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Ruthenium(ii) polypyridyl complexes with π-expansive ligands: synthesis and cubosome encapsulation for photodynamic therapy of non-melanoma skin cancer
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RESEARCH ARTICLE
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Ruthenium(II) polypyridyl complexes with
π-expansive ligands: synthesis and cubosome
encapsulation for photodynamic therapy of
non-melanoma skin cancer†
Gina Elena Giacomazzo,‡a Michele Schlich, ‡b Luca Casula, ‡b
Luciano Galantini, c,d Alessandra Del Giudice, c,d Giangaetano Pietraperzia,a,e
Chiara Sinico,b Francesca Cencetti, f Sara Pecchioli, f Barbara Valtancoli,a
Luca Conti, *a Sergio Murgia *b,d and Claudia Giorgi *a
In photodynamic therapy (PDT), Ru(II) polypyridyl complexes (RPCs) featuring the popular π-expansive
benzo[i]dipyrido[3,2-a:2’,3’-c]phenazine (dppn) ligand have attracted much attention, mainly due to the
good singlet oxygen sensitizing properties imparted by this peculiar ligand. However, notwithstanding the
intriguing perspectives, much remains to be explored about the use of RPC-based photosensitizing
agents (PSs) with more than a dppn ligand in their scaffolds. Herein, two bis-heteroleptic RPCs of the
general formula [Ru(dppn)2L]n+ (L = 4,4’-dimethyl-2,2’-bipyridine, n = 2, Ru1 or 2,2’-bipyridine-4,4’-dicarboxylate, n = 0, Ru2) were prepared in good yields by adopting an alternative synthetic approach to previously reported methods. The optimal singlet oxygen sensitizing properties and capabilities to interact
with DNA displayed by Ru1 and Ru2 were paralleled by a potent light-triggered toxicity (λmax = 462 nm)
exerted on squamous epithelial carcinoma cells. To improve the biopharmaceutical properties of these
compounds, Ru1 and Ru2 were encapsulated into cubosomes, soft nanoparticles with a lyotropic liquid
crystalline core. In vitro studies probed the effectiveness of these formulations against light-irradiated
cancer cells and confirmed intracellular ROS generation as the mechanism likely to be responsible for the
observed PDT efficacy. This work highlights the potential of [Ru(dppn)2L]-based PSs in PDT, beyond pro-
Received 16th December 2022,
Accepted 6th April 2023
viding a general and straightforward synthetic route for the preparation of this class of compounds. To
DOI: 10.1039/d2qi02678c
the best of our knowledge, this is also the first example of the encapsulation of a RPC into cubosome
nanostructures, paving the way for the development of nano-formulations with augmented biopharma-
rsc.li/frontiers-inorganic
ceutical properties for PDT application.
Introduction
Department of Chemistry “Ugo Schiff”, University of Florence, Via della Lastruccia
3, 50019 Sesto Fiorentino (FI), Italy. E-mail: luca.conti@unifi.it,
claudia.giorgi@unifi.it
b
Department of Life and Environmental Sciences, University of Cagliari, 09124
Cagliari (CA), Italy. E-mail: murgias@unica.it
c
Department of Chemistry, University of Rome La Sapienza, P.le A. Moro 5, 00185
Rome, Italy
d
CSGI, Consorzio Interuniversitario per lo Sviluppo dei Sistemi a Grande Interfase,
50019 Sesto Fiorentino (FI), Italy
e
European Laboratory for Non-Linear Spectroscopy (LENS), Via Nello Carrara 1,
50019 Sesto Fiorentino (FI), Italy
f
Department of Experimental and Clinical Biomedical Sciences “Mario Serio”, 50134
Florence, Italy
† Electronic supplementary information (ESI) available: Methods, supplementary
figures and schemes, and the spectra of compounds. See DOI: https://doi.org/
10.1039/d2qi02678c
‡ These authors contributed equally.
a
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Photodynamic therapy (PDT) continues to attract increasing
attention thanks to the encouraging results that its application
has led to the treatment of a variety of cancers, spanning from
skin tumors to lung, bladder and prostate cancers,1,2 as well as
bacterial infections.3,4 The main advantage of this therapeutic
approach, which consists of the light activation of a prodrug,
called a photosensitizer (PS), to produce harmful reactive
oxygen species (ROS), is represented by the complete spatiotemporal control over drug activation, which provides a precious chance to limit the severe side effects normally occurring
with standard chemotherapeutics.
Ruthenium(II) polypyridyl complexes (RPCs) have been
largely employed in the research of suitable PSs in PDT, with
the Mc Farland compound TLD1433 being the first Ru(II)based PS to enter human clinical trials for bladder cancer.5–8
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The interest towards this versatile class of compounds can be
attributed to its rich chemical–physical repertoire, which
includes a variety of excited-state electronic configurations
accessible with light, good singlet oxygen sensitizing properties, and the capacity to interact with key biological targets
(such as DNA or proteins).9–11 Of relevance is that a fine choice
of ligands in their octahedral geometries permits convenient
modulation of the photophysical, photochemical, and photobiological properties of the resulting RPCs, in an effort to
improve cellular uptake,12,13 shift the absorption profiles
towards red,14 confer targeting ability,15,16 and boost 1O2 sensitization. With regard to the latter aim, as prolonged excited
state lifetimes are important for efficient energy transfer to
molecular oxygen to form 1O2, changing the nature of the
lowest-lying excited state from metal-to-ligand charge-transfer
(3MLCT) to long-lived intraligand 3IL states represents a suitable way to endow the resulting RPCs with augmented
cytotoxicity.6,17 Following this strategy, over the past few years
much interest has been devoted to the use of the π-expansive
benzo[i]dipyrido[3,2-a:2′,3′-c]phenazine (dppn) ligand in the
rational design of RPC-based PSs. Indeed, this peculiar ligand
has been largely exploited not only to improve the photobiological activity of the resulting compounds, via the population of
long-lived dppn-centered 3ππ* excited states, but also to shift
their 1MLCT absorption towards longer wavelengths18 and,
given its known DNA-intercalating properties, to strengthen
their interaction with the nucleic acid.19–21 A recent example of
this was reported by Zhao and coworkers, who showed the
benefits derived from the substitution of a bpy (bipyridine)
unit by a dppn ligand in their tris-heteroleptic RPC-based
PSs.22
Notwithstanding the advantages derived from the use of
dppn, it is surprising that PSs containing two dppn ligands
simultaneously coordinated to a Ru(II) center have been only
sparingly explored,23,24 while numerous examples of dppn-containing RPCs for PDT are reported in the literature25–31 (some
of them have also been applied for compounds at the boundary between PDT and photoactivated chemotherapy PACT).32,33
Such net discrepancy between RPCs containing one and two
dppn units would be related to synthetic issues concerning the
preparation of the latter compounds by the general procedures
for bis-heteroleptic Ru(II) complexes,34,35 involving the intermediate [(dppn)2RuCl2] which is scarcely soluble in most
organic solvents.
In addition, the potential anticancer activity of these
systems might be limited by their common hydrophobic
nature, leading to poor bioavailability and compromised therapeutic outcomes. To overcome these limits, nanocarriers have
been widely investigated as a formative approach to increase
the water solubility of insoluble drug candidates, prevent drug
degradation, and enhance their delivery.36–38 In the midst of
the innovative exploited nano-systems, great interest has
arisen around cubosomes, also known as bicontinuous cubic
liquid crystalline nanoparticles with a three-dimensional
arrangement of the lipid bilayer forming a honeycomb-like
inner structure. Compared to single-bilayer liposomes, cubo-
3026 | Inorg. Chem. Front., 2023, 10, 3025–3036
Inorganic Chemistry Frontiers
somes are characterized by an inner portion completely filled
with the lipid matrix, providing a greater hydrophobic volume
and thus a higher loading efficiency.39 Despite the fact that
some investigations illustrated a possible cubosome
cytotoxicity,40,41 appropriate formulation strategies and administration at lower concentrations can be used to achieve the
desired therapeutic effects. In fact, recent studies have proven
their useful biomedical applications for diagnostic purposes,
anticancer activity, and PDT.42–46
Prompted by this scenario, herein we explored the potential
as PSs of two Ru(II) compounds featuring two dppn ligands
simultaneously coordinated to the Ru(II) centers; [Ru
(dppn)2(dmbpy)]2+ (Ru1) and [Ru(dppn)2(dcbpy2−)] (Ru2)
(dmbpy = 4,4′-dimethyl-2,2′-bipyridine, dcbpy2− = 2,2′-bipyridine-4,4′-dicarboxylate) (Chart 1). Besides the Ru(dppn)2-core,
different dmbpy and dcbpy2− ancillary ligands were chosen to
provide a potential synthetic platform for obtaining differently
functionalized (dppn)2-RPCs, to investigate their possible
influence on the chemical–physical and biological properties
of the resulting compounds.
Ru1 and Ru2 were prepared by adopting a straightforward
synthetic route where the dppn ligands were allowed to react
with Ru(II)-intermediates in the last step of the reaction, thus
avoiding the use of [Ru(dppn)2Cl2] and leading to the production of RPCs in good yields. These systems exhibited promising features as PSs, by virtue of optimal singlet oxygen sensitizing properties and capacity to interact with DNA, and for
this reason their phototoxicity and biocompatibility were
tested on non-melanoma skin cancer cells in vitro, a model
tumor selected for the feasibility of its treatment by photodynamic therapy.47 To further ascertain their potential as PSs,
Ru1 and Ru2 were also encapsulated in monoolein-based
cubosomes stabilized with Pluronic F108. Following a preliminary investigation of the obtained formulations, Ru2-cubo was
then selected for further development including a thorough
physicochemical characterization and the assessment of its
phototoxic activity against epidermoid carcinoma cells.
The results herein discussed may provide fundamental
knowledge for the design of novel and highly performant PSs
Chart 1 Chemical structures of ruthenium complexes Ru1 and Ru2 of
this study.
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Inorganic Chemistry Frontiers
based on (dppn)2-containing RPCs. Moreover, to the best of
our knowledge, this study reports the first example of the
encapsulation of a RPC into cubosome nanostructures, thus
paving the way for the development of pharmaceutically viable
nano-formulations for PDT applications.
Results and discussion
Synthesis and characterization of ruthenium compounds
Ru(II) complexes Ru1 and Ru2 were obtained via stepwise
ligand addition following the synthetic route shown in
Scheme 1c. In this synthetic approach, the polymeric precursor
[Ru(CO)2Cl2]n was first prepared by the reaction of the commercial RuCl3·nH2O with paraformaldehyde in formic acid.
Then, this compound was allowed to react with the bidentate
ligands in refluxing methanol (dmbpy) or DMF (dcbpy),
affording the trans-Cl[Ru(dmbpy)(CO)2Cl2] and trans-Cl[Ru
(dcbpy)(CO)2Cl2] intermediates, with yields of 75 and 55%,
respectively. In the latter case, DMF was chosen as the solvent
because of the limited solubility of dcbpy in methanol.48
Finally, two equivalents of dppn ligands were added to solutions of the trans-Cl[RuL(CO)2Cl2] (L = 4,4′-dimethyl-2,2′-bipyridine or dmbpy, 2,2′-bipyridine-4,4′-dicarboxylic acid or dcbpy)
intermediates in 2-methoxyethanol, and in the presence of trimethylamine N-oxide (TMAO), to favour the detachment of the
strongly coordinated CO ligands49 and allow their replacement
by the bidentate dppn ligands. The addition of aqueous KPF6
led to the precipitation of the hexafluorophosphate salt of Ru1
whereas Ru2 precipitated as a neutral product from the reaction mixture. Ru1 and Ru2 were obtained, after purification by
flash chromatography, in 78% and 50% yields, respectively.
Research Article
The identity of the obtained compounds was confirmed by 1H,
13
C, COSY and HSQC NMR and high-resolution mass spectrometry (HR-MS) analysis (see the ESI, Fig. S1–S10†). 1H NMR
signal assignment is reported in the ESI;† recording of 13C and
HSQC spectra of Ru2 was prevented by its poor solubility in
(CD3)2SO.
As shown in Scheme 1, it can be highlighted that, compared to the most employed synthetic approach used for the
preparation of bis-heteroleptic complexes with the general
formula [Ru(NN)2L]2+ (N,N = polypyridyl bidentate ligand)50,51
(Scheme 1a), commonly obtained by the reaction of [Ru
(NN)2Cl2] with a third chelate ligand (L), in the method of this
work the two dppn ligands are allowed to react with the Ru(II)scaffolds only in the last step of the reaction. This would
permit to overcome solubility issues arising from the use of
the [Ru(dppn)2Cl2] intermediate. A similar “reverse” concept
was also previously applied by Turro and coworkers in the synthesis of a rare example of a (dppn)2-containing RPC reported
in the literature, namely [Ru(bpy)(dppn)2][PF6]2,24 which was
indeed obtained by the reaction of dppn with [Ru(bpy)
(CH3CN)4]2+ in the last reaction step (Scheme 1b). However,
long reaction times (in the order of 7–24 days) were required
by this route to prepare the intermediate [Ru(bpy)(CH3CN)4]2+
using RuCl3·nH2O as the starting material.52,53
In light of these considerations, the synthetic strategy
employed in this work may provide an alternative and straightforward way for the preparation of RPCs featuring the general
formula [Ru(dppn)2L]n+ (L = variously functionalized bidentate
polypyridyl chelates), in good yields and reaction times.
The electronic absorption spectra of Ru1 and Ru2 in acetonitrile are shown in Fig. 1a, whereas their molar extinction
coefficients (ε) at different absorption maxima (λmax) are listed
Scheme 1 Synthetic route followed for the preparation of complexes Ru1 and Ru2 of this work (3c), compared to the one generally employed for
the preparation of bis-heteroleptic RPCs (3a) and to the one previously reported for the Turro’s compounds [Ru(bpy)(dppn)2][PF6]2 and [Ru( phpy)
(dppn)2][PF6] (3b).
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Inorganic Chemistry Frontiers
Fig. 1 Electronic absorption spectra of Ru1 and Ru2 in acetonitrile (a). Singlet oxygen determination as evaluated through UV-Vis analysis by using
DHN as an indirect 1O2 reporter; in the inset are compared the semilogarithmic plots of ln(A/A0) as a function of the irradiation time registered for
Ru1 and Ru2 and [Ru( phen)3]2+ as the reference control ([DHN] = 3.3 × 10−4 M, [Ru1] = [Ru2] = 10 µM) (b). Sketch of the 1O2 determination by
employing DHN as an indirect probe for 1O2 (c). Absorption spectra of aqueous solutions of Ru1 registered in the presence of increasing concentrations of ct-DNA; in the inset are reported the [DNA]/Iεa − εfI values obtained for Ru1 and Ru2 versus the molar concentration of DNA ([Ru1] =
[Ru2] = 10 µM, TRIS buffer pH 7.4) (d).
Table 1 Electronic absorption maxima measured in acetonitrile, rate constants Kobs, quantum yields for 1O2 generation (ϕΔ) and binding constants
with ct-DNA (Kb) of ruthenium complexes of this study
Compound
Ru1
Ru2
a
λabs nm−1 (ε × 103 M−1 cm−1)a
324 (146.1), 387 (25.3), 409 (32.2), 440 (26.6)
323 (123.2), 387 (27.8), 410 (32.4), 445 (30.0)
Kb (×106 M−1)
ϕΔ (1O2)b
Kobsa
−3
1.85 × 10
2.71 × 10−3
5
0.54 ± 0.06
0.50 ± 0.07
7.49 × 10
2.34 × 106
pKa
––
pKa1, pKa2°3.6 ± 0.3,
pKa2* 4.6 ± 0.4
Determined in acetonitrile. b Determined for air-saturated acetonitrile solutions of Ru(II) complexes.
in Table 1. As shown, besides the intense intraligand π → π*
transitions at 280–330 nm, both complexes display a double
humped absorption at ∼387 and ∼410 nm, which is typical of
the dppn centered π → π* transitions, plus a broad 1MLCT
absorption centered at ∼445 nm, in good agreement with
those of dppn-containing RPCs reported in the literature.24,54
It can also be noted that the absorptions relative to the dppncentered transitions of Ru1 and Ru2 are more intense than the
corresponding ones reported for the parental compound [Ru
(bpy)2dppn]2+,24 as expected due to the presence of two dppn
units in their Ru(II) scaffolds. On the other hand, Ru1 and Ru2
resulted to be weakly luminescent, with the highest emission
3028 | Inorg. Chem. Front., 2023, 10, 3025–3036
being displayed by Ru2 in acetonitrile and ethanol (Fig. S11,
ESI†).
Finally, given the presence of the ionizable dcbpy ligand in
Ru2, the acid–base behavior of this complex in water was
examined by means of spectrophotometric titrations, as
described in the ESI.† Similar to what was previously reported
for a parental dcbpy-containing Ru(II) complex,55 of the two
possible protonation equilibria only pKa2 values of 3.6 ± 0.3
and 4.6 ± 0.4, respectively, for the ground ( pKa2°) and the
excited state ( pKa2*) (Table 1) were determined by these
measurements. This, along with the presence of two inflection
points in the fluorescence titrations, suggested that the first
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pKa value was too low to be accurately determined. The higher
value found for pKa2* relative to pKa2° would be in line with
the higher basicity of the complex in the excited state. It
should also be noted that these data confirm that the carboxylic functions of Ru2 are likely to be fully deprotonated at
neutral pH, conferring an overall total neutral charge to the
complex. Therefore, along with the different nature of their
ancillary ligands, it can be envisaged that the different charges
of metal complexes in physiological media (+2 for Ru1, 0 for
Ru2) might have an influence on their biological behavior and
interaction with cubosome nanostructures (vide infra).
Singlet oxygen sensitizing properties of Ru(II)-complexes and
DNA interaction
A crucial requisite for a candidate PS for PDT applications
relies on its ability to trigger the formation of harmful reactive
species under light-irradiation, such as the highly oxidant
singlet oxygen 1O2, the classical warhead of PDT produced as
the result of type-II-based pathways.56
The singlet oxygen sensitizing properties of Ru(II) complexes Ru1 and Ru2 were first assessed spectrophotometrically,
by employing 1,5-dihydroxynaphtalene (DHN) as an indirect
reporter for singlet oxygen. Indeed, in the presence of 1O2,
DHN is promptly and quantitatively oxidized to give 5-hydroxy1,4-naphthalenedione (Juglone), thus allowing to easily follow
the photoexcitation process by monitoring the decrease of the
DHN absorption band, centered at 297 nm, and the simultaneous increase of the broad Juglone band at around 427 nm
(see Fig. 1c for a schematic illustration of the 1O2 analysis by
the DHN method for Ru1 and Ru2 complexes).
Fig. 1b shows the absorption spectra of an acetonitrile solution containing Ru1 and DHN subjected to increasing
irradiation times (LED emitting at 434 nm, 160 mW), lightexposure determined the progressive decrease of the DHN
absorption band along with the simultaneous increase of that
of Juglone, thus clearly demonstrating the photosensitizing
properties of Ru1. It should also be noted that the appearance
of two clear isosbestic points in the UV-Vis titration, at ∼280
and 330 nm, ruled out the formation of long-lived intermediates or byproducts. An analogous behavior was displayed by
Ru2, as reported in Fig. S13 of the ESI.† Compared to [Ru
( phen)3]2+, taken as a reference RPC for 1O2 sensitization, both
Ru1 and Ru2 exhibited remarkably higher photosensitizing
features. This can be easily appreciated from the corresponding semilogaritmic plots of ln(A/Ao) over the irradiation
time frame (A0 and A are the absorbance values at 297 nm at
time “zero” and at a generic time “t”) reported in the inset of
Fig. 1b, in which can be evidenced, for example, that a similar
amount of 1O2 was produced within 65–75 s by Ru1 and Ru2,
and in more than 200 s by [Ru( phen)3]2+. In detail, Ru1 and
Ru2 displayed a comparable potency, as denoted by the slight
differences emerging between their relative rate constants for
the DHN photooxidation processes (kobs), of 1.85 × 10−3 and
2.71 × 10−3, respectively (Table 1). In addition to the indirect
DHN method, the 1O2 sensitizing properties of Ru1 and Ru2
were further probed through direct measurement of the phos-
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Research Article
phorescence signal of 1O2 at 1270 nm, induced by irradiation
of air-saturated acetonitrile solutions of ruthenium complexes.
This allowed us to determine the relative quantum yields of
1
O2 generation (ϕΔ), which are listed, along with the one of
[Ru( phen)3]2+ for comparison (ϕΔ = 0.38 ± 0.06), in Table 1. As
shown, ϕΔ values of 0.54 ± 0.06 and 0.50 ± 0.07 were respectively obtained for Ru1 and Ru2, thus confirming that the simultaneous presence of two dppn units into the Ru(II) scaffolds
confers to these complexes a potent and comparable ability to
sensitize the formation of singlet oxygen, in well agreement
with the results of the UV-Vis analysis.
Since it is known that 1O2 rapidly reacts with the surrounding biological substrates (estimated half-life <40 ns, range of
action in the order of 20 nm),57 leading to an extremely localized oxidative damage, the ability of a PS to effectively interact
with a desired biological target may be important for its potential application in PDT, as it would ensure drug localization in
close proximity to the target to be treated, strengthening the
oxidative damage induced by ROS sensitization. This, along
with the known DNA intercalating properties imparted by the
π-expansive dppn ligands, prompted us to consider the affinity
of the studied RPCs with the nucleic acid. The DNA-binding
abilities of Ru1 and Ru2 were evaluated on calf thymus (ctDNA) through UV-Vis analysis, by monitoring the changes in
the absorption profiles of the aqueous solution of RPCs
buffered at pH 7.4 induced by increasing concentrations of ctDNA. As shown in Fig. 1d for a 10 µM solution of Ru1, the
addition of ct-DNA resulted in a strong hypochromism in both
the MLCT and π → π* absorption bands of the metal complex,
with a reduction of approximately 50 and 65% of their relative
intensities in the presence of only 3 µM DNA. No blue or red
shift was observed upon the addition of DNA and a very
similar trend was also observed in the case of Ru2 (see
Fig. S14, ESI†). The intrinsic binding constants (Kb) of Ru1
and Ru2 were calculated from titration data (see the inset of
Fig. 1d for a comparison between the two RPCs) as described
in the ESI† and the resulting values are reported in Table 1. As
shown, Kb values of 7.49 × 105 M−1 and 2.34 × 106 M−1 were
respectively obtained for Ru1 and Ru2, thus confirming the
ability of these systems to strongly interact with DNA under
abiotic conditions. It can be noted that these values are in line
with the ones reported for other dppn-containing ruthenium
complexes (Kb in the order of 106 M−1)54,58,59 and though not
conclusive, together with the large extent of hypochromism
observed, they hint at the intercalation as the most likely
binding mode for these complexes. Moreover, the possible
beneficial role played by the presence of a second dppn ligand
in strengthening the interaction of complexes with the biopolymer is particularly evidenced by comparing Ru1 with its
mono-dppn containing analogue, [Ru(dmbpy)(dppn)]2+, for
which a lower Kb, of almost 5.8-fold has been reported.28
Cytotoxicity and photoactivity of Ru(II)-complexes
To be qualified as a potential agent for photodynamic therapy,
newly developed photosensitizers should be biologically inert
in the dark, but highly cytotoxic when exposed to light of a
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given wavelength.60 This simple mechanism allows for selective action against the light-exposed area (i.e. the tumor), abolishing the systemic toxicity typically associated with traditional
chemotherapeutic drugs.46 Here, the anticancer activity of Ru1
and Ru2 was evaluated on A431 cells, an in vitro model of
human epidermoid carcinoma.
As shown in Fig. 2, both compounds were found to be well
tolerated by cells when no light was provided to the culture
dishes. A slight difference between their in dark toxicities was
observed, thus indicating that seemingly small modifications
on the groups gathered on the bpy moieties of complexes
(methyl or carboxylic functions) may influence their toxicity. In
details, cell viability was reduced to 75.1 ± 4.1% and 82.4 ±
2.0% upon exposure to the highest dose of Ru1 and Ru2
(25 µM) in the dark, respectively. Conversely, 30-minutes of
irradiation with an LED array (λmax = 462 nm, 18 mW cm−2)
induced potent activation of the complexes, triggering complete cell death (viability < 10%) at concentrations of 0.25 µM
(Ru1, Fig. 2a) and 5 µM (Ru2, Fig. 2b): Fig. 2c summarizes the
IC50 values calculated from in vitro experiments. As shown,
both Ru1 and Ru2 displayed high photo-toxic indexes (PI,
defined as IC50 in the dark/IC50 upon irradiation), with values
exceeding 988 and 130, respectively. From a translational point
of view, higher PIs are predictive of a larger therapeutic
Fig. 2 Viability of A431 epidermoid carcinoma cells assessed by MTT
following treatments with Ru1 (a) or Ru2 (b), with or without exposure
to light for 30 minutes (n = 5). Table summarizing the IC50 values
(±SEM) for the different experimental groups (c).
3030 | Inorg. Chem. Front., 2023, 10, 3025–3036
Inorganic Chemistry Frontiers
window, with limited off-target cytotoxicity and enhanced ontarget potency. Of note, notwithstanding the lack of data for
the phototoxicity of dppn-containing Ru(II) complexes in A431
cells, it can be highlighted that the in vitro therapeutic outcomes of complexes of this study are ones of the highest
among those reported in the literature for the PDT effect of
dppn-containing RPCs.23,25,61–63
Cubosome loading and characterization
The in vitro results highlighted the promising activity of the
obtained systems in PDT. Nevertheless, their poor aqueous
solubility would not be compatible with direct administration
to a patient. In fact, self-aggregation phenomena might occur
due to the high hydrophobicity of these systems, leading to
low bioavailability, possible off-target activation and reduction
of their photosensitivity and photophysical properties.64 The
encapsulation of PSs into nanocarriers is a well-known technique used to overcome these issues and to facilitate their biomedical application.65 In this study, we prepared Ru1 and Ru2
cubosome-loaded formulations using monoolein (MO) as the
molecular building block and PF108 as the stabilizing agent.
In line with previous results,66 the obtained samples were fluid
aqueous dispersions with a milky macroscopic appearance.
Cubosomes, here proposed as PS carriers, were prepared as
described in paragraph 4.1 of the ESI† and characterized in
terms of encapsulation efficiency and colloidal properties,
namely size, size distribution and zeta potential.
Unencapsulated PSs were removed by exhaustive dialysis,
then cubosomes were dissolved in methanol and the drug
content was spectrophotometrically quantified. The results
revealed high encapsulation values of Ru2 (60%), whereas the
amount of encapsulated Ru1 was 9%. Besides their different
structures, the two complexes also display different overall
charges (at neutral pH Ru1 features a double positive charge
whereas Ru2 is likely to be present in its neutral form) and
this can be reasonably assumed to affect the encapsulation
efficiency into cubosomes. Indeed, the production procedure
and the excipients employed were identical for both formulations, the encapsulated PS being the sole difference.
As for the colloidal properties, DLS analysis revealed the
presence of nanoparticles with an average diameter of approximately 138 and 142 nm, for Ru1-cubo and Ru2-cubo respectively (Fig. 3a). Both formulations showed a narrow size distribution with PDI values below 0.2. Concerning the nanoparticle
zeta potential, we recorded a value of −9 mV for Ru1-cubo and
−30 mV for Ru2-cubo, thus indicating a superior stabilization
of the latter.
We monitored the average diameter, PDI and zeta potential
over a period of 30 days, for a medium-term stability study of
the colloidal systems (Fig. S16, ESI†). The size distribution
study revealed optimal stability of Ru2-cubo, since the mean
diameter did not vary appreciably during the 30 days on
storage at 25 °C, with an average diameter of approximately
140 nm during the whole study. The PDI and zeta potential
were almost constant, confirming the retention of the fairly
narrow size distribution on storage. Conversely, the average
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Fig. 3 Ru1-cubo and Ru2-cubo composition and characterization in terms of average diameter (D, nm), polydispersion index (PDI), zeta potential
(ZP, mV) and encapsulation efficiency (EE%) (a). Cryo-transmission electron microscopy (b) and small angle X-ray scattering patterns of Ru2-cubo
with indication of the Bragg peaks corresponding to the Im3 m (red dotted lines) and the Pn3 m (blue continuous lines) cubic bicontinuous phases (c).
diameter of Ru1-cubo increased from 138 nm (day 0) to
235 nm (day 30), the zeta potential moved to lower values,
while PDI values were almost steady.
Given the obtained preliminary results of Ru1-cubo,
namely, low encapsulation efficiency and an increase of the
average diameter over 30 days of storage, we selected Ru2-cubo
for further characterization and in vitro bioactivity tests.
Firstly, we evaluated the nanoparticles morphology of Ru2cubo by means of cryo-transmission electron microscopy
(Cryo-TEM). As shown in Fig. 3b, cubosomes appear as spherical nanoparticles with an internal structure characterized by a
dark matrix and bright spots, which represent the lipid phase
and the water channels respectively. We then evaluated the
inner nanostructure of Ru2-cubo through small angle X-ray
scattering. Particularly, the recorded SAXS pattern shown in
Fig. 3c strongly suggests the simultaneous presence of two
bicontinuous cubic phases, the Pn3 m and the Im3 m, respectively characterized by lattice parameters of 92 ± 1 Å and 117 ±
1 Å and water channel radii of 38 ± 1 Å and 37 ± 1 Å. In fact,
the coexistence of the two phases is often observed when MO
cubosomes are stabilized with Pluronics.66,67
Cytotoxicity, photoactivity and ROS production of cubosomesencapsulated Ru2
In addition to promoting solubility and stability, nanoencapsulation of photosensitizers in soft colloids has shown to
improve the management of cancer in previous studies, as it
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allows targeted delivery and favors bio-membranes
crossing.68–71 When designing novel PS-loaded nanoparticles,
it is critical to assess that the biological activity of the cargo is
retained upon nano-encapsulation, and that no unspecific toxicity comes from the nanoparticle itself (i.e. empty vector). For
such reasons, we tested the cytotoxicity (in the dark) and
phototoxicity (upon LED illumination) of Ru2-cubo on the previously described epidermoid carcinoma model, comparing
the results with the effect triggered by empty cubosomes
(E-cubo, not loaded with PS). Ru2-cubo sensitized cancer cells
to light even at a very low concentration of 0.025 µM ([Ru2]),
with more than 50% reduction of cell viability at a dose of
0.25 µM (Fig. 4a). Calculated IC50 for Ru2-cubo was 0.268 ±
0.079 µM. The slightly higher IC50 of Ru2-cubo compared to
free Ru2 is expected for a nano-encapsulated molecule and can
be partially explained by the lower intracellular localization of
ruthenium, evidenced by inductively coupled plasma atomic
emission spectrometry (ICP-AES), when entrapped in the soft
lipid matrix (Fig. S17, ESI†). As expected, treatment with Ru2cubo was efficacious only when coupled with LED irradiation,
as cells incubated in the dark did not show signs of sufferance.
The risk of unspecific toxicity of other components of the
nanoformulation (i.e. monoolein and PF108) was ruled out by
exposing cells to E-cubo under the same conditions (Fig. 4b).
To obtain preliminary information about the mechanism of
the observed phototoxicity, we first investigated the production
of intracellular ROS upon PDT using the 2′,7′-dichlorodihydro-
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Fig. 4 Viability of A431 epidermoid carcinoma cells assessed by MTT following treatments with Ru2-cubo (a) or E-cubo (b), with or without
exposure to light for 30 minutes. The dose is expressed as concentration of Ru2 in the cell culture well or the corresponding volume of E-cubo. The
dashed line is a guide for the eye to highlight the viability of cells exposed to light without PS. One way ANOVA with post-hoc Tukey HSD test was
employed to substantiate differences between cells exposed only to light (no PS, 0 µM) vs. cells treated with Ru2-cubo or E-cubo and exposed to
light (*p < 0.01) (n = 8). Production of ROS by A431 epidermoid carcinoma cells estimated by the oxidation of the DCF-DA sensor and visualized by
confocal laser scanning microscopy (c–e). Cells treated with Ru2-Cubo (100 nM) and exposed to light for 10 minutes (c) or incubated in the dark (d).
Untreated cells (e). The green signal corresponds to the sensor oxidized by intracellularly produced ROS to its fluorescent derivative DCF. Red signal
shows the cell membranes stained with WGA. Scalebar = 50 µm.
fluorescein diacetate (DCFH-DA) assay.72 When applied to the
cell culture, the cell permeable probe DCFH-DA crosses the
cell membrane and it is deacetylated by cytosolic esterases
into a non-fluorescent metabolite (DCFH). In the presence of
intracellular ROS, the metabolite can be oxidized to produce
highly fluorescent 2′,7′-dichlorofluorescein (DCF). The amount
of ROS produced by the cells in response to PDT can be estimated by measuring the green fluorescence intensity of DCF
localized within the cell body.
A431 cells were treated with Ru2-cubo, supplied with the
DCFH-DA probe and exposed to light to trigger the activation
of the photosensitizer. The dose of Ru2-cubo (100 nM of Ru2)
was selected to allow for the observation of ROS generation,
limiting the extent of cell toxicity. Immediately after
irradiation, cells were fixed, and their membranes were
stained with WGA for microscopy observation. Representative
images acquired by confocal laser scanning microscopy allow
to observe a diffuse green fluorescence in almost 87.4% of the
cells exposed Ru2-cubo + light (Fig. 4c). Conversely, the treatment with Ru2-cubo in the dark did not induce significant
production of ROS, as the amount of green signal detectable
(Fig. 4d) was comparable to the one observed in a well of
untreated cells (control, Fig. 4e). More specifically, the percentage of ROS-producing cells calculated through image analysis
3032 | Inorg. Chem. Front., 2023, 10, 3025–3036
was 1.3% and 0.3% for Ru2-cubo in the dark and for untreated
cells, respectively.
We then inspected the intracellular distribution of Ru2cubo into A431 cells by employing laser-scanning confocal
microscopy (Fig. S18, ESI†). Despite the ability of the PS to bind
DNA, our results indicated a modest localization of Ru2-cubo
within the nuclei, at least after 1 hour of incubation of A431
cells. This was also observed for the non-encapsulated metal
complex, thus suggesting that ROS oxidation of other types of
macromolecules, such as proteins or membrane lipids, rather
than DNA, is likely to be the cause of the observed phototoxicity
under our experimental conditions. These oxidized species, in
addition to losing their function, can initiate the pro-apoptotic
and pro-necrotic cascade, resulting in cell damage and death.73
Interestingly, it can also be noted that, in contrast to the
free metal complex, which, after 1 hour of incubation, evidenced a random distribution in the cellular cytosol, after the
same incubation time Ru2-cubo was rather found to be finely
localized in discrete areas.
Overall, these results confirm that the cytotoxic effect
observed upon PDT with Ru2-cubo would be related to the
capacity of this system to effectively trigger the production of
intracellular ROS, as expected due to the good singlet oxygen
sensitizing properties of Ru2.
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Inorganic Chemistry Frontiers
Research Article
Conclusions
Author contributions
In this study, we explored the potential as PSs for PDT applications of two novel Ru(II) complexes, Ru1 and Ru2, characterized by two π-expansive dppn units simultaneously coordinated to their Ru(II) centers. The synthetic route followed
for the preparation of these complexes may represent a valid
alternative to commonly employed methods and can be potentially harnessed for the preparation of bis-heteroleptic RPCs of
the general formula [Ru(dppn)2L]2+ (L = variously functionalized bpy ligands), whose chemical–physical and photobiological properties can be finely modulated by tuning the nature of
their bidentate chelates. The simultaneous presence of two
dppn ligands conferred to Ru1 and Ru2 optimal singlet oxygen
sensitizing features and DNA-interaction capabilities, which
were paralleled by a potent light-triggered toxicity exerted on
squamous epithelial carcinoma cells, with PI values exceeding
988 (Ru1) and 130 (Ru2).
Given their scarce solubility in physiological media, which
would preclude their direct administration for therapeutic use,
Ru1 and Ru2 were encapsulated into cubosomes, chosen as
soft nanoparticles to obtain Ru(II)-formulations with improved
biopharmaceutical properties. Among the resulting hybrid
systems, Ru2-cubo displayed superior encapsulation efficiency
and stability as compared to Ru1-cubo, thus hinting at a
subtle role played by the nature of the ancillary ligands and/or
the overall charge of RPCs. For this reason, we focused our
attention on the former system, which was further characterized and subjected to bioactivity investigations. Our results
probed the effectiveness of Ru2-cubo, as denoted by the photoactivity observed even at a very low drug concentration,
whereas mechanistic studies confirmed that intracellular ROS
generation was likely responsible for the Ru2-cubo-mediated
PDT efficacy.
An important aspect that deserves consideration is that soft
matter nanoparticles are prone to phase transition/degradation when dispersed in fluids of biological interest.74
However, several studies evidenced that monoolein-based
cubosomes are rather stable when incubated in fetal bovine
serum solution,75,76 while when dispersed in human plasma77
after 15 min they start to evolve towards a different kind of
nanoparticle known as hexosomes, characterized by a hexagonal inner nanostructure.78,79 Indeed, at least one investigation proved that after 10/15 min from i.v. administration in
mice, cubosomes are non-altered and able to reach all the biological compartments without the release of the imaging agent
they carried.
In conclusion, the results herein discussed highlight the
great potential of RPCs featuring two π-expansive dppn ligands
as photosensitizing agents in the blooming field of research of
PDT. Going beyond providing a simple and general synthetic
route for the preparation of this class of compounds, to the
best of our knowledge this work also reports the first RPC to
be encapsulated into cubosome nanostructures, providing fundamental knowledge about the design of pharmaceutically
viable Ru(II)-cubosome formulations for PDT applications.
G. E. G., M. S. and L. Casula: investigation and data curation,
L. G., A. D. G., C. S., G. P., F. C., S. P. and B. V.: investigation,
S. M. and C. G.: supervision and project administration,
L. Conti.: writing the original draft and project
administration. G. E. G., M. S., L. Casula, L. Conti, C. S., B. V.,
C. G. and S. M. are inventors on a pending patent application
pertaining to the ruthenium polypyridyl complexes described
in this work. All authors have given approval to the final
version of the manuscript.
This journal is © the Partner Organisations 2023
Conflicts of interest
The authors declare no conflicts of interest.
Acknowledgements
The authors would like to thank Dr Annalisa Guerri, from the
Department of Chemistry Ugo Schiff of the University of
Florence for the Cryo-TEM measurements. UniCA-Progetti
biennali di Ateno Finanziati dalla Fondazione di Sardegna
2018 (CUP F741I19000950007) is gratefully acknowledged for
( partial) financial support.
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