionalised polystyrene microspheres.15,17
To demonstrate the importance of the labile nitrato ligands in the reaction of PSS with hexamolybdenum cluster complexes, we also tested (Bu4N)2[{Mo6I8}(OOCCH3)6] (obtained according to ref. 1) under the same conditions and even at increased temperature. Indeed, we observed that PSS did not acquire the yellow colour of the cluster complex at all (see Fig. S8, ESI†) as well as ICP data did not show any Mo in the sample.
According to the ICP data of {Mo6X8}n@PSS, the content of molybdenum in the polymer increased, while the content of sodium decreased with the increase of the value n. Notably, the content of both elements was significantly lower than the theoretical content, especially for the samples {Mo6X8}100@PSS, for which the content of the metals was almost the same as for {Mo6X8}10@PSS (Fig. S9–S11, ESI†). The real loading of the cluster in the samples {Mo6X8}100@PSS estimated from both ICP and elemental analyses was about one cluster unit per 150 ± 10 monomer units. All further characterisations were performed using the samples {Mo6X8}100@PSS.
To evaluate the influence of the conjugation of the cluster complexes to PSS on hydrodynamic properties, we compared the SEC and viscometry data for an aqueous solution of neat PSS with those of {Mo6I8}100@PSS. The molecular mass of the hybrid material {Mo6I8}100@PSS as determined by SEC was 1.9 MDa, i.e. slightly lower than that determined for neat PSS. This decrease in molecular mass, although unexpected, is attributed to the use of poly(ethylene glycol) (PEO) standards, which can provide only relative values of Mn. Moreover, the Mn determined from SEC is largely dependent on the behaviour of the hybrid polymer in the eluent and therefore can deviate from the linear dependence. In particular, one can expect that the PSS polymer could form a more globular structure, when it is bonded to metal cluster complexes. Notably, the viscosity of both solutions was found to be the same (ηr = 3.7), which confirms the similarity of the molecular mass of the starting polymer and the derivative hybrid material.
![]() | ||
Fig. 2 Emission spectra of the powdered samples of {Mo6X8}100@PSS normalised by the emission of PSS. The excitation wavelength was 355 nm. |
Sample | λ em, nm | τ em, μs (A) | Φ em |
---|---|---|---|
In solid state | |||
(Bu4N)2[{Mo6Cl8}(NO3)6]15 | 765 | τ 1 = 17 (0.14) | <0.005 |
τ 2 = 9.3 (0.02) | |||
τ 3 = 1.9 (0.84) | |||
(Bu4N)2[{Mo6Br8}(NO3)6]15 | 785 | τ 1 = 19 (0.25) | <0.01 |
τ 2 = 11 (0.20) | |||
τ 3 = 0.9 (0.55) | |||
(Bu4N)2[{Mo6I8}(NO3)6]17 | 666 | τ 1 = 96 (0.71) | 0.26 |
τ 2 = 26 (0.29) | |||
(Bu4N)2[{Mo6Cl8}(OTs)6]2 | 723 | τ 1 = 228 (0.7) | 0.34 |
τ 2 = 174 (0.3) | |||
(Bu4N)2[{Mo6Br8}(OTs)6]2 | 708 | τ 1 = 185 (0.7) | 0.29 |
τ 2 = 86 (0.3) | |||
(Bu4N)2[{Mo6I8}(OTs)6]2 | 662 | τ 1 = 135 (0.6) | 0.44 |
τ 2 = 56 (0.4) | |||
{Mo6Cl8}@PS-SH15 | 745 | τ 1 = 34.4 (0.07) | <0.005 |
τ 2 = 7.7 (0.16) | |||
τ 3 = 0.68 (0.77) | |||
{Mo6Br8}@PS-SH15 | 730 | τ 1 = 32.0 (0.14) | <0.005 |
τ 2 = 9.3 (0.32) | |||
τ 3 = 1.0 (0.54) | |||
{Mo6I8}@PS-SH17 | 677 | τ 1 = 45 (0.15) | 0.04 |
τ 2 = 16 (0.40) | |||
τ 3 = 2.2 (0.45) | |||
{Mo6Cl8}100@PSS | 753 | τ 1 = 25 (0.08) | 0.01 |
τ 2 = 3.5 (0.31) | |||
τ 3 = 0.7 (0.61) | |||
{Mo6Br8}100@PSS | 725 | τ 1 = 10.6 (0.09) | 0.01 |
τ 2 = 1.3 (0.24) | |||
τ 3 = 0.2 (0.67) | |||
{Mo6I8}100@PSS | 671 | τ 1 = 74.8 (0.19) | 0.03 |
τ 2 = 30.8 (0.38) | |||
τ 3 = 3.5 (0.43) | |||
In aqueous solution (deaerated) | |||
{Mo6I8}100@PSS | 718 | τ 1 = 43.4 (0.83) | 0.01 |
τ 2 = 8.1 (0.17) |
There are two maxima in the emission spectra of {Mo6X8}100@PSS: at ∼420 and ∼700 nm that correspond to the fluorescence of the PSS matrix and the phosphorescence of the cluster complex, respectively.
Similarly to the recently described materials {Mo6X8}@PS-SH (X = Cl, Br or I; PS-SH – thiol-modified polystyrene microbeads),15 powdered samples of PSS doped by chloride and bromide clusters were characterised by noticeably lower values of τem and Φem than the one doped by {Mo6I8}4+, while λem values gradually decreased in the order Cl > Br > I (Fig. 2 and Table 1).
We were unable to determine the photophysical characteristics of aqueous {Mo6Cl8}100@PSS and {Mo6Br8}100@PSS reliably, since both aerated and deaerated solutions of {Mo6Cl8}100@PSS were not emissive at all, while the solutions of {Mo6Br8}100@PSS showed only very poor luminescence (Fig. 2, 3 and Fig. S12, S13, ESI†). In contrast, an aqueous solution of {Mo6I8}100@PSS showed appreciable red luminescence. As expected, the aerated aqueous of {Mo6I8}100@PSS exhibited relatively weak emission, while in the argon-saturated solution the emission peak of the cluster complexes was noticeably higher (Fig. 2 and Fig. S12, S13, ESI†). Indeed, the observed luminescence quenching in an aerated solution can be explained by the interaction of molecular oxygen with the triplet excited state of the cluster unit.2–4,17,22,23
![]() | ||
Fig. 3 Aqueous solutions of {Mo6X8}100@PSS under daylight illumination (top) and UV-light (bottom) illumination. |
In comparison with the initial cluster complexes (Bu4N)2[{Mo6X8}(NO3)6] in the solid state, the positions of the emission maxima of solid {Mo6X8}100@PSS are 12 nm and 60 nm blue shifted for X = Cl and Br, respectively, while for X = I the shift is only 5 nm to the red region. Notably, in work15 a similar trend of the emission maxima positions of materials {Mo6Cl8}@PS-SH was noticed (Table 1). This behaviour could be explained by the change in the apical ligand environment of the cluster, i.e. by the substitution of nitrato ligands with sulfonate groups of the polymer matrix and water molecules. In contrast, in an earlier work, the emission profile of [{Mo6I8}(OTs)6]2− (where OTs− is p-toluene sulfonate) incorporated into the poly(methyl methacrylate) matrix did not significantly change from that of the starting cluster complex, since no substitution of the apical ligands took place in the latter case.3 It should be also noted that the lifetimes and quantum yields of {Mo6X8}100@PSS are significantly lower than those found for hexamolybdenum cluster complexes in a pure sulfonate ligand environment.2,3 We believe that this is due to the presence of water molecules in the ligand environment of the cluster core in the {Mo6X8}100@PSS materials. The quenching of photoluminescence by aqua-ligands via non-radiative relaxation associated with O–H vibrations is indeed well recognised in the literature.5,24
![]() | ||
Fig. 4 Viability of Hep-2 (top) and HeLa (bottom) cells incubated with PSS and {Mo6X8}100@PSS determined by MTT assay. |
The confocal microscopy imaging of both cell lines incubated with the solutions of {Mo6X8}100@PSS (0.10 mg mL−1) for 24 h has not registered any red emission of the cluster compounds within the cells.
Since the detection sensitivity of flow cytometry (FACS) is significantly higher than that of confocal microscopy,25 we also analysed the cells by this technique. Indeed, FACS showed that the luminescence intensity of HeLa cells treated with {Mo6Br8}4+ and {Mo6I8}4+ doped materials increased, but only very slightly. However, in the case of Hep-2 cells the luminescence intensity of the cells treated with {Mo6I8}100@PSS was significantly higher than that of the control cells (Fig. S14, ESI†).
Since the FACS analysis demonstrated some uptake of the cluster-doped materials, we also evaluated the photoinduced cytotoxicity of {Mo6X8}100@PSS hybrids in both cell cultures, HeLa and Hep-2, within the non-toxic concentration range 3.2–51.6 μg mL−1 (Fig. 5). According to our data, materials {Mo6Br8}100@PSS and {Mo6I8}100@PSS demonstrated some photoinduced cytotoxicity towards HeLa cells: at the highest concentration, 51.6 μg mL−1, the percentage of the living cells after photoirradiation for 30 min was ∼70% for {Mo6Br8}100@PSS and ∼62% for {Mo6I8}100@PSS. {Mo6Cl8}100@PSS, however, did not show any appreciable phototoxicity, likely due to its poor photoluminescence properties.
![]() | ||
Fig. 5 Viability of Hep-2 (top) and HeLa (bottom) cells treated with {Mo6X8}100@PSS after photoirradiation (λ = 400 nm, 30 min) determined by dual staining with Hoechst 33342/PI. |
Surprisingly, in the case of Hep-2 cells even {Mo6I8}100@PSS (one that was taken up well by the cells according to FACS) did not demonstrate any noticeable photoinduced cytotoxicity. This observation together with the noticeably higher IC50 values for the dark toxicity of {Mo6X8}100@PSS clearly demonstrate higher resistance of Hep-2 cells to external influences in comparison with HeLa cells.
The CHNS elemental analyses were performed on a Euro-Vector EA3000 elemental analyser. The molybdenum content in all samples was determined on a high-resolution spectrometer iCAP-6500 (Thermo Scientific) with a cyclone-type spray chamber and “SeaSpray” nebulizer. The spectra were obtained by axial plasma viewing. Standard operating conditions of the ICP-AES system were as follows: power = 1150 W, injector inner diameter = 3 mm, carrier argon flow = 0.7 L min−1, accessorial argon flow = 0.5 L min−1, cooling argon flow = 12 L min−1, number of parallel measurements = 3, and integration time = 5 s. Deionised water (R ≈ 18 MΩ) was used to prepare sample solutions.
For {Mo6X8}100@PSS found: C 37.2, H 4.8, N 0, S 12.2 (X = Cl); C 35.7, H 4.5, N 0, S 12.5 (X = Br); C 36.7, H 4.7, N 0, S 12.5 (X = I).
The study of the biological properties of the materials in Hep-2 and HeLa cells showed that their dark cytotoxicity is noticeably higher than that of PSS, especially in the case of HeLa cells. FACS provided evidence that the treatment of the cells with {Mo6X8}100@PSS led to some uptake of the cluster – at least in the case of the “heavier” (i.e. the more emissive) ones – as assessed by the increase of the overall luminescence intensity of the cells. Moreover, materials {Mo6Br8}100@PSS and {Mo6I8}100@PSS also demonstrated some photoinduced cytotoxicity towards HeLa cells. Finally, the overall resistivity of Hep-2 cells towards {Mo6X8}100@PSS was higher than that of HeLa cells.
Footnote |
† Electronic supplementary information (ESI) available: FTIR spectra, UV-Vis spectra, ICP data, emission spectra and FACS data. See DOI: 10.1039/c6nj03469a |
This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2017 |