María
Sancho-Albero‡
a,
Giada
Rosso‡
b,
Luisa
De Cola
*ac and
Valentina
Cauda
*b
aDepartment of Biochemistry and Molecular Pharmacology, Istituto di Ricerche Farmacologiche Mario Negri IRCCS, Via Mario Negri, 2, 20156, Milan, Italy. E-mail: luisa.decola@marionegri.it
bDepartment of Applied Science and Technology, Politecnico di Torino, Corso Duca degli Abruzzi 24, 10129 Turin, Italy. E-mail: valentina.cauda@polito.it
cDepartment of Pharmaceutical Science, DISFARM, Università degli Studi di Milano, 20133, Milan, Italy
First published on 24th August 2023
The recent nanomedicine advancements have introduced a variety of smart nanoparticles in cancer treatment and diagnostics. However, their application to the clinic is still hindered by several challenges related to their biocompatibility, elimination and biodistribution. Here we propose breakable organosilica mesoporous nanoparticles, i.e. nanocages, able to efficiently incorporate cargo molecules and be coated, with different lipid compositions, to enhance their biomimetic behaviour. We exploit the electrostatic interactions between the organosilica surface and the opposite charge of the lipid mixtures in order to obtain an efficient organosilica coverage. The lipid-coated nanocages are proved to have an incredibly high hemocompatibility, significantly increased with respect to pristine nanocages, and excellent colloidal stability and biocompatibility. The cargo-loaded and lipid-coated nanocages are tested and compared in vitro on two different cancer cell lines, demonstrating the key role played by the lipid coating in mediating the internalization of the nanocages, evaluated by the enhanced and rapid cellular uptake. The efficient intracellular delivery of the therapeutic agents is then assured by the destruction of the organosilica, due to the disulfide bridges, introduced into the silica framework, that in reducing media, like the intracellular one, are reduced to thiols causing the breaking of the nanoparticles. The possibility to image and effectively kill cancer cells demonstrates the potentiality of the lipid-coated nanocages as a powerful tool in anticancer research and as a promising smart theranostic platform.
The silica surface, rich in hydroxyl groups, offers not only a highly-hydrophilic nature, but also efficacious chemical anchoring sites for functional molecules,17 such as targeting ligands,18 polymers19 and lipid bilayers20 able to improve the biodistribution and colloidal stability of the porous silica nanoparticles. In fact, the colloidal stability of a generic nanoparticle in biological media has to be strictly preserved to avoid the aggregation and degradation phenomenon,21 as it can negatively affect the biodistribution, the endocytosis process and the delivery of the entrapped active molecules to the target tissue. A strategy was indeed proposed, consisting of phospholipidic bilayers encapsulating solid-state nanoparticles, and among others also mesoporous silica.22 This approach offers several advantages: besides guaranteeing the colloidal stability of nanoparticles in biological media, it increases their biocompatibility and biomimicking features and improves the interaction with the cell membrane, facilitating the endocytosis process.23 The lipidic bilayer also offers a valid barrier to the rapid drug leakage out of the nanoparticle pores,20,24 avoiding off-target release, while assuring the drug delivery only intracellularly. Indeed, literature reports have shown the proficient use of lipid bilayer-coated nanoparticles for effective biostabilization in biological media25 and for efficient cell internalization. Moreover, in combination with mesoporous silica nanoparticles, lipidic bilayers allowed the retention of anticancer drugs, such as doxorubicin, paclitaxel, curcumin, irinotecan,26–28 enzyme inhibitors,24 and nucleic acids, such as mRNA or dsDNA.29,30
However, efficient endocytosis needs to be coupled with an effective endosomal escape to intracellularly release the therapeutic content. For this reason, some solutions were developed to overcome the endosomal membrane “barrier” and allow the therapeutic content to efficiently reach the cell sub-compartment. Towards this goal, mesoporous silica, coated by an artificial lipid bilayer, can be equipped with stimuli responsive surface modifiers, e.g. to induce an osmotic pressure inside the endosome,31 or photoactive molecules32–34 to escape from the endosomal compartments. Another successful strategy relies on the nanoparticle degradation itself, triggered by acidic pH or redox reactions.23,35
In this work, we report breakable organosilica nanocages, ssOSCs, containing disulfide groups in the silica structure, coated by lipidic bilayers. The nanocages are able to encapsulate an anticancer drug, doxorubicin, and are effectively internalized into cancer cells, functioning as an anticancer therapy. We demonstrate that these nanostructures can be covered with different lipid mixtures using electrostatic interactions, and the resulting hybrids maintain high colloidal stability and, most importantly, improve the cellular uptake and hemocompatibility. Remarkably, we observed that lipid bilayers can modify the cell interaction of the disulfide-bridged organosilica nanocages: once they are coated by a negatively charged lipid mixture, a prompt internalization is observed, guaranteeing a successful cargo release into cancer cells. Therefore, the combination of two sophisticated strategies, i.e. the breakable organosilica carrying an anticancer cargo and a biomimicking lipid bilayer, produces a smart hybrid nanoparticle with improved properties and is ready to be further tested in a preclinical context.
In order to create an electrostatic interaction between the ssOSCs and the phospholipids, the nanocages were functionalized with amino groups (ssOSCs–NH2) that are protonated under physiological conditions, leading to positive charges. TEM images depicted in Fig. 1A indicate that the functionalized ssOSCs preserved their morphology and size even after functionalization with amino silane (see the Experimental section for further details). DLS (Fig. 1B) revealed a hydrodynamic diameter of around 30 nm and a positive ζ potential (+23.6 ± 0.7 mV) was also obtained, corroborating the correct surface functionalization of the ssOSCs with the amino groups. Similarly, by FTIR analysis (Fig. 1C) it was possible to confirm, besides the other bands, the characteristic fingerprint of amino silane employed for the NPs functionalization, and the bands at 3378 and 1416 cm−1 were attributed to the NH2 groups. When comparing TGA of the naked and the NH2 functionalized ssOSCs (Fig. 1D), an estimate of a functionalization corresponding to 5 to 10% in weight of the amino groups was achieved.
Finally, the colorimetric Kaiser test allowed us to determine the presence of the positively-charged amine groups and roughly estimate the amount of the amine groups on the silica surface. Fig. 1E shows that the ssOSC solution remained colorless (when no free primary amines were present); in contrast, the ssOSCs–NH2 solution turned dark blue, indicating the presence of primary amines. The absorption spectra of both solutions recorded from 450 nm to 750 nm are shown in Fig. 1E. Considering the absorbance obtained at 570 nm and taking into account the density of SiO2 (2.65 g mL−1), the diameter of NPs obtained by TEM and the sample concentration, we roughly estimated the presence of 105 NH2 molecules per particle (Table S1 in the ESI†).
In order to evaluate the effect of the nanoparticle's surface functionalization and its interaction with differently charged lipids, various combinations of nanoparticles and lipid formulations were tested and characterized (Fig. 2). In particular, ssOSCs and ssOSCs–NH2 were combined with two lipid mixtures: one possessing a neutral charge and one with a negative net charge, as already reported by some of us.22 We indeed expected that the correct matching between the superficial charge of the nanoparticles and the charge manifested by the lipid mixture could promote efficient encapsulation of the nanoparticles, through favourable electrostatic interactions. All combinations of lipids and nanoparticles were thus tested by DLS, ζ potential measurements, and fluorescence microscopy to verify our hypothesis. Additionally, nanoparticles without lipid coverage and liposomes without nanoparticles were tested as controls. Interestingly, the DLS measurements in Fig. 2A evidenced a shift in the hydrodynamic diameter from the naked and unfunctionalized nanocages (26 nm) to the coated ones with a neutral lipid mixture (50 nm); the peak of these lipid-coated ssOSCs is also distant from that of neutral liposomes as the control, which have a size distribution peaking at 28 nm, approximately in the same range of pristine uncovered ssOSCs, but with a broader size distribution. Similar observations can be made for ssOSCs–NH2 combined with neutral lipids, as shown in Fig. 2B. The measurements evidenced a clear shift in the size distribution from uncoated (28 nm) to coated ssOSCs–NH2 (78 nm). In contrast, the negative lipid formulation combined with pristine ssOSCs (Fig. 2C) did not produce a narrow size distribution, but a range of sizes with two larger populations (peaks at 33 and 114 nm). This result indicates the presence of particles which could be a mixture of covered and uncovered ssOSCs and even free liposomes and suggests an unsuccessful nanocage encapsulation in the lipidic shell, probably due to electrostatic repulsions.
Fig. 2 Characterization of lipid coated nanoparticles. (A) DLS results of non-functionalized ssOSCs, uncovered and covered with neutral lipids, and control liposomes; (B) DLS results of non-functionalized ssOSCs, uncovered and covered with negative lipids, and control liposomes; (C) DLS results of NH2-functionalized ssOSCs uncovered and covered with neutral lipids and control liposomes; (D) DLS results of NH2-functionalized ssOSCs uncovered and covered with negative lipids and control liposomes; for negative lipids, two ssOSCs:lipids mass ratios were tested: 2:1 and 1:1; (E) ζ potential results of non-functionalized ssOSCs, covered with neutral and negative lipids; and (F) ζ potential results of non-functionalized ssOSCs, covered with neutral and negative lipids; for negative lipids, two ssOSCs:lipids mass ratios were tested: 2:1 and 1:1. A table of the above plotted data is available in the ESI (Table S2†). |
The coating of ssOSCs–NH2 with negative lipids was explored for two different lipid amounts (mass ratios 2:1 and 1:1 of ssOSCs:lipids, see Fig. 2D); both lipid coatings produced a uniform and significant shift in size distribution, with respect to the pristine nanocages. The size distribution peaks were at 124 nm and 108 nm for 2:1 and 1:1 mass ratio, respectively, and were very different from the two peaks obtained by the negative control liposomes (56 and 246 nm), also characterized by the highest polydispersity index (PdI = 1, see Table S2 in the ESI†). Interestingly the different ratios do not lead to markedly different sizes suggesting, already at a low ratio, good coverage of the nanocages by the lipids. Fig. 2E and F show the ζ potential results. The value obtained for the pristine ssOSCs (Fig. 2E) was −11 ± 0.5 mV; for the control neutral liposomes, it is −7.3 ± 2.4 mV and for the negative control liposome, it is −48.2 ± 1.8 mV. Both zeta potentials of neutral and negative lipid-coated ssOSCs were slightly negative: −6.2 ± 0.12 mV and −13.7 ± 0.3 mV, respectively, with neither reaching the desired colloidal stability. On the other hand, ssOSCs–NH2 showed a positive ζ potential due to the presence of protonated amine groups on the surface and, when covered with the neutral lipid mixture, they evidenced a ζ potential of +30.7 ± 1.5 mV. The ssOSCs–NH2 coated with the negative lipid mixture showed a ζ potential of −48.6 ± 0.3 mV and −50.7 ± 4.8 mV for 2:1 and 1:1 nanocages to lipid mass ratios respectively. These data are also summarized in Table S1.† Interestingly, the addition of negatively charged lipids on the ssOSCs–NH2 sample produced a drastic shift in the ζ potential value, which was very similar to the free negative liposomes, indicating a well-formed lipid bilayer on the functionalized silica cores due to the favourable electrostatic interaction. In both cases, the absolute value of the zeta potential for the lipid coated ssOSCs–NH2 was higher than +30 mV, indicating the colloidal stability of the obtained nanoconstructs. Taken together, the ζ potential and DLS results suggest that functionalization of the nanocages is fundamental to achieve an effective, stable, homogeneous lipid bilayer coverage of the negative lipid mixture because of an optimal electrostatic interaction, with the positively charged ssOSCs–NH2. Fig. S2† presents the nanoparticle tracking analysis results of the ssOSC–NH2-negative lipid sample with a 2:1 nanoparticle to lipid ratio, which shows a mode size of 125 nm, confirming DLS data and corroborating the achievement of a quite narrow and an almost Gaussian-shaped distribution.
To further evaluate the efficacy of the self-assembly of lipids around the nanocages, a fluorescence colocalization analysis was performed. ssOSCs were covalently labelled with a red cyanine (Cy5) fluorescent dye through the coupling of the sulfo–Cy5–NHS derivative with the amino groups grafted on the nanocages. Independently, the lipids were labelled with DiO, a lipophilic dye, exhibiting green emission. Although the resolution limit dictated by Abbey's law does not permit appreciation of the core–shell structure, the observation of the spots collected from the two channels suggests the co-localization of lipids and nanocages. In Fig. 3 it is clearly visible that the ssOSC–NH2-negative lipid sample with a 2:1 nanocage to lipid ratio presented the best colocalization of the lipidic shells with the organosilica cores, since almost the totality of the spots appears white. This means that the visible objects in the far-red channel and in the green one were completely superimposed. The number of white spots was remarkably lower for the other samples, where single green or magenta spots were identified, indicating the presence of free nanoparticles or liposomes without the organosilica core. Considering the multitude of images collected in the two fluorescence channels, an estimation of the encapsulation efficacy was performed. Remarkably, the calculated colocalization percentages (reported in Tables S3 and S4, ESI†) reflected the scenario prospected by DLS and ζ potential measurements. The best results were again obtained for the NH2-functionalized nanocages covered by negative lipids, achieving a colocalization percentage above 80%. In contrast, both ssOSCs and ssOSC–NH2 covered with neutral lipids showed a moderate colocalization percentage of 65.7% and 50.1% on average, respectively. Finally, the lowest colocalization percentage (5.3%) was registered for the ssOSC-negative lipid sample, which showed the poorest size distribution among all lipid-coated samples, together with a low ζ potential, despite the charge of the lipids. Regarding the coupling between negative lipid formulation and functionalized nanocages, which was expected to be the best match, two different ssOSCs–NH2 to lipid (w/w) ratios were tested and compared: 1:1 and 2:1. While DLS (Fig. 2D) and the ζ potential measurements (Fig. 2F) showed rather similar results, the colocalization percentage was higher (92%) for the 2:1 ratio, compared to the 1:1 ratio (82%). For this reason, the nanocages to lipid ratio equal to 2:1 w/w was chosen for the subsequent experiments. Fig. 3 shows a representative set of fluorescence microscopy images (merged channels) of the lipid coated nanoparticles, whereas single-channel images are reported in Fig. S3 and S4 of the ESI.†
FTIR analysis of the negative lipid-coated and the naked ssOSCs–NH2 (Fig. S5†) confirmed once again the correct wrapping of the phospholipid coating around the silica core: together with the silica characteristic bands (previously described), the typical phospholipid fingerprinted peaks37,38 were observed. In particular, CO (1765–1720 cm−1), PO2 (1200–1145 cm−1 and 830–740 cm−1), P–O–C (1145–970 cm−1), P–O–C + PO2 (1200–970 cm−1) and CH2 (2926–2855 cm−1) vibrational bands were clearly observed. TGA confirmed the last results and demonstrated the effective coating of the nanocages with the lipids (almost 50% of the sample weight corresponds to the lipidic fraction).
Remarkably, both ssOSCs–NH2 and ssOSCs–NH2-negative lipids showed coagulation times that were not significantly different from the control sample: the ssOSC–NH2 had an average coagulation time slightly inferior to the control and the ssOSCs–NH2-negative lipids even slightly superior. These results corroborate the data obtained with the previous characterization methods; in fact, the fast coagulation time of ssOSC-negative lipids can be interpreted as proof of an unsuccessful encapsulation of the nanocages, supporting the hypothesis that the functionalization with aminopropyl groups is fundamental. Remarkably, ssOSC–NH2-negative lipids are characterized by the highest coagulation time, confirming that lipids confer to the nanoparticles a superior hemocompatibility. Moreover, the higher coagulation time reported for lipid-coated ssOSCs–NH2 with respect to the uncoated ones is indirect proof of the optimal encapsulation achieved with these functionalized nanocages and the negatively charged lipid formulation.
Fig. 7 Characterization of ssOSCs@DOX. (A) TEM images, (B) DLS analysis, (C) FTIR and (D) absorption spectrum. |
The DLS results and ζ potential (−8.3 ± 1.3 mV) of the ssOSCs@DOX (Fig. 7B) corroborated the TEM findings, confirming that doxorubicin was encapsulated inside the NP pores rather than being attached to the surface. In the FTIR spectra of Fig. 7C, the characteristic peaks of the organosilica NPs were observed together with the main bands of doxorubicin (the characteristic sharp peak at 1727 cm−1 is related to the carbonyl (CO) of the pure doxorubicin). Finally, the absorption spectrum of the ssOSCs@DOX was also recorded showing maximum peaks at 470 and 496 nm (Fig. 7D). The ssOSCs@DOX were then functionalized with amino–silane and further covered with the negative lipids, as previously described for the calcein loaded samples. Fig. S10A† includes the FTIR spectra of ssOSCs@DOX–NH2-negative lipids. It is possible to observe the presence of the characteristic bands coming from the organosilica groups, the disulfide breakable bonds, the doxorubicin fingerprint and the lipid bands. The hydrodynamic diameter obtained by DLS was around 100 nm (Fig. S10B†) and the ζ potential was −29.2 ± 2.2 mV, demonstrating again the successful coating of the silica core with the lipidic shell.
The breakable properties of the nanocages and the effect of the lipidic shell on the release kinetics were evaluated for the doxorubicin-loaded ssOSCs and conducted by mimicking the physiological conditions in cancer cells, and in particular the glutathione concentration. The reduction of the disulfide groups in the ssOSCs was achieved by adding a solution of glutathione (10 mM) to the particles suspended in a PBS solution at a final concentration of 0.1 mg mL−1 incubated at 37° C (pH = 7.4). Then, centrifugation of each vial led to the formation of a pellet with a supernatant that was collected at different time points (1, 3, 5, 7 and 24 h). In the same volume of supernatant, we expected to see different amounts of the released drugs depending on the time. Fig. S11A and S11B† show the absorption spectra of the supernatant of naked and lipid-coated ssOSCs@DOX–NH2, respectively. A time-dependent increment in the doxorubicin absorption signal intensity in the supernatant was observed only in the presence of the reducing agent (GSH) for both naked and lipid-coated NPs. These results confirmed that the degradation of the NPs was triggered by the reduction of the disulfide bonds present in the silica framework of the ssOSCs. However, differences were observed between naked and lipid-coated ssOSCs@DOX–NH2 (Fig. S11C†): lipid-coated ssOSCs exhibited a slower and smaller amount of dox release compared with the naked NPs. In particular within the first hour without the lipidic coverage the naked nanoparticles released more than 50% of the entrapped DOX. Data are in agreement with previously published works, demonstrating that the lipidic bilayer offers a valid shell to (1) retain the encapsulated molecule and (2) prevent the rapid drug leakage and release from the NP pores, maximizing the drug accumulation in the intracellular compartments.20,24,26
Finally, the tolerability of the tested cells (B16-BL6 and PC3 cells) to the exposure of ssOSCs@DOX (both lipid-coated and naked NPs) was determined by incubating increasing quantities of NPs (15, 30, 60 and 120 μg mL−1) for 2, 4, 24 and 48 h (Fig. 8). Unloaded ssOSCs were also tested as a negative control to corroborate the absence of toxicity for the carriers in the absence of the anticancer drug. The cell viability assays revealed that the naked and empty ssOSCs induce minimal effects on cell toxicity, even at the highest dose during the last time point tested (Fig. 8A and B). The lipid-coated and empty ssOSCs produced a minimal decrease in cell proliferation, probably attributed to their higher internalization level inside the cells (yet confirmed by confocal microscopy and flow cytometry). Remarkably, in the two tested cell lines, both ssOSCs@DOX–NH2 and lipid-coated ssOSCs@DOX–NH2 induced significant mortality. More interestingly, Fig. 8C and D demonstrate that when the DOX-loaded nanocages were coated with the lipid layer, the proliferation was significantly reduced compared with the DOX-loaded naked ones in the two cell lines. This trend, in the decrease of the cell viability, when treating both cell lines with the ssOSCs@DOX–NH2-negative lipids (120 μg mL−1), can be observed after 4 h and 24 h of incubation. The viability was compared to the cultures treated with the naked ssOSCs loaded with the same amount of DOX at the same time points. Indeed, statistically significant differences were obtained when comparing the cell viability of PC3 cells treated with naked or lipid coated ssOSCs@DOX after 24 h. These findings demonstrate how the presence of the lipid layer around the NPs favour their internalization toward the cell cytoplasm and does not hinder the cytotoxic drug release resulting in the highest efficiency of the delivered drug.
A previously published strategy was employed for the synthesis of the breakable ssOSCs. In summary, 408 mg (1.12 mmol) of cetyltrimethylammonium (CTAB) was dissolved in 50 mL of deionized water and magnetically stirred for 30 min at 250 rpm at 50 °C. Then, an ammonia aqueous solution (12.5 μL) was added and the stirring speed was increased to 750 rpm. Subsequently, 448.1 μL (2 mmol) of tetraethyl orthosilicate (TEOS) and 102.8 μL (0.223 mmol) of bis[3-(triethoxysilyl)propyl]disulphide (BTDS) were mixed and added to the previous solution and stirred at 750 rpm, for 20 h at 50 °C. Subsequently, APTES (87.2 μL) was added to the stirring solution and the reaction mixture was stirred for 14 h at 50 °C. The particle dispersion was purified by dialysis against an EtOH/H2O/AcOH (1:1:0.007 v/v/v) mixture for 24 h and finally against an EtOH/H2O (1:1 v/v) mixture for another 24 h whereby the dialysis solution was replaced every 2 h, when possible.
For the colocalization study and the internalization experiments, the ssOSCs–NH2 were labelled with the sulfo–Cy5–NHS probe. First, a sulfo–Cy5–silane was prepared by suspending a solution of sulfo–Cy5–NHS ester (0.5 mg, 0.643 μmol) in dry dimethylsulfoxide (DMSO). Afterwards, APTES (4.5 μL, 0.142 M in dry DMSO) was added and the reaction mixture was allowed to stir for 30 min in the dark.
The obtained ssOSCs were purified by dialysis against an EtOH/H2O/AcOH (1/1/0.007 v/v/v) mixture for 72 h, then against EtOH/H2O (1/1 v/v) for 24 h and finally against dH2O for 24 h. The dialysis solutions were replaced every 12 h.
The resulting naked and functionalized ssOSCs were characterized by a broad battery of physicochemical techniques. The dimensions and morphology of the NPs were evaluated by transmission electron microscopy (TEM) using an Energy Filter Transmission Electron Microscope (EFTEM, Zeiss Libra 120). For TEM observations, samples were deposited onto a TEM copper grid. The size distribution and the surface charge of the nanoparticles were obtained employing a dynamic light scattering (DLS) instrument. The DLS measurements were performed on dispersions of ssOSCs in dH2O (pH 7) using Zetasizer Ultra equipment equipped with Multi-Angle Dynamic Light Scattering (MALDLS®) technology from Malvern Panalytical and using the software ZS Xplorer. Fourier Transform Infra-Red (FTIR) spectra were recorded using a Shimadzu IRAffinity-1 spectrometer. The transmittance spectrum was collected using a spectral resolution of 1 cm−1 accumulating 64 scans from 600 to 4000 cm−1. Thermogravimetric assay (TGA) was conducted on a Netzsch model STA 449 fi Jupiter instrument. The samples (0.5–3 mg) were maintained at 100 °C for 30 minutes for stabilization and then heated from 130 to 800 °C at a speed of 10 °C min−1, before being held at this temperature for a further 30 minutes at the end of the measurement. The analysis was carried out under a 20 mL min−1 airflow. Nitrogen physisorption isotherms were obtained to evaluate the porosity of the ssOSCs with a Micromeritics ASAP-2020 physisorption instrument. The particle sample was degassed at 100 °C for 12 h. The N2 adsorption/desorption measurement was performed at −196 °C. The surface areas were calculated using the Brunauer–Emmett–Teller (BET) method in the relative pressure range (p/p0) of 0.06–0.3. The pore size distributions and pore volumes were calculated using the classical method on the adsorption branch using a cylindrical model. The total pore volume was calculated to be P/P0 0.99. The emission spectra of Cy5 functionalized NPs were recorded on a Horiba Jobin–Yvon IBH FL-322 Fluorolog 3 spectrometer equipped with a 450 W xenon arc lamp, double grating excitation, emission monochromators (2.1 nm mm−1 of dispersion; 1200 grooves per mm) and a TBX-04 single photon-counting detector. The samples were excited by a wave laser at λex = 633 nm. The emission of the samples was collected in the range from 640 to 820 nm (Fig. S12†). The presence of primary amines in the surface of the ssOSCs was assessed using the Kaiser test (Sigma Aldrich) and by measuring the absorbance in a Shimadzu UV-3600 spectrophotometer double-beam UV-VIS-NIR spectrometer with quartz cuvettes with a path length of 10 mm.
In the case of calcein, a solution of CaCl2 2 M in ethanol was employed as a solvent for the encapsulation approach. Briefly, 20 mg of naked ssOSCs was dissolved in 5 mL of CaCl2 2 M (in ethanol). Meanwhile, 20 mg of calcein molecules were also dissolved in 5 mL of CaCl2 2 M (in ethanol). Both solutions were vigorously vortexed and sonicated for 10 min separately until they were completely dissolved. Then, they were mixed and briefly sonicated for a further 20 min and stirred for 12 h at room temperature. Successively, NPs were functionalized with cyclic silane, as previously mentioned, and they were finally washed several times to discard the non-encapsulated calcein.
Before the lipid coating, ssOSCs@DOX and ssOSCs@CAL were covered with a positive cyclic silane and stored at 4 °C until use. In particular, 10% of 2,2-dimethoxy-1,6-diaza-2-silacyclooctane was incubated overnight at room temperature with the loaded NPs using toluene as the solvent and in the presence of NH3 28%. The positive NPs were washed three times with water and stored at 4 °C until further use. The loaded ssOSCs were characterized as previously described by DLS, ζ potential measurements, TEM and FTIR. Moreover, the absorption of the ssOSCs@DOX and ssOSCs@CAL was measured on a Shimadzu UV-3600 spectrophotometer double-beam UV-VIS-NIR spectrometer and baseline corrected. Quartz cuvettes with a path length of 10 mm were used.
The functionalized organosilica nanocages (ssOSCs–NH2) synthesized in this work show a positive ζ potential; therefore a negatively charged phospholipid mixture was ad hoc designed to efficiently exploit electrostatic interactions driving the lipid self-assembly on the nanocages surface, as recently reported.40 The phospholipids were purchased from Avanti Polar Lipids: DOPA (1,2-dioleoyl-sn-glycero-3-phosphate) as a negatively charged lipid, DOPC (1,2-dioleoyl-sn-glycero-3-phosphocholine dissolved in chloroform, by Avanti Polar Lipids) as a neutral one, and DSPE–PEG(2000)–amine (1,2-distearoyl-sn-glycero-3-phosphoethanolamine-N-[amino(polyethylene glycol)-2000]. The phospholipids were mixed with cholesterol (from Sigma Aldrich) in chloroform, in a molar ratio of DOPA/DOPC/DSPE–PEG(2000)–amine/cholesterol equal to 50/10/1.5/38.5, and dried under vacuum overnight in glass vials. The obtained lipid film was then rehydrated with a 2:3 volume ratio of ethanol/bd water solution, obtaining a final concentration of 3 mg mL−1. As a control, a non-charged lipid mixture was prepared, substituting the DOPA fraction with DOPC, thus having DOPC/DSPE–PEG(2000)–amine/cholesterol with a 60/1.5/38.5 molar ratio.
ssOSCs or ssOSCs–NH2, dispersed in water, were sonicated for 3 minutes at 59 kHz using a sonication bath (Branson 3800 CPXH, Branson Ultrasonics Corporation); subsequently, ethanol was added to the nanoparticle dispersion to reach a volume ratio of 2:3 ethanol to water. Then, the lipid solution was added to the nanoparticle dispersion at a weight ratio of 2:1 (preferred option) or a 1:1 nanoparticle to lipid ratio. Thereafter, the mixture was sonicated for 3 minutes to increase homogeneity. Finally, to self-assemble the lipid bilayer on the nanoparticle surface, an excess of deionized water was added to the mixture, until reaching a 1:9 ethanol to water volume ratio. The final suspension was then sonicated for 5 minutes to obtain better size uniformity and to help the formation of a homogeneous self-assembled lipid bilayer encasing the nanoparticles. Similarly, control liposomes were obtained: the lipid mixture in 2:3 ethanol to water solution was sonicated for 3 minutes; successively, water was added achieving a 1:9 ethanol to water volume ratio and 5 minutes sonication was eventually performed for homogeneity.
To characterize the size distribution and colloidal stability of the coated nanoparticles, DLS and Z-potential measurements (Zetasizer Nano ZS90 from Malvern Instruments) and Nanoparticles Tracking Analysis (NTA, NanoSight NS300 from Malvern Panalytical) were performed in deionized water and at room temperature. All the measurements were conducted 3 times and then averaged. In the case of NTA, for each sample, three 60-second videos of the samples flowing through the instrument chamber were recorded and analyzed with the NTA 3.4 software from Malvern Panalytical.
In order to prove the correct formation of the lipid layer around the nanocages, fluorescence microscopy colocalization analyses were performed. In particular, Cyanin 5-labelled nanocages (ssOSCs–NH2–Cy5) were obtained in a one-pot synthetic approach. Lipids, after nanocages coating, were labelled with DiO (DiOC18(3) (3,3′-dioctadecyloxacarbocyanine perchlorate)) from ThermoFisher Scientific, adding 0.5 μL of 10 μg mL−1 DiO solution in DMSO for each mg of lipid-coated nanocages. The nanoconstructs were then incubated at 37 °C for 30 minutes in shaking mode (200 rpm). After the incubation, 5 μL of lipid-coated nanocage dispersion was deposited on a glass slide, coated by a cover glass slip and analyzed through an inverted wide-field fluorescence microscope (Eclipse TiE from Nikon) equipped with a 100× oil-immersion PlanAPO objective. At least 10 multichannel images from different regions were taken for each sample and analyzed with the colocalization tool of the NIS software (NIS-Elements AR 4.5, Nikon). In particular, the objects in the far-red channel (representing the nanocages), the ones in the green channel (representing the lipids) and the colocalized spots in the merged image were counted and the colocalization percentage was calculated following the formula:
For each sample, the colocalization percentage was calculated for 10 images and then the results were averaged.
The point corresponding to ac on the t axis was individuated as the coagulation time (tc) and used to compare the samples. Three independent experiments were carried out and the resulting coagulation times were averaged.
Finally, the release of calcein loaded within the lipid-coated NPs (ssOSCs@CAL–NH2-negative lipids) was also assessed by confocal microscopy. Cells were incubated for 8, 24 and 48 h with the calcein-loaded and lipid-coated ssOSCs (0.05 mg mL−1). Calcein was observed exciting the sample at λ = 488 nm, cell cytoplasm was stained with phalloidin-Alexa568 (λ = 568 nm), nuclei were labelled with Hoechst (λ = 405 nm) and NPs were visualized upon excitation at λ = 633 nm, thanks to Cy5.
Furthermore, an enhanced cellular uptake, which proves the key role of the lipid coating in mediating the internalization of the nanoparticles, was observed. The efficient intracellular delivery of the therapeutic agent effectively affected cancer cells, demonstrating the potentiality of the lipid-coated nanocages as a powerful tool in anticancer research.
Footnotes |
† Electronic supplementary information (ESI) available: Estimation of amine groups on the NP surface, DLS and Z-potential, nanoparticle tracking analysis, fluorescence microscopy co-localization results, additional characterization of nanocages and lipid-coated nanocages, haemocompatibility assays, additional characterization of nanocages loaded with calcein and doxorubicin, and videos of 3D reconstruction of internalization of lipid-coated nanocages within cells. See DOI: https://doi.org/10.1039/d3nr02155f |
‡ These authors have equally contributed to the work. |
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