Ramesh Marasini1,2,3, Santosh Aryal4. 1. Department of Chemistry, College of Arts and Sciences, Kansas State University, Manhattan, Kansas 66506, United States. 2. Russell H. Morgan Department of Radiology and Radiological Sciences, Division of MR Research, The Johns Hopkins University School of Medicine, Baltimore, Maryland 21205, United States. 3. Cellular Imaging Section and Vascular Biology Program, Institute for Cell Engineering, The Johns Hopkins University School of Medicine, Baltimore, Maryland 21205, United States. 4. Department of Pharmaceutical Sciences and Health Outcomes, The Ben and Maytee Fisch College of Pharmacy, The University of Texas at Tyler, Tyler, Texas 75799, United States.
Abstract
Organic small-molecule photosensitizers are well-characterized and known for the light-responsive treatment modality including photodynamic therapy. Compared with ultraviolet-visible (UV-vis) light used in conventional photodynamic therapy with organic photosensitizers, near-infrared (NIR) light from 700 to 900 nm is less absorbed and scattered by biological tissue such as hemoglobin, lipids, and water, and thus, the use of NIR excitation can greatly increase the penetration depth and emission. Additionally, NIR light has lower energy than UV-vis that can be beneficial due to less activation of fluorophores present in tissues upon NIR irradiation. However, the low water stability, nonspecific distribution, and short circulation half-life of the organic photosensitizers limit its broad biological application. NIR responsive small-molecule fluorescent agents are the focus of extensive research for combined molecular imaging and hyperthermia. Recently a new class of NIR dye, IR-820 with excitation and emission wavelengths of 710 and 820 nm, has been developed and explored as an alternative platform to overcome some of the limitations of the most commonly used gold nanoparticles for photothermal therapy of cancer. Herein, we synthesized a core-shell biocompatible nanocarrier envelope made up of a phospholipid conjugated with poly(ethylene glycol) as a shell, while poly(lactic glycolic acid) (PLGA) was used as a core to encapsulate IR-820 dye. The IR-820-loaded nanoparticles were prepared by nanoprecipitation and characterized for their physicochemical properties and photothermal efficiency. These nanoparticles were monodispersed and highly stable in physiological pH with the hydrodynamic size of 103 ± 8 nm and polydispersity index of 0.163 ± 0.031. The IR-820-loaded nanocarrier showed excellent biocompatibility in the dark, whereas remarkable phototoxicity was observed with breast cancer cells (MCF-7) upon NIR laser excitation. Therefore, the IR-820-loaded phospholipid mimicking biodegradable lipid-polymer composite nanoparticles could have great potential for cancer theranostics.
Organic small-molecule photosensitizers are well-characterized and known for the light-responsive treatment modality including photodynamic therapy. Compared with ultraviolet-visible (UV-vis) light used in conventional photodynamic therapy with organic photosensitizers, near-infrared (NIR) light from 700 to 900 nm is less absorbed and scattered by biological tissue such as hemoglobin, lipids, and water, and thus, the use of NIR excitation can greatly increase the penetration depth and emission. Additionally, NIR light has lower energy than UV-vis that can be beneficial due to less activation of fluorophores present in tissues upon NIR irradiation. However, the low water stability, nonspecific distribution, and short circulation half-life of the organic photosensitizers limit its broad biological application. NIR responsive small-molecule fluorescent agents are the focus of extensive research for combined molecular imaging and hyperthermia. Recently a new class of NIR dye, IR-820 with excitation and emission wavelengths of 710 and 820 nm, has been developed and explored as an alternative platform to overcome some of the limitations of the most commonly used gold nanoparticles for photothermal therapy of cancer. Herein, we synthesized a core-shell biocompatible nanocarrier envelope made up of a phospholipid conjugated with poly(ethylene glycol) as a shell, while poly(lactic glycolic acid) (PLGA) was used as a core to encapsulate IR-820 dye. The IR-820-loaded nanoparticles were prepared by nanoprecipitation and characterized for their physicochemical properties and photothermal efficiency. These nanoparticles were monodispersed and highly stable in physiological pH with the hydrodynamic size of 103 ± 8 nm and polydispersity index of 0.163 ± 0.031. The IR-820-loaded nanocarrier showed excellent biocompatibility in the dark, whereas remarkable phototoxicity was observed with breast cancer cells (MCF-7) upon NIR laser excitation. Therefore, the IR-820-loaded phospholipid mimicking biodegradable lipid-polymer composite nanoparticles could have great potential for cancer theranostics.
With
the progress of nanotechnology, there has been considerable
attention in the treatment of cancer using thermal therapies such
as magnetic hyperthermia, microwave-assisted hyperthermia, photosensitizer-induced
photodynamic therapy, and plasmonic nanoparticle-mediated photothermal
therapy (PTT) due to their high tumor ablation efficiency, good spatial
resolution, and minimal side effects.[1−6] The most common feature in the aforementioned modalities is the
use of heat energy to modulate cancer cells. Near-infrared (NIR) responsive
fluorescent agents are the focus of extensive research for combined
molecular imaging and hyperthermia. A key advantage of the PTT strategy
is the fact that photothermal agents are capable of annihilating cancer
cells with remote light irradiation while causing minimal damage to
normal tissues.[6] On the one hand, in contrast
to inorganic nanoparticles such as super-paramagnetic iron oxide nanoparticles
and gold nanoparticles, NIR-absorbing small-molecule organic dyes
overcome the issue of metal-induced toxicity such as redox-active
and unknown metabolic pathways when incorporated in a suitable envelope
and thus are generally considered to be more biocompatible.[7−12] On the other hand, optical imaging is inexpensive with good resolution,
easy to handle, and can be made portable offering broad application
when compared to other modalities such as magnetic resonance imaging,
computed tomography, or positron-emitting tomography,[13−15] thanks to the advancement in fiber optics technology that makes
optical imaging ideal for incorporation into an endoscope used in
minimally invasive procedures. However, conventional optical imaging
that uses the light of lower wavelengths in the ultraviolet–visible
(UV–vis) region suffers due to high light scattering and absorption
by tissues.[16] Instead, NIR light of wavelengths
from 700 to 900 nm has a deep tissue penetration limit owing to minimal
scattering and tissue absorption.[17] Small
organic molecule fluorescent probes that absorb energy in the NIR
region will release vibrational energy in the form of heat following
exposure to light illumination and can kill cancer cells similar to
that of plasmonic PTT mediated by noble-metal nanoparticles.[13]Indocyanine green is a tricarbocyanine-type
dye with NIR-absorbing
properties approved for visualization of retinal and choroidal vasculature,
blood volume determination, and photodynamic therapy.[11,12,18,19] However, the low water stability and short circulation half-life
limit its broad application for hyperthermia and in vivo imaging.[20] To address these issues, the use of IR-820 dye
as a potential alternative has been described in the literature.[7,21−25] IR-820 dye has similar structural and optical characteristics to
those of indocyanine green with a relatively longer absorption range
through maximal excitation and emission wavelengths of 710 and 820
nm, respectively. Prajapati and colleagues reported the use of IR-820
as a blood pool contrast agent to image tissue injuries and tumors
in mice with improved circulation half-life compared to the indocyanine
green.[25] In an in vivo study by Pandey
and colleagues, they conjugated IR-820 with a photodynamic therapy
drug and studied its potential for dual imaging and thermotherapy.[26] Although these reports indicate that IR-820
has the potential for in vivo applications and provides an attractive
alternative to metallic nanoparticles, there is still more for the
field to provide a detailed in vitro characterization regarding its
photothermal efficiency and cellular behavior in nanoformulations.When an NIR dye, as an organic photothermal agent, is encapsulated
into a suitable delivery vehicle, it can be selectively activated
by the external stimulus such as light after the dye has reached its
intended target, for example, tumor offering an image-guided treatment
platform. The incorporation of the photothermal agent into self-assembled
polymeric nanocarriers confers several benefits to PTT including biodegradability,
scalability, and reproducibility.[26−29] Herein, we designed a lipid polymer-based
core–shell nanocarrier by encapsulating the indocyanine class
of IR-820 dye into the polymeric form for the photothermal treatment
of breast cancer. These lipid–polymer hybrid nanocarriers delivered
IR-820 to MCF-7 breast cancer cells as a potent mediator of PTT exhibiting
significant cytotoxic effects upon excitation with a clinically approved
external laser light stimulus. The results also showed that these
NPs induced cell death primarily through apoptosis, a preferred cell-death
pathway over necrosis that may lead to the recurrence and metastasis
of tumors.[30] With the great success of
photothermal cancer treatment in vitro, this approach exhibits promising
potential for in vivo applications. Furthermore, the photothermal
treatment modality could be improved by combining NIR-responsive agents
with anticancer drugs or photosensitizers for combination therapy
like photothermal–chemotherapy or photothermal–photodynamic
therapy to maximize their therapeutic efficacy with a synergistic
cancer treatment.
Materials and Methods
Chemicals and Reagents
Carboxylic end group terminated
PLGA (lactide/glycolide = 50:50 dL g–1) was purchased
from the DURECT Corporation and used after purification by repeated
precipitation in diethyl ether. 1,2-Distearoylphosphatidylethanolamine
poly(ethylene glycol succinyl) (DSPE-PEG-COOH), 1,2-distearoyl-sn-glycero-3-phosphoglycerol, sodium salt (DSPG), and phospholipid
conjugated l-α-phosphatidylethanolamine-N-(lissamine
rhodamine-B sulfonyl) (ammonium salt) (RhB) was purchased from Avanti
Polar Lipid Inc. (Alabaster) and used as received. 4′,6-Diamidino-2-phenylindole
dihydrochloride (DAPI), (3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyl
tetrazolium bromide) (MTT), acetonitrile, and dimethyl sulfoxide (DMSO)
were purchased from Sigma-Aldrich. IR-820 (CAS No. 172616-80-7) dye
was purchased from BOC Sciences, and Annexin V/propidium iodide (PI)
stain was purchased from BD Bioscience. All other analytical grade
reagents and solvents were used without further purification.Human breast cancer (MCF-7) and Dulbecco’s Modified Eagle’s
Medium (DMEM) were purchased from American Type Cell Culture (ATCC).
Fetal bovine serum (FBS) USDA Premium Select, heat-inactivated, was
purchased from MIDSCI. Cells were maintained in DMEM supplemented
with 10% (v/v), FBS and 1% streptomycin at 37 °C in a 5% CO2 environment. When cells reached 80–90% confluency
in T75 cell culture flasks, they were passaged or plated by detaching
the cells from the flask using Trypsin–ethylenediaminetetraacetic
acid (EDTA) (Thermo Fisher) and then counting the cells with a hemocytometer.
The cell lines were used from passage 10 for bionano interaction studies.
Preparation of IR-820 Encapsulated Nanoparticles
PLGA
with a carboxylic acid-terminated end group of molecular weight 50
kDa was used to synthesize IR-820 encapsulated PLGA nanoparticles
following the well-established nanoprecipitation protocol.[31−38] In a typical experiment, the calculated amount of IR-820 in DMSO
was physically adsorbed with 1 mg of PLGA in acetonitrile and made
the final volume of the mixture to 1 mL to prepare IR-820-encapsulated
PLGA nanoparticles. Then the phospholipids that consist of lipid mixture
formulations having 260 μg of DSPE-PEG and 200 μg of DSPG
were used in 4% ethanol, respectively. This lipid mixture was stirred
at 60 °C for 30 min, and then an IR-820 encapsulated PLGA nanoparticle
solution was added dropwise to the lipid suspension with stirring
followed by the addition of 1 mL of deionized water (acetonitrile/water
= 1:3). The content was further stirred at room temperature for 1
h to facilitate the formation of nanoparticles. The IR-820 encapsulated
PLGA nanoparticles thus formed were purified using a 10 kDa Amicon
wash at 3500 rpm for 10 min. The washing was done three times in 1X
phosphate-buffered saline (PBS), made to a final concentration of
1 mg/mL in 1X PBS, and stored at 4 °C until further use. Similarly,
control nanoparticles were prepared in the same phospholipid ratio
and PLGA content without IR-820.
Characterization of Nanoparticles
The morphology of
the purified NPs was characterized using a transmission electron microscope
(TEM) (FEI Technai G2 Spirit BioTWIN). TEM samples were prepared by
incubating 20 μL of IR-820 PLGA NPs (1 mg/mL) with 20 μL
of 0.1% uranyl acetate for 5 min at room temperature. The sample was
then placed on a Formvar-coated copper grid (400 mesh) and let stand
for an additional 20 min. The excess amount of sample was removed
before image acquisition. TEM images were acquired at 120 kV and analyzed
by the GATAN digital imaging system (GATAN, Inc.). Similarly, NPs
were characterized for hydrodynamic size and zeta potential measurements
using a Malvarian Zeta sizer Nano. In this instrument, the Brownian
motion and the Smoluchowski equation were used to calculate the average
hydrodynamic size and zeta potential value, respectively. The colloidal
stability of NPs was investigated in both ionic and serum conditions
to mimic the biological environment. In brief, 1 mg of NPs dispersed
in the medium was subjected to a hydrodynamic size analysis over the
period to obtain size, polydispersity index (PDI), and zeta potential
values. The reported intensity-based hydrodynamic diameter is the z-average of three measurements, while the total count-based
zeta potential is also the average of three measurements. The formulation
with low PDI, high stability, and uniform narrow size distribution
was selected for the in vitro application. Likewise, the stability
of IR-820 dye in NPs was studied by mixing 500 μL of IR-820
encapsulated NP and 500 μL of 1X PBS (n = 3)
over the period to ensure the dispersity and colloidal stability of
NPs in physiological media. The size and PDI of the particles after
being dispersed in PBS was measured each day for a week using dynamic
light scattering (DLS).The optical properties of IR-820 PLGA
NPs were characterized by ultraviolet–visible spectrophotometry
(BIOMATE-3S, Thermo Scientific) with 1.0 mm path length quartz cuvettes
based on reading the absorbance of the NPs at 710 nm and comparing
to a standard curve of known dye concentration dissolved in DMSO with
dilution as required. The samples were scanned from 400 to 1100 nm
with a baseline correction. The amount of IR-820 released from the
NPs while in storage conditions was also examined by UV–vis
spectroscopy. At several time points between 0 and 7 d post preparation,
samples were centrifuged using a 10 kDa Amicon filter to separate
the NPs from released IR-820, and the collected released IR-820 was
compared to a standard curve of known dye concentration using the
same scanning conditions as described above. The dye release study
was performed three times, and the average and standard deviation
of all three trials are reported.For the IR-820 dye loading
and release study, IR-820 was loaded
on PLGA NPs by the direct mixing of a known concentration of dye into
the PLGA polymer followed by the nanoprecipitation technique.[39−42] To optimize the maximum IR-820 loading, different calculated amounts
such as 150, 300, and 400 μg of IR-820 were initially fed with
1 mg of PLGA dissolved in 400 μL of acetonitrile solution. The
amount of encapsulated IR-820 was quantified, after purification,
spectrophotometrically using a UV–vis spectrophotometer by
measuring the absorbance of the NPs at 710 nm. The drug loading
efficiency was calculated using the following equation.The cumulative
free IR-820 dye release from IR-820 PLGA NPs and
free IR-820 (Mw = 849.47) was studied using 3.5 kDa molecular cutoff
dialysis bags at physiological pH (pH 7.4, PBS). For this purpose,
300 μg of IR-820 input formulation was selected for further
studies due to the stable physiochemical properties. Free IR-820 release
from selected formulations was tracked throughout 72 h by dialysis.
One milliliter of IR-820 PLGA containing 1 mg/mL of NPs or an equivalent
concentration of free IR-820 dye was dialyzed in 200 mL of PBS release
media kept at 37 °C, while constant stirring (80 rpm) was maintained
to retain the sink condition during the experiment. One milliliter
of release media was taken at a regular interval and replaced with
equivalent fresh media. The amount of free IR-820 in the release media
was quantified spectrophotometrically, and the cumulative release
percentage was calculated using the following equation.The photothermal efficiency
of free IR-820 and IR-820 PLGA NPs
was measured in an aqueous suspension upon 808 nm laser (China Deheng
Group, Inc.) irradiation with a thermal camera imaging system (Forward
Looking InfraRed FLIR A5 systems). Samples were suspended in PBS at
an IR-820 concentration of 20–120 μM with a total volume
of 1 mL in the Eppendorf tube. The free dye and IR-820 PLGA NPs were
then irradiated with a continuous-wave constant diode laser power
of 808 nm laser for 2 min at varying power densities from 5.3
to 21.2 W/cm2 while maintaining an ∼1 cm distance
between the laser and sample. The concentration dependence of the
photothermal efficiency for IR-820 PLGA NPs was examined by irradiating
nanoparticles at concentrations of 20, 60, or 120 μM
of IR-820 content with the 808 nm laser set to different power
densities for 2 min. The temperature in each sample was recorded once
every 30 s during irradiation, and the experiments were repeated three
times. To further evaluate the influence of NIR laser exposure on
the optical and physical properties of the NPs, we recorded the absorbance
spectra, hydrodynamic diameter, and polydispersity index of IR-820
PLGA NPs by UV–vis spectroscopy and DLS both before and after
irradiation.
Cellular Biocompatibility and NIR-Mediated
Phototoxicity Study
The in vitro biocompatibility of free
IR-820 dye and IR-820 PLGA
NPs was conducted in MCF-7 cells using a colorimetric assay for assessing
cell metabolic activity by an MTT assay. A time-dependent MTT assay
in dark was conducted as discussed in the literature.[43−46] In brief, cells at a density of 1 × 104 cells per
well in a 96-well plate were incubated overnight. The seeded cells
were washed twice with 1X PBS to remove the debris before NPs treatment.
Then the medium was replaced with various concentrations of NPs (0.01,
0.1, 0.5, 5, 10, 25, 50,100, 200 μg/mL) suspended in DMEM. The
control cell was maintained without treatment. After 24 h of incubation,
cells were washed with 1X PBS to remove surface-absorbed and excess
NPs. After the washing, 100 μL of MTT (5 mg/mL in PBS, filtered
through a 0.22 μm syringe) reagent was added to each well following
the manufacturer’s recommendation. Then the supernatant was
aspirated followed by the addition of 100 μL of DMSO for solubilizing
formazan crystal. The plate was gently shaken in an orbital shaker
for 5 min in the dark, and absorbance was recorded at 560 nm using
a microplate reader (BioTek, Synergy H1 hybrid reader). To analyze
the data, the background (DMSO only) was subtracted from the absorbance
reading in each well. Triplicate well signals were averaged and then
normalized to untreated cells. These experiments were performed in
triplicate and analyzed by Student’s t-tests
at each concentration.The in vitro phototoxicity of IR-820
or IR-820 PLGA NPs was conducted in cells seeded as described above
and treated with IR-820 PLGA NPs at the IR-820 concentration of 60 μM
or with fresh media for 24 h of incubation at 37 °C. The cells
were then washed with PBS and incubated in fresh media for 1 h to
bring the temperature to 37 °C. The appropriate wells were then
irradiated with continuous-wave 808 nm light at 14.1 W/cm2 for 30 s/well such that the treatment groups included no treatment,
laser light only, IR-820 PLGA NPs only, or IR-820 PLGA NPs with laser
light with an ∼1 cm distance between the laser and sample.
The irradiation was performed at room temperature, and the sample
was returned to the 37 °C incubator immediately following irradiation.
After 24 h, the MTT assay was performed as described above.
Data obtained were compared side-by-side with the control experiment
to map the relative toxicity. Data shown are from three experiments
that were each run with triplicate wells, and the data were analyzed
by a one-way analysis of variance (ANOVA) with post hoc Tukey.
Intracellular
Uptake Study
To evaluate the cellular
internalization competence of IR-820 PLGA NPs, experiments were conducted
with MCF-7 cells using confocal microscopy and flow cytometry studies.[47] For the confocal study, cells were seeded on
poly-d-lysine-coated eight-chamber slides at a density of
50 000 cells per well and incubated for 24 h. Then the cells
were treated with 50 μg/mL rhodamine-lipid labeled IR-820 PLGA
NPs suspension prepared in complete DMEM and incubated for 3 h. After
the incubation, the treated cells were washed twice with 1X PBS (pH
= 7.4) and fixed with 4% paraformaldehyde for 30 min at room temperature.
The nucleus of the cells was stained with DAPI for an additional 10
min and imaged under a confocal laser scanning microscope (Carl Zeiss,
CLSM-700). Cells without any treatment served as control cells. The
quantitative percentage of fluorescence intensity was determined using
the Image-J software. The quantification of the intensity of internalized
RhB-lipid labeled NPs was calculated in terms of corrected total cell
fluorescence (CTCF) by use of the following equation.To investigate the quantitative
cellular
uptake of IR-820 PLGA NPs, a fluorescence-activated cell sorting (FACS)
study was conducted after we labeled NPs with rhodamine B-lipid dye
using lipid insertion followed by the nanoprecipitation technique
described above.[31,32,46] In brief, MCF-7 cells with passage 10 were plated at the density
of 1 × 105 cells per well on poly-d-lysine-coated
24-well plates and incubated overnight. Cells were then treated with
0, 20, or 60 μM IR-820 content in IR-820 PLGA NPs prepared
as described above and incubated for 3 h to evaluate dose dependency.
After 3 h, the cells were rinsed with 1X PBS, lifted off the plate
with Trypsin–EDTA, and resuspended in 500 μL of 1X PBS
to yield a single cell suspension of 1 × 106 cells
that were analyzed by BD LSR Fortessa X-20 Special Order Research
Product Flow Cytometer. Control cells were maintained without any
treatments. 10 000 gated events were collected for all measurements.
Density plots showing forward and side scatter data were used to create
a primary gate for cells, excluding debris, prior to analyzing IR-820
PLGA NPs content.
Investigation of the Mechanism of Cell Death
Induced by PTT
To analyze the mechanism of cell death induced
via PTT mediated
by IR-820 PLGA NPs, cells were seeded at 3 × 105 cells per well in a 24-well plate and incubated overnight.
Cells were then treated with 20 μM of IR-820 content in IR-820
PLGA NPs for 3 h, at which time the cells were rinsed with 1X PBS
and the wells were replenished with fresh media. The appropriate wells
were then irradiated with continuous-wave 808 nm light at 14.1
W/cm2 for 30 s per well for the following groups of samples:
no treatment, cells with laser light only, IR-820 PLGA NPs only, or
IR-820 PLGA NPs with laser light. After the laser light
treatment, the samples were returned to the incubator. After 24 h,
an Annexin V/PI staining was conducted as per the manufacturer’s
recommendations. Briefly, cells were lifted from the plate with Trypsin–EDTA,
washed with 1X binding buffer, and resuspended in 100 μL
of binding buffer containing 1:500 Annexin V and 1:1000 PI stains
for 15 min in the dark condition. The samples were then diluted with
300 μL of 1X binding buffer and analyzed on the BD LSR
Fortessa X-20 Special Order Research Product Flow Cytometer with FITC
(excitation, 488 nm; emission, 530/30 nm) and PerCP
(excitation, 488 nm; emission, 675/30 nm) channels.
Density plots showing forward and side scatter data were used to create
a primary gate for cells, excluding debris, before establishing gates
for Annexin V-positive and PI-positive cells. 10 000 gated
events were collected for all measurements. Positively stained gates
were based on unstained cells, and single-stained controls including
Annexin V only, PI only, or free IR-820 dye were used for compensation.
The data presented are the average of three experiments and were analyzed
by one-way ANOVA.
Data and Statistical Analysis
The
obtained data were
plotted and compared to the significance of the results using GraphPad
software. Different statistical models and tests were performed including
a t-test, F-test, and dose–response inhibition
model fit using GraphPad software according to the requirement. All
data represent the mean ± standard deviation. Biocompatibility
and cytotoxicity data include six replicates (n =
6). All other major data include at least three replicates (n = 3).
Results and Discussions
Physiochemical Characterization
The nanoparticles were
fabricated using the nanoprecipitation technique. The morphology of
IR-820 PLGA NPs was characterized by TEM and DLS, which showed that
the nanoparticles were spherical, uniformly distributed, and had the
hydrodynamic diameter of 103 ± 8 nm (Figure A,B). The encapsulation of IR-820 dye has
no significant impact in the diameter of nanoparticles as compared
to the control particles without dye, which has a size of 96 ±
3 nm. These nanoparticles were negatively charged with a zeta potential
value of −28 ± 7 mV (Figure C), as compared to the slightly negative
charge (−1.6 ± 2 mV) of free IR-820 in aqueous condition.
No significant change in the surface zeta potential further assured
us that the IR-820 dye is loaded into the core of the NP. The negative
charge in IR-820 PLGA NPs is due to the presence of the carboxylic
acid-terminated phospholipid PEG moiety. The optical property of the
particles including free IR-820 and IR-820 PLGA NPs by using UV–vis
spectroscopy revealed a characteristic extinction spectrum peak at
710 nm of free dye that is shifted further to the longer wavelength
by 15 nm, red-shift, after loading into the nanoparticles (Figure D,E). To evaluate
the stability and retention of optical properties of IR-820 dye free
in solution or loaded into the NPs, we analyzed the extinction spectrum
of freshly prepared samples and samples that had been stored at 4
°C for three weeks. After storage in MilliQ water, we observed
that free IR-820 dye loses its absorption capabilities, whereas IR-820
PLGA NPs fairly maintain their optical properties (Figure D,E). To further examine the
stability of IR-820-loaded PLGA NPs, we evaluated the colloidal stability
by monitoring the hydrodynamic size and PDI up to 7 d as shown in Figure F. During 7 d of
incubation time, the PDI of NPs varied from 0.116 to 0.163, and the
size varied from 97 to 108 nm. Taken together with optical properties,
these characterization data show minimum variation during the storage
condition signifying better stability and the retention of dye in
the NPs compared to the free dye solution.
Figure 1
Morphology, size, and
photostability of IR-820-PLGA NPs. (A) TEM
image of IR-820-PLGA NPs. (B) Hydrodynamic size with different initial
input of IR-820 concentration (150–400 μg) per milligram
of PLGA NPs. (C) Zeta potential of IR-820 and IR-820 PLGA NPs. (D,
E) Optical properties (absorption profiles) of free IR-820 dye and
IR-820 PLGA NPs in water before and after storage at 4 °C, as
determined by UV–vis spectrophotometry. The concentration of
IR-820 is 60 μM (corresponding to 300 μg input)
for both free and encapsulated dye. (F) Stability of particles over
storage. Data represent n = 3.
Morphology, size, and
photostability of IR-820-PLGA NPs. (A) TEM
image of IR-820-PLGA NPs. (B) Hydrodynamic size with different initial
input of IR-820 concentration (150–400 μg) per milligram
of PLGA NPs. (C) Zeta potential of IR-820 and IR-820 PLGA NPs. (D,
E) Optical properties (absorption profiles) of free IR-820 dye and
IR-820 PLGA NPs in water before and after storage at 4 °C, as
determined by UV–vis spectrophotometry. The concentration of
IR-820 is 60 μM (corresponding to 300 μg input)
for both free and encapsulated dye. (F) Stability of particles over
storage. Data represent n = 3.Next, we studied the dye loading and release kinetics to explore
the potential application of IR-820 in the drug delivery platform
for PTT. IR-820 dye was used as a photoresponsive agent. The IR-820
dye was loaded into PLGA NPs using the lipid insertion mediated nanoprecipitation
technique. As shown in Figure A, the percentage loading efficiency of dye with respect to
the various initial input concentrations of dye was calculated. Our
synthetic protocol yielded a high loading efficiency of 84%–96%
with input IR-820 concentration ranging from 400 μg to 150 μg/mg
polymer, respectively. Unfortunately, in the case of high loading
content with 400 μg, IR-820 is aggregated, as observed from
the increased size and bimodal distribution (Figure B). However, in the case of 300 μg
IR-820 initial input, the size and PDI of NPs after loading (103 nm,
0.135 PDI) was similar to that before loading (96 nm, 0.112 PDI),
as shown in Figure B. Also, the loading efficiency was 93%, and the percentage of dye
content (%wt) to the carrier was 1.37%. So, among the different formulations
studied, it was found that 300 μg/mg polymer showed the best
stability in media while maintaining its loading content. Therefore,
we chose the 300 μg/mg polymer input formulation as a standard
for further experiments. No significant changes in the size and PDI
of this formulation were observed when incubated at 37 °C for
7 d in PBS (pH = 7.4), confirming the excellent physicochemical properties
(Figure F). To determine
the release efficiency of the dye from the NPs, 2 mL samples of 1
mg/mL were placed in a dialysis bag and processed under identical
conditions. We observed burst and sustained dye-release kinetics for
free IR-820 and IR-820 PLGA NPs over a 72 h period at 37 °C (pH
= 7.4), respectively. On the one hand, the results, as shown in Figure C, indicate that
∼36% IR-820 was released within a period of 1 h, while, over
12 h, we observed ∼90% in dye-release kinetics. On the other
hand, we found a higher order of dye stability in the IR-820 PLGA
NPs. Less than 20% of IR-820 was released throughout the release study
period of 72 h. These data are consistent with the literature with
the release of similar lipophilic dyes such as DiR dye or indocyanine
green from the nanoparticles.[22,25,39,40,48] The stability of the dye is highly essential in device NPs for a
theragnostic application.
Figure 2
IR-820 loading and release study. (A) IR-820
loading into PLGA
NPs. (B) Hydrodynamic size with different initial input of IR-820
concentration (150–400 μg) per milligram of PLGA NPs.
(C) Cumulative dye-release kinetics from free IR-820 and IR-820 PLGA
NPs at physiological condition (PBS at pH 7.4). The concentration
of IR-820 is 60 μM (corresponding to 300 μg input)
for both free IR-820 and IR-820 PLGA NPs. Data represent n = 3.
IR-820 loading and release study. (A) IR-820
loading into PLGA
NPs. (B) Hydrodynamic size with different initial input of IR-820
concentration (150–400 μg) per milligram of PLGA NPs.
(C) Cumulative dye-release kinetics from free IR-820 and IR-820 PLGA
NPs at physiological condition (PBS at pH 7.4). The concentration
of IR-820 is 60 μM (corresponding to 300 μg input)
for both free IR-820 and IR-820 PLGA NPs. Data represent n = 3.
IR-820-Mediated Photothermal
Efficiency
The concentration
dependence and laser power dependence photothermal efficiencies of
free IR-820 and IR-820 PLGA NPs were investigated under 808 nm NIR
laser irradiation using three different concentrations of IR-820 from
20 to 120 μM and power densities of 5.3, 14.1, and 21.2 W/cm2. All samples suspended in an aqueous solution were irradiated
where the change in temperature versus time was noted using a thermal
imaging system at an interval of 30 s. As shown in Figure , a time-dependent increase
in temperature was observed in all samples. As expected, we observed
low heat evolution at a lower concentration of dye or laser power
used for both samples. However, we did not observe any bigger difference
in the temperature rise between free IR-820 dye or IR-820 PLGA NPs
at an identical dye content. As a general trend, we found that IR-820
PLGA NPs produced more temperature compared to the free IR-820 under
identical conditions of dye concentration and laser power used (Figure A,B). At 5.3 W/cm2, free IR-820 increased the temperature (ΔT) from 3.7 to 19 °C, while IR-820 PLGA NPs increased from 6
to 20.4 °C under similar dye content ranging from 20 to 120 μM.
The temperature was increased from 6.5 to 33.3 °C and from 8
to 33.6 °C while from 9.4 to 34.2 °C and from 10.2 to 35
°C for free IR-820 and IR-820 PLGA NPs at 14.1 and 21.2 W/cm2, respectively. Interestingly, we did not find a significant
difference in heat evolution at 14.1 versus 22.2 W/cm2 irrespective
of the sample. To investigate the effect of laser exposure to the
optical and physicochemical properties of IR-820 PLGANPs or free IR-820,
we recorded the UV–vis spectra and size of the particles. We
observed a significant reduction in the absorption peak of free IR-820
but a lesser effect of laser in the case of IR-820 PLGA NPs after
a laser exposure of 2 min (Figure A,B). As shown in Figure C, we did not have much effect on laser irradiation
in terms of size and PDI of the IR-820 PLGA NPs. However, during the
NIR exposure, a change in the color of the free IR-820 suspension
was observed, which was confirmed by recording the change in optical
density and absorption peak, as can be seen in Figure A. This is presumably because the aqueous
stability of IR-820 is greatly affected by the local temperature,
and a high local temperature makes free dye unstable in the suspension.
In contrast to free IR-820, the retention of optical density and higher
order of colloidal stability was observed in the case of IR-820 PLGA
NPs. These results demonstrate that IR-820 PLGA NPs could act as an
excellent photothermal source for therapeutic study.
Figure 3
Comparative photothermal
efficiency of free IR-820 dye and IR-820
PLGA NPs. (A) The concentration and power-dependent NIR laser (λ
= 808 nm) heating thermograph profile of IR-820 PLGA NPs and free
IR-820 dye suspension upon laser irradiation. Three different laser
power densities 5.3, 14.1, and 21.2 W/cm2 and 20, 60, and
120 μM IR-820 dye corresponding to 150, 300, and 400 μg
input/mg polymer were irradiated for 2 min with the laser-to-sample
distance of ∼1 cm. The evolution of temperature throughout
the suspension was recorded using an FLIR thermal camera system. (B)
The corresponding temperature plots showing the average change in
temperature as a function of time from (A). Data represent n = 3.
Figure 4
Optical response and
alteration in the size of IR-820 PLGA NPs
after laser exposure. (A, B) UV–Vis absorption profile showing
the changes in optical density of free IR-820 dye and IR-820 PLGA
NPs before and after laser irradiation. (C) Changes in the hydrodynamic
size of PLGA NPs and IR-820 PLGA NPs after laser exposure measured
by DLS. These data were recorded for the laser power density of 14.1
W/cm2 and 60 μM IR-820 dye content either in free
dye or in NPs that were irradiated for 2 min.
Comparative photothermal
efficiency of free IR-820 dye and IR-820
PLGA NPs. (A) The concentration and power-dependent NIR laser (λ
= 808 nm) heating thermograph profile of IR-820 PLGA NPs and free
IR-820 dye suspension upon laser irradiation. Three different laser
power densities 5.3, 14.1, and 21.2 W/cm2 and 20, 60, and
120 μM IR-820 dye corresponding to 150, 300, and 400 μg
input/mg polymer were irradiated for 2 min with the laser-to-sample
distance of ∼1 cm. The evolution of temperature throughout
the suspension was recorded using an FLIR thermal camera system. (B)
The corresponding temperature plots showing the average change in
temperature as a function of time from (A). Data represent n = 3.Optical response and
alteration in the size of IR-820 PLGA NPs
after laser exposure. (A, B) UV–Vis absorption profile showing
the changes in optical density of free IR-820 dye and IR-820 PLGA
NPs before and after laser irradiation. (C) Changes in the hydrodynamic
size of PLGA NPs and IR-820 PLGA NPs after laser exposure measured
by DLS. These data were recorded for the laser power density of 14.1
W/cm2 and 60 μM IR-820 dye content either in free
dye or in NPs that were irradiated for 2 min.
Biocompatibility and Cellular Internalization Study
The
biocompatibility of free IR-820 and IR-820 PLGA NPs was assessed
in human breast cancer cell MCF-7 as presented in Figure A,B for 48 h of treatment.
The IR-820 dye concentration as a handle was used to assess the biocompatibility.
IR-820 PLGA NPs showed at least 80% cell viability (Figure A) at a high concentration
(200 μg/mL), while the viability of free IR-820 was found to
be 42% at an equivalent concentration (65 μM of IR-820), (Figure B). The dye concentration
was used according to the dye content in nanoparticles used in Figure A. These data signify
the biocompatibility of IR-820 PLGA NPs even at high concentrations.
We further extended our approach to see if IR-820-loaded NPs were
taken up by cells. We labeled IR-820 PLGA NPs with Rh–B-lipid,
treated with cells for 3 h, and found that these nanoparticles were
taken up by cells (Figure C). To further evaluate the dose dependency and quantitative
cellular uptake of the same Rh–B-lipid-labeled nanoparticles
upon treatment and incubation for 3 h with an IR-820 concentration
of 20 or 60 μM, an FACS study was performed. As shown in Figure D, nanoparticles
were taken up by the cells, and as expected, we observed that a significantly
larger amount of IR-820 PLGA NPs was taken up by cells when treated
with 60 μM IR-820 content. It is worth mentioning that this
concentration of nanoparticles is well-tolerated with more than 70%
of cells being viable even at the large concentration input of 200
μg/mL (Figure A). Taken together, these observations reflect excellent biocompatibility
and uptake of IR-820 PLGA NPs signifying that it can be used as a
safe photothermal delivery agent.
Figure 5
Cellular interaction study in MCF-7 cells.
(A) Concentration-dependent
relative cell viability of MCF-7cells exposed to PLGA NPs or IR-820
PLGA NPs without light exposure. (B) Concentration-dependent cell
relative viability of MCF-7 cells exposed to free IR-820 dye. The
concentration of IR-820 was used similar to the IR-820 content encapsulated
in PLGA NPs as shown in (A). (C) Confocal microscopic micrographs
capture Rh–B-lipid labeled IR-820 PLGA NPs cellular internalization
at 3 h of incubation, and (D) corresponding FACS analysis (Data represent n = 6 for biocompatibility and n = 3 for
FACS study).
Cellular interaction study in MCF-7 cells.
(A) Concentration-dependent
relative cell viability of MCF-7cells exposed to PLGA NPs or IR-820
PLGA NPs without light exposure. (B) Concentration-dependent cell
relative viability of MCF-7 cells exposed to free IR-820 dye. The
concentration of IR-820 was used similar to the IR-820 content encapsulated
in PLGA NPs as shown in (A). (C) Confocal microscopic micrographs
capture Rh–B-lipid labeled IR-820 PLGA NPs cellular internalization
at 3 h of incubation, and (D) corresponding FACS analysis (Data represent n = 6 for biocompatibility and n = 3 for
FACS study).
NIR-Mediated Phototoxicity
Study
We next investigated
the use of IR-820 PLGA NP-mediated PTT as a treatment strategy for
breast cancer and probed the mechanism of cell death induced by this
treatment modality. MCF-7 cells were treated with 60 μM
dye in IR-820 PLGA NPs, the maximum tolerated dose determined previously
(Figure A) for 3 h,
and then samples were irradiated with an 808 nm laser and compared
with free IR-820 having the identical dye concentration. Cells without
any treatment were used as a control throughout the treatment experiments
(Figure A). The combination
of IR-820 PLGA NPs and laser exposure for 30 s resulted in significant
phototoxicity having 70% and 42% cell viability after 24 h
post-treatment as measured by an MTT assay for 5.3 and 14.1 W/cm2 laser power density, respectively, while 77% and 56% cell
viability were observed for free IR-820 under similar conditions before
and after laser illumination. We note that the laser alone or laser
+ PLGA NPs (without dye) has no noticeable effect on the viability
of cells. These data when taken together with aqueous photothermal
efficiency data from Figure showed that 14.1 W/cm2 is optimal for the IR-820-assisted
photothermal therapy of cancer in vitro. Additionally, we evaluated
the concentration-dependent phototoxicity at 14.1 W/cm2 while varying the IR-820 concentration in samples, both free IR-820
and IR-820 PLGA NPs, from 1.5 to 65 μM as shown in Figure B. With the increase
in IR-820 content, the increase in IR-820-assisted phototoxicity was
observed after laser exposure as measured by MTT. At lower concentrations
of dye, we do not see much difference in the phototoxicity pattern.
However, the IR-820 PLGA NPs produced significant phototoxicity at
the concentrations of 16–65 μM when compared with its
free dye counterpart (Figure B).
Figure 6
NIR-mediated phototoxicity study and its mechanism of cell death
in MCF-7 cells. (A) A comparative power-dependent PTT using either
cells, PLGA NPs, free IR-820, or IR-820 PLGA NPs (60 μM) with
laser exposure for 30 s. These data were recorded for the laser power
density of 5.3 vs 14.1 W/cm2, respectively, to map the
best power density for further investigation. (B) A comparative dose-dependent
relative phototoxicity of MCF-7 cells after photothermal therapy generated
by free IR-820 vs IR-820 PLGA NPs having identical dye content after
808 nm laser exposure for 30 s at 14.1 W/cm2. (C) A representative
scatter plot demonstrating the fraction of cells in early apoptosis
(bottom right quadrant), late apoptosis (top right quadrant), or necrosis
(top left quadrant) following treatment with media only, cells + laser,
IR-820-PLGA NPs only, or IR-820-PLGA NPs + laser.
NIR-mediated phototoxicity study and its mechanism of cell death
in MCF-7 cells. (A) A comparative power-dependent PTT using either
cells, PLGA NPs, free IR-820, or IR-820 PLGA NPs (60 μM) with
laser exposure for 30 s. These data were recorded for the laser power
density of 5.3 vs 14.1 W/cm2, respectively, to map the
best power density for further investigation. (B) A comparative dose-dependent
relative phototoxicity of MCF-7 cells after photothermal therapy generated
by free IR-820 vs IR-820 PLGA NPs having identical dye content after
808 nm laser exposure for 30 s at 14.1 W/cm2. (C) A representative
scatter plot demonstrating the fraction of cells in early apoptosis
(bottom right quadrant), late apoptosis (top right quadrant), or necrosis
(top left quadrant) following treatment with media only, cells + laser,
IR-820-PLGA NPs only, or IR-820-PLGA NPs + laser.
Evaluation of the Mechanism for IR-820 PLGA
NPs Induced Phototoxicity
After the successful PTT in vitro
using IR-820 PLGA NPs, we next
evaluated the mechanism of cell death by identifying the percentage
of cells undergoing apoptosis versus necrosis using FACS study. Apoptosis
is a preferred programmed cell death pathway in a normal physiologic
process characterized by certain morphological features, including
loss of plasma membrane asymmetry and attachment, condensation of
cytoplasm and nucleus, and internucleosomal cleavage of DNA.[30] In apoptotic cells, the membrane phospholipid
phosphatidylserine (PS) is translocated from the inner to the outer
leaflet of the plasma membrane, thereby exposing PS to the external
cellular environment, which upon treatment with Annexin V conjugated
to fluorochromes including FIT-C, 35–36 kDa Ca2+-dependent phospholipid-binding protein that has a high affinity
for PS, binds to cells with exposed PS.[49] This format retains its high affinity for PS and thus serves as
a sensitive probe for a flow cytometric analysis of cells that are
undergoing apoptosis. FIT-C Annexin V staining leads to the loss of
membrane integrity, which accompanies the latest stages of cell death
resulting from either apoptotic or necrotic processes. Therefore,
we stained with FIT-C Annexin V in conjunction with PI to identify
early apoptotic cells (PI negative, FIT-C Annexin V positive). Thus,
we assessed the mechanism of cell death by first treating cells with
no treatment versus 20 μM of IR-820 in IR-820 PLGA NPs for 3
h and then irradiating the samples with 808 nm light for 30
s at 14.1 W/cm2. After 24 h of incubation, cells
were stained with Annexin V (FIT-C channel) and PI (PE channel) for
analysis by flow cytometry. Viable cells with intact membranes exclude
PI, whereas the membranes of dead and damaged cells are permeable
to PI. As shown in representative scatter plots in Figure C, cells that stain positive
for Annexin V only (bottom right quadrant Q4) are undergoing early
apoptosis, while cells that stain positive for Annexin V and PI (top
right quadrant Q2) are undergoing late apoptosis and cells that stain
positive for PI only (top left quadrant Q1) are undergoing necrosis.
The flow cytometric analysis showed that IR-820 PLGA NPs induced cell
death via PTT primarily through apoptosis (52%) with no notable increase
in necrotic cell percentage (0.2%) (Figure C). In contrast to the PTT using gold nanoparticles
as seen in our previous study, the rapid and high rise in the temperature
in cell suspension results in cellular necrosis where there is a reported
pro-inflammatory response that can elicit a negative immune reaction
that may actually promote tumor recurrence.[30,50−52] Therefore, it is essential to produce normal physiological
cell death to achieve long-term survival benefits. These data when
taken together with the MTT data indicate that IR-820 PLGA NPs can
successfully mediate the proapoptotic PTT of breast cancer cells in
vitro, warranting further investigation of its use in vivo. Furthermore,
because of the limitation of the Annexin V and PI assay, which does
not distinguish between cells that have undergone apoptotic death
versus those that have died as a result of a necrotic pathway because,
in either case, the dead cells will be stained with both Annexin V
and PI, we therefore recommend that the apoptosis be measured over
time so that cells can be tracked from Annexin V and PI negative (viable,
or no measurable apoptosis) to Annexin V positive and PI negative
(early apoptosis, membrane integrity is present) and, finally, to
Annexin V and PI positive (late apoptosis and death).
Conclusion
In summary, we showed that IR-820 dye encapsulated into lipid polymer
composite nanoparticles that are monodispersed and highly stable has
optical characteristics that are maintained. The IR-820 PLGA NPs were
taken up by cells and exhibited excellent biocompatibility as compared
to the free IR-820 dye. However, the combination of NIR laser with
IR-820 PLGA NPs has induced significant cell death when compared to
its counterpart free IR-820 dye at an equivalent dye concentration.
Furthermore, we confirmed the mechanism of NIR-mediated cell death
is mainly via apoptosis. Considering the fact that the polymer and
lipids used herein are biodegradable and Food and Drug Administration
(FDA)-approved biomaterials, these nanoparticles overcome the limitations
of toxicity associated with metallic especially gold and iron nanoparticle-mediated
thermal treatments. This study warranted further validation in in
vivo PTT, and the mechanism of cell death is also essentially via
apoptosis in vivo. Additionally, one could expect to compare and contrast
the photothermal efficiency and mechanism of cell death of this system
with gold nanoparticles for the quantitative analysis of each system.
Overall, IR-820 PLGA NPs showed promise in the PTT, and these results
lay the foundation for further investigation.
Authors: Marta Pérez-Hernández; Pablo Del Pino; Scott G Mitchell; María Moros; Grazyna Stepien; Beatriz Pelaz; Wolfgang J Parak; Eva M Gálvez; Julián Pardo; Jesús M de la Fuente Journal: ACS Nano Date: 2014-12-17 Impact factor: 15.881
Authors: Victoria S R Harrison; Christiane E Carney; Keith W MacRenaris; Emily A Waters; Thomas J Meade Journal: J Am Chem Soc Date: 2015-07-14 Impact factor: 15.419