Sara Demartis1, Giovanna Rassu1, Sergio Murgia2,3, Luca Casula2, Paolo Giunchedi1, Elisabetta Gavini1. 1. Department of Chemistry and Pharmacy, University of Sassari, 07100 Sassari, Italy. 2. Department of Life and Environmental Sciences, University of Cagliari, 09042 Monserrato, Cagliari, Italy. 3. CSGI, Consorzio Interuniversitario per lo Sviluppo dei Sistemi a Grande Interfase, 50019 Sesto Fiorentino, Florence, Italy.
Abstract
Cutaneous melanoma is one of the most aggressive and metastatic forms of skin cancer. However, current therapeutic options present several limitations, and the annual death rate due to melanoma increases every year. Dermal delivery of nanomedicines can effectively eradicate primary melanoma lesions, avoid the metastatic process, and improve survival. Rose Bengal (RB) is a sono-photosensitizer drug with intrinsic cytotoxicity toward melanoma without external stimuli but the biopharmaceutical profile limits its clinical use. Here, we propose deformable lipid nanovesicles, also known as transfersomes (TF), for the targeted dermal delivery of RB to melanoma lesions to eradicate them in the absence of external stimuli. Considering RB's poor ability to cross the stratum corneum and its photosensitizer nature, transfersomal carriers were selected simultaneously to enhance RB penetration to the deepest skin layers and protect RB from undesired photodegradation. RB-loaded TF dispersion (RB-TF), prepared by a modified reverse-phase evaporation method, were nanosized with a ζ-potential value below -30 mV. The spectrophotometric and fluorimetric analysis revealed that RB efficiently interacted with the lipid phase. The morphological investigations (transmission electron microscopy and small-angle X-ray scattering) proved that RB intercalated within the phospholipid bilayer of TF originating unilamellar and deformable vesicles, in contrast to the rigid multilamellar unloaded ones. Such outcomes agree with the results of the in vitro permeation study, where the lack of a burst RB permeation peak for RB-TF, observed instead for the free drug, suggests that a significant amount of RB interacted with lipid nanovesicles. Also, RB-TF proved to protect RB from undesired photodegradation over 24 h of direct light exposure. The ex vivo epidermis permeation study proved that RB-TF significantly increased RB's amount permeating the epidermis compared to the free drug (78.31 vs 38.31%). Finally, the antiproliferative assays on melanoma cells suggested that RB-TF effectively reduced cell growth compared to free RB at the concentrations tested (25 and 50 μM). RB-TF could potentially increase selectivity toward cancer cells. Considering the outcomes of the characterization and cytotoxicity studies performed on RB-TF, we conclude that RB-TF represents a valid potential alternative tool to fight against primary melanoma lesions via dermal delivery in the absence of light.
Cutaneous melanoma is one of the most aggressive and metastatic forms of skin cancer. However, current therapeutic options present several limitations, and the annual death rate due to melanoma increases every year. Dermal delivery of nanomedicines can effectively eradicate primary melanoma lesions, avoid the metastatic process, and improve survival. Rose Bengal (RB) is a sono-photosensitizer drug with intrinsic cytotoxicity toward melanoma without external stimuli but the biopharmaceutical profile limits its clinical use. Here, we propose deformable lipid nanovesicles, also known as transfersomes (TF), for the targeted dermal delivery of RB to melanoma lesions to eradicate them in the absence of external stimuli. Considering RB's poor ability to cross the stratum corneum and its photosensitizer nature, transfersomal carriers were selected simultaneously to enhance RB penetration to the deepest skin layers and protect RB from undesired photodegradation. RB-loaded TF dispersion (RB-TF), prepared by a modified reverse-phase evaporation method, were nanosized with a ζ-potential value below -30 mV. The spectrophotometric and fluorimetric analysis revealed that RB efficiently interacted with the lipid phase. The morphological investigations (transmission electron microscopy and small-angle X-ray scattering) proved that RB intercalated within the phospholipid bilayer of TF originating unilamellar and deformable vesicles, in contrast to the rigid multilamellar unloaded ones. Such outcomes agree with the results of the in vitro permeation study, where the lack of a burst RB permeation peak for RB-TF, observed instead for the free drug, suggests that a significant amount of RB interacted with lipid nanovesicles. Also, RB-TF proved to protect RB from undesired photodegradation over 24 h of direct light exposure. The ex vivo epidermis permeation study proved that RB-TF significantly increased RB's amount permeating the epidermis compared to the free drug (78.31 vs 38.31%). Finally, the antiproliferative assays on melanoma cells suggested that RB-TF effectively reduced cell growth compared to free RB at the concentrations tested (25 and 50 μM). RB-TF could potentially increase selectivity toward cancer cells. Considering the outcomes of the characterization and cytotoxicity studies performed on RB-TF, we conclude that RB-TF represents a valid potential alternative tool to fight against primary melanoma lesions via dermal delivery in the absence of light.
Entities:
Keywords:
dermal delivery; liposome; melanoma; nanoparticle; rose bengal; skin cancer
According
to the Italian Association for Cancer Research (AIRC),
cutaneous melanoma represents only 5% of skin cancers. Nevertheless,
its ability to rapidly metastasize makes melanoma the most aggressive
and deadly form of skin cancer. It remains a significant health problem
worldwide, with death often occurring due to metastasis.[1] Statistics predicted that around 106,110 cases
of melanoma would be diagnosed in the United States in 2021, and about
7,180 people are expected to die ;[2] also,
the incidence of invasive melanoma in European regions showed an average
annual increase of 4.0% in men and 3.0% in women during the 1995–2012
period.[3] Cutaneous melanoma typically localizes
in the epidermis’ bottom layers or deeper in the dermis and
originates from melanocytes’ tumor transformation. Depending
on the location and stage, the primary cutaneous melanoma can be treated
via surgical resection but it cannot be applied in all cases. Current
therapeutic approaches, including chemotherapy, radiotherapy, immunotherapy,
and photodynamic therapy, have reported two main limitations: adverse
effects (usually related to an immune reaction and lack of specificity)
and induced resistance to immune–chemotherapeutics or intralesional
therapy.[4] Thus, better therapeutic options
are required. For this purpose, primary melanoma lesions can be effectively
eradicated via dermal delivery of therapeutics, increasing patient
compliance. Indeed, the dermal route offers direct access to melanoma
cells avoiding systemic administration and its disadvantages. Considering
the complexity of human skin, the challenge in developing an effective
dermal delivery system is to bypass the skin barrier and target the
drug only to cancer cells.[1,5]Rose Bengal (RB)
(3′,4′,5′,6′-tetrachloro-2,4,5,7-tetraiodofluorescein)
is a dye with a xanthenic structure mainly used in ophthalmology as
a diagnostic tool[6] (Figure ).
Figure 1
Rose Bengal chemical structure. Created with BioRender.com.
Rose Bengal chemical structure. Created with BioRender.com.Moreover, RB is a sono-photosensitizer drug employed in sono-photodynamic
therapy and demonstrated intrinsic cytotoxicity against tumor and
microbial cells.[6] Of relevant importance
in this context is RB’s antimelanoma activity in the absence
of external stimuli, including light or ultrasounds. In particular,
RB was reported to induce death in different cultured melanoma cell
lines, probably via necrosis, even if both caspase-dependent and -independent
apoptotic pathways were observed.[7,8] PV-10 is a
10% RB solution currently tested to treat melanoma after intralesional
injection. PV-10 acts through a dual mechanism: it first induces chemical
ablation of the tumor and a second systemic effect following the onset
of a tumor-specific immune response.[9,10] Therefore,
RB can be proposed as a valid alternative for both local and metastatic
melanoma.Despite its potential, RB’s clinical application
is limited
by its biopharmaceutical profile. RB (employed in the disodium salt
form) is an amphiphilic and water-soluble molecule with a molecular
weight of 1017.64 g mol–1, presenting two negative
charges in solution.[6] For an efficient
permeation through the skin layers, a drug first needs to pass the
stratum corneum (SC), which is the main barrier against the penetration
of external agents. Considering the anionic nature and the high molecular
weight, RB would not easily pass the SC and therefore cannot be considered
a drug candidate suitable for the cutaneous administration route.[11,12] In addition, RB suffers from poor cell crossing hampering suitable
accumulation in the target cells. Nevertheless, nano-based delivery
systems have proved to overcome the RB limits mentioned above efficiently.[6]Lipid-based nanosystems were widely employed
for the dermal delivery
of photosensitizer drugs.[13,14] Among these, transfersomes
(TF) are considered the most innovative dermal and transdermal carriers
to date.[15] TF are liposome-like vesicles
consisting of a hydrophilic core surrounded by a hydrophobic bilayer
but the additional surfactant present in the phospholipid arrangement
provides ultra flexibility.[16] A conventional
liposome presents the disadvantage of poor penetration into the viable
skin, limiting its therapeutical application to the diseases involving
outermost skin layers. Because of their composition, the elasticity
of TF increases, making them squeeze and pass through skin pores smaller
than their size. Considering that TF tend to avoid dry surroundings,
the sufficient force to drive them through the skin is generated by
the transdermal hydration gradient, the increasing water concentration
gradient from the superficial to the inner skin strata. In conventional
liposomes, the rigid structure hampers the migration as they require
high energy to deform. On the other hand, TF can deform without losing
their integrity, and undesirable leakage and drug loss are avoided.
As a result, the drug is efficiently delivered in the deepest region
of the skin.[17,18] Although the mechanism above
is considered the primary one operating, other mechanisms can be involved
in the transfersomal action.[18,19]The current work
aims to provide a dermal delivery of RB to melanoma
lesions via optimizing its biopharmaceutical profile and enhancing
RB’s intrinsic antimelanoma activity in the absence of light
or ultrasounds. To achieve this goal, RB has been formulated in TF
made of phosphatidylcholine (Lipoid S 100), cholesterol, and Span
80. RB-loaded TF were characterized in dimensional properties, ζ-potential,
and morphology; in addition, the storage stability and photostability
of RB-loaded TF and corresponding blank formulation were determined.
Spectrophotometric, fluorimetric, and small-angle X-ray scattering
(SAXS) analyses were performed to evaluate the interaction between
the dye and the lipid phase of vesicles. Ex vivo epidermis permeation
experiment determined TF’s ability to permeate across the epidermal
barrier reaching the dermis. Finally, an in vitro toxicity study on
melanoma cells (SK-MEL28) was carried out to investigate the new RB
delivery system’s antimelanoma efficacy.
Materials
and Methods
Materials
Rose Bengal sodium salt
(RB), cholesterol, Span 80, and ethanol were purchased by Sigma-Aldrich
(St. Louis, MO). Lipoid S 100 was gifted by Lipoid GmbH (Ludwigshafen,
Germany). Acetonitrile and dimethylsulfoxide (DMSO) were acquired
from Merck (Darmstadt, Germany). Phosphate-buffered saline (PBS, NaCl
0.138 M; KCl 0.0027 M; pH 7.4; 25 °C) was obtained by Sigma-Aldrich
(Milan, Italy). Ultrapure bidistilled water was obtained by a MilliQ
R4 system, Millipore (Milan, Italy).
Preparation
and Characterization of TF
TF Preparation
A previous preformulation
study set the most suitable manufacturing parameters to prepare unloaded
and RB-loaded TF (Supporting Information), including the preparative technique, the choice of the organic
solvent and the sonication technique, and time.RB-loaded TF
dispersion (RB-TF) was prepared by a slightly modified reverse-phase
evaporation method (REV).[20] The lipid phase
consisting of a mixture of 400 mg of Lipoid S 100 (phosphatidylcholine),
75 mg of cholesterol, and 40 μL of Span 80 was dissolved in
7 mL of ethanol at 50 °C and mixed with 10 mL of an aqueous solution
(MilliQ water) containing 5 mg of RB. After sonication treatment using
a probe sonicator Bioblock Vibracell (Fisher Bioblock Scientific,
Illkirch, France) for 30 s at 50% ultrasound (US) amplitude, the resulting
dispersion was placed in a dry, round-bottom flask. Ethanol was removed
under vacuum (Rotavapor RE111, Büchi Labortechnik AG, Flawil,
Switzerland) at 50 °C, and the vesicles were swollen for 1 h
at room temperature and sonicated by three probe sonication cycles:
each cycle consisted of 10 s of US followed by an interval of 20 s.[21] Finally, RB-TF dispersion was extruded 10 times
through a regenerated cellulose syringe filter (pore size: 0.45 μm,
filter size: 25 mm, AlfaTech, Genova, Italy) and stored at 4 °C.
The dispersion of corresponding unloaded vesicles (b-TF) was prepared.
Particle Size and ζ-Potential Analysis
Dimensional analyses of RB-TF and b-TF were performed by photon
correlation spectroscopy (PCS). A Coulter nanosizer N5 (Beckman-Coulter
Inc., Miami, FL) was used to determine the hydrodynamic diameter and
the polydispersity index (PDI) to measure the dimensional heterogeneity
of the sample. Before each analysis, all samples were diluted adequately
with MilliQ water previously filtered (regenerated cellulose syringe
filter, pore size: 0.20 μm, filter size: 15 mm, Albet LabScience,
Dassel, Germany) to ensure light-scattering intensity within the required
range of the instrument (between 5 × 104 and 1 ×
106 counts s–1). Particle size was calculated
in unimodal using the following conditions: fluid refractive index
1.333; temperature 25 °C; viscosity 0.890 cP; angle of measurement
90°; sample time 3.0 ms; and sample run time 300 s. ζ-Potential
was measured using the Zetasizer Nano (Malvern Instrument, Worcestershire,
United Kingdom) through the M3-PALS (Phase Analysis Light Scattering)
technique. Just before the analysis, the formulations were diluted
with distilled water.
Drug Content
The RB content in
the RB-TF dispersion was evaluated as described here. Thirty microliters
of the RB-TF dispersion was diluted up to 2 mL with acetonitrile under
magnetic stirring to dissolve the nanovesicles and extract RB. Successively,
the RB content was measured with a UV-spectrophotometer (Shimadzu
UV-1800, Kyoto, Japan) and calculated referring to the calibration
curve prepared in acetonitrile (standard solution in the range of
1–10 mg L–1; y = 101610959x + 0.020676712; R2 = 0.999).
Finally, the drug content (DC%) was determined according to eq
Transmission
Electron Microscopy (TEM)
RB-TF and b-TF were analyzed through
transmission electron microscopy
(TEM) to investigate the vesicles’ morphology. A drop of sample
and an equal volume of an aqueous 1% phosphotungstic acid solution
were adsorbed on the surface of a carbon-coated copper grid (200 mesh).
The vesicles were observed after drying at room temperature using
a JEOL JEM 1400 Plus (JEOL Ltd., Tokyo, Japan) with an accelerating
voltage of 80 kV in the bright-field mode.
Degree
of Deformability
Deformability
tests of b-TF and RB-TF were performed using a modified extrusion
device[22] illustrated in Figure .
Figure 2
Schematic illustration
of the modified extrusion device employed
to evaluate the deformability indexes of RB-TF and b-TF: (A) 500 g
calibration weight; (B) weight support; (C) syringe; (D) support for
the membrane filter (0.2 μm pore size); and (E) collecting beaker.
Created with BioRender.com.
Schematic illustration
of the modified extrusion device employed
to evaluate the deformability indexes of RB-TF and b-TF: (A) 500 g
calibration weight; (B) weight support; (C) syringe; (D) support for
the membrane filter (0.2 μm pore size); and (E) collecting beaker.
Created with BioRender.com.The samples (2 mL) were withdrawn with a syringe
successively connected
to a membrane filter with a pore size of 0.2 μm (regenerated
cellulose membrane filter, filter size: 47 mm, Whatman, GE Healthcare
Life Sciences, Buckinghamshire, United Kingdom);[23,24] extrusion process was performed by constantly applying a calibration
weight of 500 g on the top of the syringe. Particle size was determined
just before and after experimenting; deformability index was measured
following eq (25)where D is the deformability
index of nanovesicles; J is the amount of formulation
extruded in 5 min; rv is the particle
size after the experiment; and rp is the
membrane pore size.
Small-Angle X-ray Scattering
(SAXS)
SAXS was recorded with an S3-MICRO SWAXS camera system
(HECUS X-ray
Systems, Graz, Austria). A GeniX X-ray generator, operating at 1 mA
and 50 kV, provided a Cu Kα radiation of 1.542 Å wavelength.
The scattered X-rays were detected in the small-angle region by a
1D-PSD-50 M system (Hecus X-ray Systems, Graz, Austria) containing
1024 channels of 54.0 mm width. The working q-range
(Å) was 0.002 ≤ q ≤ 0.06, with q = 4π sin(θ)λ–1 being the modulus of the scattering wave vector. Glass capillaries
of 2 mm were used in experiments while diffraction patterns were recorded
for 10 800 s. Scattering from the air was minimized, keeping
the camera volume under vacuum during measurements. Silver behenate
(CH3–(CH2)20–COOAg),
with a d spacing value of 58.38 Å was the standard
for calibration of the angular scale of the measured intensity. The
SAXS pattern of RB-TF was analyzed by GAP (Global Analysis Program),
which allows the fitting of bilayer-based structures.[19,26] Particularly, the membrane thickness (dB) was defined as 2(ZH + 2σH), where ZH and σH are parameters obtained from SAXS curve fitting and, respectively,
represent the head group-to-bilayer center distance and the polar
head amplitude. The latter parameter was kept fixed at 3 A° as
suggested by the software developers.[26]
Evaluation of the Interaction between RB and
the Lipid Phase
Studies on absorption (Abs) and emission
(Ems) spectra of (i) RB aqueous solution, (ii) RB-TF dispersion, and
(iii) RB added in b-TF dispersion were recorded as previously proposed
by Chang et al.,[27]. Abs spectra were measured
with a UV-Spectrophotometer (Shimadzu UV-1800, Kyoto, Japan); and
Ems spectra were recorded with an RF-600 spectrofluorometer (Shimadzu,
Kyoto, Japan), exciting each sample at 549 nm. Before each measurement,
all samples were diluted with MilliQ water previously filtered (regenerated
cellulose syringe filter, pore size: 0.20 μm, filter size: 15
mm, Albet LabScience, Dassel, Germany) up to 7.5 mg L–1 RB concentration. Spectra of b-TF dispersion were recorded following
the same procedure.
Stability Studies
Storage Stability
b-TF and RB-TF
dispersions were stored for 60 days at 4 °C, protected from light.
At each predetermined time point (1, 3, 7, 15, 30, 60 days), samples
were analyzed in terms of dimensional properties and ζ-potential
as described in Section .
Chemical Stability
The chemical
stability of RB-TF dispersion was evaluated in terms of RB content
over time and compared with the RB aqueous solution after storing
samples at 4 °C protected from light. Samples were analyzed at
each predetermined time point (1, 3, 7, 15, 30, 60 days), as described
in Section . The RB amount was calculated for the RB aqueous solution, referring
to the calibration curve prepared in water (standard solution in the
range of 1–20 mg L–1; y =
0.10640119x + 0.00531086; R2 = 0.999).
Photostability
The photostability
of RB-TF dispersion was evaluated and compared with the RB aqueous
solution. One milliliter of each sample (0.5 mg of RB) was exposed
to light in the visible region delivered from an artificial daylight
lamp (220 V, 40 W) over 24 h at room temperature. Photodegradation
of RB was monitored at each predetermined time point (1, 2, 3, 6,
24 h) in terms of RB content by UV-vis spectrophotometry. The RB content
in RB-TF dispersion was determined as described in Section ; for RB aqueous solution,
the amount of RB was calculated referring to the calibration curve
prepared in water as mentioned previously.
In Vitro Release Study
The in vitro
release profile of RB-TF dispersion was evaluated across a polycarbonate
membrane (0.050 μm pore size, 47 mm diameter, Sigma-Aldrich,
St. Louis, MO) using a dissolution apparatus (DT 70, Erweka, Langen,
Germany), as previously described by Gavini et al.[28] The membrane was mounted on the bottom of a cylindrical
plastic support consisting of a tube (height = 1.91 cm, diameter =
2.28 cm) connected to a drive shaft of the dissolution apparatus (Supporting Information). The membrane was clamped
to the support by a plastic ring, and then 2 mL of the sample (1 mg
of RB) was placed on the surface of the membrane. The system was then
inserted into the vessel containing 250 mL of PBS as the acceptor
medium, keeping the membrane in contact with the surface of the PBS
all the time. The system was continuously stirred at 100 rpm and thermostated
at 32 °C; it was allowed to equilibrate for 30 min before starting
the experiment. The samples of the acceptor medium (3 mL) were collected
at each predetermined time point (0.08, 0.17, 0.25, 0.5, 1, 2, 3,
6, 24, 32, 48 h); in the case of RB-TF dispersion, acetonitrile was
used to ensure the complete recovery of RB. The RB aqueous solution
was also tested as a comparison. The amount of dye in the acceptor
medium was measured by UV–vis spectrophotometry and calculated
using the calibration curve prepared in acetonitrile for RB-TF dispersion
and in water for RB. An equal volume of the fresh medium was immediately
replaced after each sampling. The cumulative amount of RB was plotted
against time and determined through eq where Q is the
cumulative amount of the drug; C is the
drug concentration of the acceptor medium at each time point; V0 is the acceptor medium’s volume; C is the drug concentration of the sample at
each time point; and V is the volume
of the sample collected at each time point.
Ex Vivo
Epidermis Permeation and Retention
Study
Ex vivo permeation of RB-TF dispersion and RB aqueous
solution was performed across epidermal membranes excised from porcine
ears. Adult pig ears were obtained from a local slaughterhouse (Milia
S.r.L, Approval Number CE IT 1856 M (Regulation EC 853/2004)). Epidermal
membranes, comprising viable epidermis and stratum corneum, were prepared
by the heat separation technique described here:[29] hairs of ears were removed using a hair clipper; shaved
ears were immersed in water at 60 °C for about 2 min; following
removal from the water, the epidermis was gently peeled off. The experiment
was performed using a 12-multiwell cell culture plates suitability
modified[30] (project INCREASE SARDINIA 2016–17,
protocol number 31351, University of Sassari) as illustrated in Figure .
Figure 3
Schematic illustration
of the diffusion apparatus (project INCREASE
SARDINIA 2016–17, protocol number 31351, University of Sassari)
employed to evaluate the ex vivo epidermis permeation profile of
RB-TF dispersion and RB aqueous solution. Created with BioRender.com.
Schematic illustration
of the diffusion apparatus (project INCREASE
SARDINIA 2016–17, protocol number 31351, University of Sassari)
employed to evaluate the ex vivo epidermis permeation profile of
RB-TF dispersion and RB aqueous solution. Created with BioRender.com.Each well had an effective diffusion area of 1 cm2.
Wells were filled with 5.5 mL of PBS (pH. 7.4) as an acceptor medium,
and the epidermis was mounted on the plates with the inner side facing
PBS. RB-TF dispersion (0.3 mL, 0.15 mg of RB) was added on the top
of the epidermis and the plates were incubated at 32 °C (SKI
4 Shaker Incubator, Argo Lab, Carpi, Italy). The system was allowed
to equilibrate for 30 min before starting the experiment. Samples
(0.2 mL) were withdrawn at each predetermined time point (0.25, 0.5,
1, 3, 5, 8, 24 h) from a sampling port directly connected to the receptor
chamber; successively, the samples were added to 1 mL of DMSO to dissolve
both lipids of RB-TF dispersion and skin to extract RB completely.
The amount of RB permeated was measured by UV–vis spectrophotometry
and calculated using the calibration curve prepared in DMSO (standard
solution in the range of 2–12 mg L–1; y = 87.814x – 0.1041, R2 = 0.998). After each sampling, an equal volume of fresh
medium was immediately replaced through the sampling port previously
employed to withdraw the sample. The same procedure was applied to
evaluate the ex vivo permeation profile of the RB aqueous solution.
The cumulative amount of RB permeated was plotted against time and
determined as described in Section .At the end of the permeation experiment, the
epidermis was carefully
removed from the plate and cut into small pieces, added to 2 mL PBS,
and boiled for 10 min; after that, 2 mL of DMSO was added to ensure
RB extraction and further boiled for 10 min. The amount of RB retained
in the tissue was measured with a UV–vis spectrophotometer
and calculated using the DMSO calibration curve.
Cytotoxicity and Antiproliferative Studies
The antiproliferative
and cytotoxic activity of b-TF, RB-TF, and
RB aqueous solution at different concentrations (12.5–50 μM)
were evaluated on SK-MEL28 melanoma cells; the HFFF2 human fetal foreskin
cell line was tested as a control on normal cells. Cells were cultured
in Dulbecco’s modified Eagle’s medium (DMEM) (Sigma-Aldrich
D5671) supplemented with 10% fetal bovine serum (Euroclone ECS0180L),
2 mM l-glutamine (VWR X0550), 1 mM sodium pyruvate (Sigma-Aldrich
S8636), nonessential amino acids (Sigma-Aldrich M7145), 100 units
mL–1 penicillin, 10 μg mL–1 streptomycin, and 25 ng mL–1 amphotericin B (AA,
VWR L0010) at 37 °C with 5% of CO2. Two thousand
cells per well were plated in 384-well microplates and incubated for
24 h at 37 °C with 5% CO2; the day after,
5 μL of each formulation was added to samples. After 48 h of
treatment, cell death was estimated by measuring green fluorescence
intensity, provided by staining dead cells with CellTox Green dye
(Promega), and cell viability was evaluated by CellTiter-Glo kit (Promega),
following manufacturer’s instructions. A second plate was prepared
in parallel to assess cell viability at the time of treatment.
Statistical Analysis
Statistical
analysis was done with Graph Pad Prism 8.0 software (GraphPad Software
Inc. San Diego, CA). The variance analysis (one-way analysis of variance
(ANOVA)) was used to analyze the data, followed by Tukey’s
multiple comparison test. Differences were considered significant
for p < 0.05.
Results
Preparation and Characterization of TF
The TF dispersion
was milky, white-colored in the case of b-TF, and
pink-colored for RB-TF dispersion; no phase separation or aggregation
phenomena were observed. The particle size and PDI (Table ) indicate that b-TF were in
a nanosize range and homogenous (PDI < 0.4); also, b-TF were spherical
and multilamellar as seen through TEM (Figure ). RB-TF showed a PDI similar to b-TF one
(p > 0.05), proving that encapsulating RB did
not
perturb the system’s dimensional homogeneity. On the other
hand, a slight increase in the particle size was observed compared
to b-TF (p < 0.01). In addition, nanovesicles
surface charge expressed as ζ-potential measurements decreased
from a slightly negative value to a highly negative one (p < 0.0001) following RB loading (Table ). TEM images (Figure ) revealed a morphological difference between
the two formulations, as b-TF were multilamellar vesicles (MLV) whereas
RB-TF were spherical large unilamellar vesicles (LUV). Also, the SAXS
experiments evidenced the differences in terms of lamellarity between
the two formulations. Indeed, the diffractogram related to b-TF (Figure ) revealed the presence
of two strong Bragg reflections superimposed to a barely visible diffusive
scattering. While the latter was expected when nanoparticles dispersion
was analyzed, the observed Bragg peaks proved, beyond any doubt, the
high lamellarity of the vesicles. The average inter-bilayer distance
(dav) of 6 nm was calculated from the
Bragg relation dav = 2πh/q, where h is the Miller index
and q is the position of the Bragg peaks. On the
other hand, the SAXS profile of RB-TF was characterized by a simple
diffusive scattering, indicating the absence of lamellarity. To get
deeper insights into the TF nanostructure, the double-layer thickness
(dB) was measured in both b-TF and RB-TF.
In the case of b-TF, dB (indicated by arrows in Figure A) was measured exploiting the TEM images
using the ImageJ program and it was found equal to 50 Å. Unfortunately,
the same analysis cannot be performed on RB-TF due to the low resolution
(see Figure B). Therefore,
in that case, dB was extracted by fitting
the SAXS diffractogram using the Global Analysis Program (GAP, see Section ). The GAP analysis
yielded ZH = 18 Å. Therefore, a double-layer
thickness of 48 Å was calculated, in good agreement with that
measured in b-TF liposomes and other similar nanoparticles reported
in the literature.[31] This finding evidenced
that the addition of RB to the formulation did not significantly modify
the transfersome double-layer thickness, although an evolution from
MLV to LUV was observed.
Table 1
Characteristics
of b-TF and RB-TFa
formulation
particle size (nm)
PDI
ζ-potential (mV)
loading efficiency (%)
deformability index
b-TF
193.10 ± 7.53**
0.175 ± 0.004
–4.9 ± 0.9***
not deformable
RB-TF
206.42 ± 2.67
0.200 ± 0.024
–45.90 ± 0.85
94.50 ± 3.20
1.92 ± 0.06
Results are expressed as mean value
± standard deviation (n = 6); deformability
index n = 3. **p value < 0.01
vs RB-TF; ***p value < 0.0001 vs RB-TF.
Figure 4
TEM images of b-TF (A) and RB-TF (B). Scale
bar: 200 nm; magnification
×30k (A) and ×40k (B). Red arrows show the thickness of
the lipid double layer (A).
Figure 5
SAXS diffractograms
of b-TF and RB-TF.
TEM images of b-TF (A) and RB-TF (B). Scale
bar: 200 nm; magnification
×30k (A) and ×40k (B). Red arrows show the thickness of
the lipid double layer (A).SAXS diffractograms
of b-TF and RB-TF.Results are expressed as mean value
± standard deviation (n = 6); deformability
index n = 3. **p value < 0.01
vs RB-TF; ***p value < 0.0001 vs RB-TF.Particle size and PDI of RB-TF did
not change after the deformability
test (p > 0.05) (size: 195.70 ± 0.95 vs 196.07
± 0.31; PDI: 0.375 ± 0.002 vs 0.387 ± 0.011), whereas
the size of b-TF significantly decreased, revealing no deformable
vesicles (p < 0.01) (size: 226.67 ± 2.80
vs 217.20 ± 2.51; PDI: 0.215 ± 0.012 vs 0.239 ± 0.016).
Although the membrane pore size employed in the deformability test
did not vary much with the particle size of the tested formulation,
RB-TF revealed elastic properties since no change in the dimensional
profile was experienced, contrary to the unloaded formulation.
Evaluation of the Interaction between RB and
Lipid Phase
Two analysis techniques were used to evaluate
RB’s ability to interact with lipid nanovesicles, including
spectrophotometry and fluorimetry. Figure reports Abs and Ems spectra of RB in the
450–700 nm range in distinct molecular environments.
Figure 6
Absorption
and emission spectra of RB (7.5 mg L–1) included
in different molecular environments. RB aqueous solution
(black line), b-TF (purple line), RB added to b-TF (green line), and
RB-TF (red line).
Absorption
and emission spectra of RB (7.5 mg L–1) included
in different molecular environments. RB aqueous solution
(black line), b-TF (purple line), RB added to b-TF (green line), and
RB-TF (red line).The spectra demonstrated
that RB Abs and Ems λmax are related to the composition
of the environment: 549 nm (Abs)
and 568 nm (Ems) for RB aqueous solution; 562 (Abs) and 582 (Ems)
for both RB added to b-TF and RB-TF; and no peak in Abs or Ems was
recorded for b-TF. Both RB Abs λmax and Ems λmax exhibited a shift to a longer wavelength (redshift or bathochromic)
when forced to interact with TF. The Abs spectra displayed a slight
increase in the RB maximum absorption peak intensity depending on
the formulation. In the Ems case, this increase is evident comparing
the RB aqueous solution to RB-TF and RB added to b-TF.
Stability Study
The diameter and
PDI of TF following storage at 4 °C over 60 days are illustrated
in Figure .
Figure 7
Storage stability.
Particle sizes and PDIs of b-TF and RB-TF following
storage at 4 °C over 60 days. Results represent the average value
of six independent measurements for each formulation (n = 6). PDI (**) and particle size (••) of b-TF at 0
day vs 60 days: p value < 0.01; particle size
of RB-TF at 0 day vs 60 days: p value < 0.0001(ΔΔΔ).
Storage stability.
Particle sizes and PDIs of b-TF and RB-TF following
storage at 4 °C over 60 days. Results represent the average value
of six independent measurements for each formulation (n = 6). PDI (**) and particle size (••) of b-TF at 0
day vs 60 days: p value < 0.01; particle size
of RB-TF at 0 day vs 60 days: p value < 0.0001(ΔΔΔ).Encapsulating RB in TF affected the mean particle
size and PDI
of the system over time. The PDI of b-TF increased from 0.175 ±
0.003 nm at the moment of preparation to 0.437 ± 0.032 nm after
60 days (p < 0.01) in a progressive manner; the
PDI of RB-TF proved to be reasonably constant during the first 4 weeks,
and an irrelevant increase was observed at 60 days, reaching 0.235
± 0.015 (p > 0.05). Both formulations displayed
a reduction in the particle size during storage time: b-TF decreased
to 181.08 ± 7.40 nm (p < 0.01) and RB-TF
to 164.55 ± 3.25 nm (p < 0.0001). For RB-TF,
parallel to changes in the dimensional profile, a reduction of ζ-potential
was observed: values decreased from −45.2 ± 1.4 to −35.6
± 1.6 mV at 60 days (p < 0.0001).The
chemical stability test was performed to determine if any interaction
between RB and the components of the formulation could occur over
time, leading to a degradation of the drug itself. The RB content
over time did not vary for both RB aqueous solution and RB-TF dispersion
(p > 0.05), concluding that no undesired loss
of
RB occurred and that RB-TF is chemically stable.Figure reports
the residual amount of RB in the RB aqueous solution and RB-TF over
24 h of irradiation under visible light.
Figure 8
Photostability study.
The residual RB in RB aqueous solution and
RB-TF dispersion after 24 h of irradiation with visible light. The
results represent the mean values of three independent experiments
for each formulation (n = 3). Initial free RB amount
vs free RB amount at 1, 2, 3, and 6 h: p value <
0.01(**); initial free RB amount vs free RB amount at 24 h: p value < 0.0001 (•••).
Photostability study.
The residual RB in RB aqueous solution and
RB-TF dispersion after 24 h of irradiation with visible light. The
results represent the mean values of three independent experiments
for each formulation (n = 3). Initial free RB amount
vs free RB amount at 1, 2, 3, and 6 h: p value <
0.01(**); initial free RB amount vs free RB amount at 24 h: p value < 0.0001 (•••).Photostability measurements confirmed that the RB aqueous
solution
undergoes photodegradation: after 1 h, the RB content decreased to
91.63 ± 4.75% (p < 0.01); at 6 h, the RB
content was 92.11 ± 0.9% (p < 0.01) and reached
83.09 ± 1.49% at the end of 24 h (p < 0.0001).
On the other hand, RB-TF dispersion efficiently protected RB from
visible light over 24 h: at the end of the experiment, the RB content
in RB-TF was reported to be 95.05 ± 1.49% (p > 0.05).Figure depicts
the in vitro release
profile of RB-TF dispersion and the cumulative amount of RB aqueous
solution in the acceptor medium. The results represent the mean values
of three independent experiments for each formulation over 48 h, following
a single dose of RB aqueous solution and RB-TF dispersion (RB = 1
mg).
Figure 9
In vitro release profiles of free RB and RB-TF dispersion. The
cumulative amount of RB aqueous solution (black line) and RB-TF (red
line) recovered in the acceptor medium over 48 h (n = 3).
In vitro release profiles of free RB and RB-TF dispersion. The
cumulative amount of RB aqueous solution (black line) and RB-TF (red
line) recovered in the acceptor medium over 48 h (n = 3).As data proved, when RB aqueous
solution was tested, 51.43 ±
0.15% of the dye was detected within 5 min, and 91.82 ± 0.3%
in 1 h, reaching 99.60 ± 0.3% at the end of the experiment. On
the contrary, the RB-TF dispersion release rate was slower than that
of RB aqueous solution: the maximum RB amount released was 54.81 ±
0.25%, reached after 32 h.The lack of a burst RB release for
RB-TF dispersion suggests that
a significant amount of RB interacted with lipid nanovesicles, and
thus, it is not in solution such as in RB aqueous solution.
Ex Vivo Epidermis Permeation and Retention
Study
The ex vivo permeation and retention studies were carried
out to predict the delivery performance of RB-TF dispersion across
the epidermis compared to RB aqueous solution. Figure reports the average values of RB permeated
through the epidermis and RB retained over 24 h, following a single
dose of RB aqueous solution and RB-TF dispersion (RB = 0.5 mg). The
results represent the average of three independent experiments for
each formulation.
Figure 10
Ex vivo epidermis permeation and retention profiles of
RB aqueous
solution and RB-TF dispersion. (A) The cumulative amount of RB aqueous
solution (black line) and RB-TF dispersion (red line) permeated through
the epidermis over 24 h (n = 3). RB-TF dispersion
permeated after 24 h vs RB aqueous solution permeated after 24 h: p value < 0.0001(***). (B) Amount of RB aqueous solution
and RB-TF dispersion retained by the epidermis (full green bar) and
totally permeated (striped bar) at the end of the ex vivo permeation
test (n = 3). RB-TF retained by the epidermis and
RB aqueous solution retained by the epidermis: p <
0.0001(•••).
Ex vivo epidermis permeation and retention profiles of
RB aqueous
solution and RB-TF dispersion. (A) The cumulative amount of RB aqueous
solution (black line) and RB-TF dispersion (red line) permeated through
the epidermis over 24 h (n = 3). RB-TF dispersion
permeated after 24 h vs RB aqueous solution permeated after 24 h: p value < 0.0001(***). (B) Amount of RB aqueous solution
and RB-TF dispersion retained by the epidermis (full green bar) and
totally permeated (striped bar) at the end of the ex vivo permeation
test (n = 3). RB-TF retained by the epidermis and
RB aqueous solution retained by the epidermis: p <
0.0001(•••).The amount of RB aqueous solution permeated through the epidermis
was 24.77 ± 0.88% after 1 h, and it increased to 38.31% at the
end of 24 h. On the other hand, RB-TF dispersion was found to permeate
by 55.40 ± 3.93% within 15 min, reaching its maximum after 8
h (73.99 ± 2.49%). At 24 h, an irrelevant increase of RB-TF dispersion
permeation was observed (p > 0.05). In parallel,
the drug amount detected in the epidermal layer after 24 h was significantly
different for RB aqueous solution and RB-TF dispersion (p < 0.0001): 54.00 ± 2.37% of RB aqueous solution was retained
by the skin, whereas RB-TF dispersion allowed decreasing RB retention
to 22.08 ± 1.14%. An ex vivo permeation study proved that RB-TF
dispersion doubled RB’s amount that permeates the epidermis
in 24 h, limiting the skin deposition phenomena.The impact
of RB aqueous solution and RB-TF on cell death and viability
was evaluated on SK-MEL28 and HFFF2 cells (Figure ). After 48 h, no cell death induced by
the formulations was observed (data not shown). Both cell lines displayed
a dose-dependent reduction of growth response to RB aqueous solution
and RB-TF. The data suggested that at both concentrations of 25 and
50 μM, the RB-TF cell growth reduction was significantly higher
than RB aqueous solution (p < 0.05). At a concentration
of 50 μM, RB aqueous solution inhibited the percentage of growth
of SK-MEL 28 and HFFF2 without selectivity (p >
0.05);
on the other hand, RB-TF displayed a potential selectivity for SK-MEL28
at this concentration (p = 0.05). On the contrary,
no growth reduction was noticed in b-TF, which instead promoted cell
growth.
Figure 11
Effects of RB aqueous solution, RB-TF, and b-TF on the SK-MEL28
and HFFF2 cell growth. Cells were cultured with samples for 48 h.
(A) The viability of each cell line depending on the formulation and
the concentration tested. (B) Analysis of each formulation’s
impact at different concentrations, comparing the growth suppression
of the two cell lines. The effect of RB aqueous solution (25 μM)
on SK-MEL28 vs the effect of RB-TF (25 μM) on SK-MEL28: p value < 0.05 (*). The effect of RB aqueous solution
(50 μM) on SK-MEL28 vs the effect of RB-TF (50 μM) on
SK-MEL28: p value < 0.05 (•).
Effects of RB aqueous solution, RB-TF, and b-TF on the SK-MEL28
and HFFF2 cell growth. Cells were cultured with samples for 48 h.
(A) The viability of each cell line depending on the formulation and
the concentration tested. (B) Analysis of each formulation’s
impact at different concentrations, comparing the growth suppression
of the two cell lines. The effect of RB aqueous solution (25 μM)
on SK-MEL28 vs the effect of RB-TF (25 μM) on SK-MEL28: p value < 0.05 (*). The effect of RB aqueous solution
(50 μM) on SK-MEL28 vs the effect of RB-TF (50 μM) on
SK-MEL28: p value < 0.05 (•).
Discussion
The current work aimed to
determine if a proper delivery system
can enhance the antimelanoma intrinsic activity of Rose Bengal. Considering
the localization of primary melanoma tumor, the dermal administration
was here investigated as it represents the most direct and noninvasive
access route to cancer cells, obviating the need for intralesional
injection. We developed deformable lipid nanovesicles to vehicle RB
across the epidermis and to reach the dermal layer. In this way, RB-TF
could potentially eradicate melanoma lesions at early stages localized
in the outermost layer of the skin (melanoma in situ) and localized
but invasive melanoma, which advances deeper in the dermis.[32]Based on the high water solubility of
RB disodium salt, TF were
prepared using the modified reverse-phase evaporation (REV) technique.[20] This method allows obtaining vesicles with a
high aqueous space-to-lipid ratio and, consequently, to entrap a large
percentage of drug solubilized in the aqueous phase.[33] The original REV technique, first reported in 1978 by Szoka
et al.,[34] was used to study several phospholipids,
either pure or mixed with other lipids, mainly involving diethyl ether,
isopropyl ether, and chloroform as solvents. Herein, the lipid phase
was made of phosphatidylcholine, cholesterol, and Span 80 as the surfactant.
Cholesterol was added to improve liposomes’ resistance to leakage
and degradation in vivo, as it is known to provide rigidity to the
structure;[35] simultaneously, the presence
of the surfactant destabilizes the lipid bilayer, increasing the vesicle’s
deformability. As previously reported by Joshi et al.,[36] a suitable balance of cholesterol and surfactant
can provide the desired flexibility to the lipid vesicle to improve
the migration toward the deepest region of the skin. Moreover, the
surfactant can improve properties such as encapsulation efficiency,
stability, and permeability.[15,37] In addition, ethanol
has been employed to replace solvents originally used (Supporting Information) to obtain a formulation
as safest as possible. Ethanol is a solvent with low toxic potential
(Pharmacopoeia Italica, XII ed.), whereas the toxicity
of ethers and halogenated hydrocarbons is well known.[38] To optimize the dimensional properties of nanoparticles,
formulations were finally sonicated and extruded (Supporting Information). Probe sonication reduced the particle
size, as previously reported by Zahra Hadian Sahari et al.,[39] who evaluated the effect of sonication on similar
lipid vesicles. Since lipid components here used are heat-sensitive,
the formulations were sonicated in cycles to permit TF to cool and
avoid thermal degradation.[21] The extrusion
process allowed a narrow particle size distribution because it forced
the dispersion to pass several times through a membrane with uniform
pores.[25]The final TF dispersions
appeared turbid and milky, indicating
that the average particle size was above 100 nm; indeed, formulations
having an average particle size of 100 nm or smaller are instead characterized
by a transparent, bluish appearance (Tyndall effect).[40] PCS later confirmed dimensional properties: b-TF and RB-TF
had a particle size of around 200 nm. Such a result agrees with the
study conducted by Godbole et al.,[41] reporting
that a milky appearance characterizes liposomes above 300 nm and those
ranging between 200 and 300 nm. Also, even if the average size of
formulations was around 200 nm and a PDI below 0.2, such values do
not exclude the presence of vesicles larger than 200 nm, affecting
the milky appearance of the dispersion.Lipid vesicles whose
size was between 100 and 600 nm proved to
enhance skin penetration of water-soluble photosensitizer drugs and,
in particular, TF ≤ 300 nm reached deeper into the skin.[13,15]ζ-Potential is a fundamental parameter to predict the
system’s
stability, as it measures the magnitude of the repulsion between charged
particles in the dispersion. The higher ζ-potential value denotes
highly charged particles and minimizes the possibility of aggregation
via electrostatic interaction. Conventionally, a sample exhibiting
a ζ-potential value higher than |30| mV is considered stable.[25] The ζ-potential measurement showed that
TF’s surface charge significantly decreased following RB loading,
reaching −45.9 mV. As previously observed for indocyanine green
zein-phosphatidylcholine nanoparticles, this suggests that the negatively
charged RB was incorporated into the phospholipid bilayers and the
incorporation improved the electrostatic stabilization of the system.[42] Such a result agrees with the storage stability
observed for b-TF and RB-TF. The PDI value of b-TF increased from
the preparation. In contrast, the PDI of RB-TF remained relatively
constant, implying that b-TF progressively aggregates over time and
that the RB presence limits the aggregation phenomena.The stability
of RB-TF was also studied in terms of drug content
over time and photostability. Over time, no reduction in the RB content
was noticed, evidencing the chemical compatibility between the formulation
and the drug components. On the contrary, we observed that photodegradation
of RB aqueous solution was significantly faster than RB-TF dispersion
and that the latter efficiently protected RB over 24 h. As already
observed by Ali et al.,[43] this difference
can be related to the light scattering exerted by lipid, reducing
the photon energy delivered to RB associated with vesicles. Because
the dermal administration is an administration route exposed to visible
light, protecting RB is essential to avoid an undesirable drug loss.Morphological investigation (TEM) revealed MLV b-TF and LUV RB-TF,
as also proved by SAXS analysis. The formation of LUV is a consequence
of the RB presence, which is likely to intercalate in the hydrophobic
palisade of the phospholipid bilayer, thus modifying the effective
lipid packing parameter P = v/a0lc, where v represents the volume of the hydrophobic chain, a0 is the headgroup area, and lc is the critical hydrocarbon chain length (approximately
equal to the fully extended chain length).[44,45] Such alteration of P can be undoubtedly called
into play to explain the different lamellarity degrees observed in
b-TF and RB-TF and may also play a role in the different behaviors
of nanovesicles in terms of deformability. It has been previously
discussed that cholesterol provides rigidity to the liposomal structure;
only a suitable balance of cholesterol and surfactant can provide
the desired flexibility leading to a deformable formulation. Dudhipala
et al.[46] observed that the optimal concentration
of Span 80 to obtain the best deformability index for aceclofenac-transferosomes
is 0.15% w/v and that higher concentrations reduce the deformability.
The authors hypothesized that this is due to the linear structure
of Span 80, which tends to compact the double layer and, therefore,
reduce the TF’s deformability. This evidence and the presence
of cholesterol can explain the nondeformability of b-TF. On the other
hand, Bouvrais et al.[47] proved that the
bending rigidity of lipid membranes strongly depends on the organization
of lipid bilayers, which can be modified by additives or environmental
modification, e.g., by introducing salt and buffers. In agreement
with the deformability indexes observed, it can be assumed that adding
RB to the lipid bilayer induced a softening effect on b-TF, resulting
in unilamellar and deformable RB-TF.The spectrophotometric
and fluorimetric analyses further confirmed
the interaction between RB and lipid components. For RB-TF dispersion
and RB added to b-TF dispersion, the RB absorption λmax shifted to a higher wavelength compared to RB aqueous solution.
Since the dye’s solvatochromic behavior has been reported,
λmax is indicative of the microenvironment interacting
with RB when most of the dye is bound to the dispersed phase.[48] The redshift observed in the absorption spectra
implies that RB sensed the less polar environment of TF and migrated.
Also, the emission spectra of RB-TF dispersion showed an increase
in the fluorescence signal. As previously reported by Chang et al.,[27] the higher intensity ratio suggests that free
RB intercalated through the lipid bilayer mainly as a monomeric form
but not as a dimer form, effectively limiting RB aggregates’
formation. Nevertheless, the logarithm of the partition coefficient
(log P) of the RB disodium salt is reported
to be 0.59, resulting in an amphiphilic molecule.[6] Considering the amphiphilic properties and high water solubility,
the distribution of RB both in the external lipid bilayer and in the
internal aqueous core of the TF is expected.The above characterization
agrees with the in vitro release and
ex vivo permeation profiles obtained experimentally. The in vitro
release assay proved that RB aqueous solution quickly diffuses through
the hydrophilic 50 nm-size polycarbonate membranes, whereas RB-TF
dispersion released RB slower and in a controlled manner. In contrast,
the ability of the RB aqueous solution to permeate the epidermis and
consequently reach the dermis was limited by RB’s physical–chemical
profile. The epidermis is the outermost layer of the skin; it comprises
different living epithelial cell strata (viable epidermis) localized
beneath a multilayer of dead cells called corneocytes (stratum corneum,
SC). As previously stated in the Introduction section, SC is considered
the main barrier against the penetration of external agents,[11] significantly when molecules exceed 500 Da and
present anionic or cationic charges.[12,15] RB is an amphiphilic
drug but it presents two anionic charges and a molecular weight of
1017.64 g mol–1.[6] As
proved by the ex vivo skin permeation study, less than 40% of the
RB aqueous solution permeated through the epidermis and most of it
was retained by the epidermal layer. Formulating RB in TF doubled
the RB amount that permeated the epidermis and effectively reached
the dermal layer. Herein, no studies evaluating the mechanism of RB-TF’s
permeation were performed. However, due to their deformability, the
intact permeation of nanovesicles through the skin is supposed to
be the primary operating action. In support of this hypothesis, the
elastic properties of RB-TF were assessed and previously discussed.
Nevertheless, other mechanisms of action cannot be excluded; these
include the structural modification of the intracellular lipid matrix
due to the penetration enhancing effect of the surfactant and the
vesicles adsorption to and/or fusion with the stratum corneum.[18,19]The cytotoxicity of RB and RB-TF in SK-MEL28 cells was determined
after 48 h of exposure. Although RB is mainly considered for its photodynamic
inactivation of cancer and microbial cells, previous evaluations of
its intrinsic cytotoxicity were reported. It was observed that RB
concentrations ranging between 5 and 10 μM induce cell death
only following RB photosensitization. The intrinsic toxicity of RB
on melanoma and breast cancer cell lines was observed at a concentration
of 100 μM; in particular, it was evident for melanoma in the
case of 200 μM and for breast cancer at 300 μM.[8,49] Such results agree with the values obtained in SK-MEL28 cells. Herein,
we evaluated RB-induced toxicity up to a maximum of 50 μM in
the absence of external stimuli, including light or ultrasounds. At
this concentration, a significant cytostatic effect was observed.
Based on this outcome, we also investigated the efficacy of RB-TF
to reduce the viability of SK-MEL28. The cytostatic effect of RB-TF
was higher than free RB, and the explanation is based on the chemical
profile of RB. RB is an amphiphilic water-soluble compound with a
more hydrophilic tendency due to two negative charges at physiological
pH; these characteristics make it difficult for RB to cross lipophilic
cell membranes spontaneously, resulting in an insufficient cell accumulation
at low concentrations in the absence of a carrier. We hypothesized
that the association of RB with the lipophilic TF increased the RB
cell uptake and consequently the cytostatic effect.[6] On the other hand, b-TF did not induce any effect supporting
the thesis of a safe nanocarrier enhancing RB antimelanoma activity.
In addition, at 50 μM, a promising selectivity of RB-TF on cancer
cells compared to fibroblast was noticed.
Conclusions
We have developed RB-loaded transfersomes to combine the permeation
ability of deformable lipid vesicles with the dye’s intrinsic
antimelanoma activity. The preparation technique employed (REV) avoided
using toxic organic solvents and allowed one to obtain monodispersed
nanoparticles in a dimensional range suitable for dermal delivery;
RB efficiently associated with the lipid carrier. Ex vivo epidermis
permeation confirmed that TF significantly improved the permeation
of RB across the epidermal barrier. Furthermore, in vitro antiproliferative
assays indicated a higher intrinsic cytostatic effect of RB-TF compared
to free RB. Considering these outcomes, RB-TF represent a promising
approach to fight against primary cutaneous melanoma without involving
sono-photodynamic treatments. Future studies will involve the development
of a RB-TF controlled release dosage form and the evaluation of dermatokinetic
vs its pharmacokinetic when administered intravenously.
Authors: Juan J Carreras; Willian E Tapia-Ramirez; Adrian Sala; Antonio J Guillot; Teresa M Garrigues; Ana Melero Journal: Drug Deliv Transl Res Date: 2020-04 Impact factor: 4.617
Authors: Charles M Balch; Jeffrey E Gershenwald; Seng-Jaw Soong; John F Thompson; Michael B Atkins; David R Byrd; Antonio C Buzaid; Alistair J Cochran; Daniel G Coit; Shouluan Ding; Alexander M Eggermont; Keith T Flaherty; Phyllis A Gimotty; John M Kirkwood; Kelly M McMasters; Martin C Mihm; Donald L Morton; Merrick I Ross; Arthur J Sober; Vernon K Sondak Journal: J Clin Oncol Date: 2009-11-16 Impact factor: 44.544
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