Colloidal plasmonic gold nanoparticles and gold nanorings: shape-dependent generation of singlet oxygen and their performance in enhanced photodynamic cancer therapy
Received 7 November 2017
Accepted for publication 24 January 2018
Published 5 April 2018 Volume 2018:13 Pages 2065—2078
Checked for plagiarism Yes
Review by Single anonymous peer review
Peer reviewer comments 3
Editor who approved publication: Dr Linlin Sun
Yamin Yang,1 Yue Hu,2 Henry Du,3 Lei Ren,4 Hongjun Wang5
1Department of Biomedical Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing, Jiangsu, China; 2Department of Biological and Environmental Engineering, Cornell University, Ithaca, NY, USA; 3Department of Chemical Engineering and Materials Sciences, Stevens Institute of Technology, Hoboken, NJ, USA; 4Department of Biomaterials, College of Materials, Xiamen University, Xiamen, Fujian, China; 5Department of Biomedical Engineering, Chemistry and Biological Sciences, Stevens Institute of Technology, Hoboken, NJ, USA
Introduction: In recognition of the potentials of gold nanoparticles (Au NPs) in enhanced photodynamic therapy (PDT) for cancer, it is desirable to further understand the shape-dependent surface plasmonic resonance (SPR) properties of various gold nanostructures and evaluate their performances in PDT.
Materials and methods: Monodispersed colloidal spherical solid Au NPs were synthesized by UV-assisted reduction using chloroauric acid and sodium citrate, and hollow gold nanorings (Au NRs) with similar outer diameter were synthesized based on sacrificial galvanic replacement method. The enhanced electromagnetic (EM) field distribution and their corresponding efficiency in enhancing singlet oxygen (1O2) generation of both gold nanostructures were investigated based on theoretical simulation and experimental measurements. Their shape-dependent SPR response and resulted cell destruction during cellular PDT in combination with 5-aminolevulinic acid (5-ALA) were further studied under different irradiation conditions.
Results: With comparable cellular uptake, more elevated formation of 1O2 in 5-ALA-enabled PDT was detected with the presence of Au NRs than that with Au NPs under broadband light irradiation in both cell-free and intracellular conditions. As a result of the unique morphological attributes, exhibiting plasmonic effect of Au NRs was still achievable in the near infrared (NIR) region, which led to an enhanced therapeutic efficacy of PDT under NIR light irradiation.
Conclusion: Shape-dependent SPR response of colloidal Au NPs and Au NRs and their respective effects in promoting PDT efficiency were demonstrated in present study. Our innovative colloidal Au NRs with interior region accessible to surrounding photosensitizers would serve as efficient enhancers of PDT potentially for deep tumor treatment.
Keywords: gold nanoparticles, colloidal gold nanorings, surface plasmonic resonance, photodynamic therapy
The unique optical properties and associated surface plasmonic resonance (SPR) effects of gold (Au) nanostructures have proven useful for multifaceted biomedical applications including bioimaging, biomolecule sensing, thermally modulated drug delivery, photothermal cancer therapy, photodynamic therapy (PDT), etc.1–5 Typically, gold nanomaterials exhibit collective electron charge oscillations named localized surface plasmon resonances (LSPRs), through which the optical absorption and scattering can be dramatically enhanced with elevated local near-field amplitude at the resonance frequency. Such LSPR properties greatly depend on the particle shape, size, and dielectric environment.6–9 With recent advances that allow the controlled synthesis and dedicate fabrication of gold materials on a nanoscale, the plasmonic response of Au nanostructures can be tuned for different purposes.10
The cell destruction mechanism underlying the photodynamic reaction combines the activation of photosensitizer (PS) molecules under light irradiation, generation of cytotoxic reactive oxygen species (ROS) (mainly composed of singlet oxygen, 1O2) following energy transfer from activated PS to surrounding oxygen molecules, and ROS-triggered cell death via the apoptosis and/or necrosis pathway.11 The active involvement of gold nanomaterials in PDT could offer at least two advantages over other nanomaterial-based drug delivery systems: significantly elevated 1O2 generation and increased treatment depth for deep tumors.12,13 Our previous findings have highlighted that, in addition to delivering more PS to cells, plasmonic gold nanomaterials could significantly amplify the electromagnetic (EM) field and elevate 1O2 formation, which consequently led to more destruction of cancer cells.14–18 Furthermore, by modulating the morphology and geometry, the plasmonic absorbance of Au nanostructures can be tuned into near-infrared (NIR) regions, allowing PDT for deep tumors under NIR light irradiation.19–21
In our previous studies, we have successfully synthesized various Au nanostructures with different sizes,22 opposite surface charges, different surface modifications, mitochondria-targeting capability,15 and tunable structure and controllable dimensions,17 and have tested their utility for enhanced PDT of cancer. In particular, we have theoretically and experimentally analyzed the size-dependent and surface charge-dependent enhancement of ROS formation enabled by spherical solid gold nanoparticles (Au NPs). We have also utilized our novel colloidal gold nanorings (Au NRs) as a drug delivery device and PS enhancer in PDT.23,24 In the present work, we further compared two types of gold nanostructures (Au NPs and Au NRs) with identical surface composition and outer diameter to investigate the shape-dependent SPR response during PDT. Particular emphasis was made to elucidate their corresponding efficiency in enhancing 1O2 formation due to the elevated EM field under different irradiation conditions, including the use of NIR light as a light source.
Materials and methods
Cobalt chloride hexahydrate (CoCl2•6H2O 99.99%), sodium borohydride (NaBH4 99%), sodium citrate trihydrate, gold(III) chloride solution (30 wt% of HAuCl4 in dilute HCl), poly(vinylpyrrolidone) (PVP) (weight-average molecular weight=2,500 g/mol), 5-aminolevulinic acid (5-ALA), and protoporphyrin IX (PpIX) were purchased from Sigma-Aldrich Co. (St Louis, MO, USA). The deionized water used in this study was 18.2 MΩ Milli-Q filtered by Quantum Ex, Ultrapure Oranex Cartridge filtration columns (EMD Millipore, Billerica, MA, USA).
Synthesis of Au nanostructures and characterization
Au NRs were synthesized based on a sacrificial galvanic replacement method, in which cobalt nanoparticles were used as the template. The detailed synthesis process was described in our previous reports.14,18,23,24 Briefly, 100 μL of 0.4 M CoCl2•6H2O and 400 μL of 0.1 M sodium citrate trihydrate were mixed with 100 mL Milli-Q water. The solution was deaerated with a continuous argon flow for 40 min. Then, 1 mL of freshly prepared 0.1 M NaBH4 and 200 μL of 1% (weight/volume [w/v]) PVP (molecular weight=2,500 g/mol) were simultaneously added to the solution under vigorous stirring to obtain cobalt nanoparticles. Subsequently, 150 μL of 0.1 M HAuCl4 was dropwise added to the cobalt nanoparticle solution and kept stirring for another 30 min. Then, the solution was exposed to the ambient environment, allowing for oxidization of unreacted cobalt. Solid Au NPs were synthesized using a modified Lee and Meisel method with the aid of ultraviolet (UV) irradiation. Briefly, 1% (w/v) aqueous sodium citrate (4 mL) was added to HAuCl4 solution (5 mM, 40 mL). The mixture was then irradiated with UV for 30 min under stirring. To ensure both Au nanostructures bear the same surface chemistry, the obtained Au NPs were also coated with PVP by mixing 1 mL PVP solution (1 mg/mL) with 9 mL synthesized Au NPs under constant stirring overnight. To remove free PVP, the reacting solution was centrifuged under 10,000 rpm for 10 min and washed with Milli-Q water twice. A transmission electron microscope (TEM) (Philips CM20; FEI, Hillsboro, OR, USA) was used to examine the size and morphology of the prepared Au nanostructures. The plasmon resonances of prepared Au nanostructures were measured using a UV–visible multimode microplate reader (Synergy™ HT; BioTek Instruments, Inc., Winooski, VT, USA) with 1 nm resolution. The size and zeta-potential values of Au nanostructures were measured using laser Doppler electrophoresis with a Zetasizer (Nano-ZS; Malvern Instruments, Malvern, UK).
Plasmonic simulation of Au nanostructures
Computational simulation of plasmonic properties of Au NPs and Au NRs was performed using the discrete dipole approximation (DDA) algorithm implemented in the DDSCAT 7.3 code developed by Draine and Flatau.25,26 Target Au nanostructures were respectively constructed based on the captured TEM images of Au NPs and Au NRs. BLENDER3D (version 2.78; Blender Foundation, www.blender.org) was used to generate a triangular mesh file of the 3D target geometries in this study. This file was then converted to a DDA compatible shape file using the online tool DDSCAT Convert (available at nanohub.org). The overall target is composed of 33,552 dipoles for Au NPs and 44,416 dipoles for Au NRs. The optical spectra and near-field distribution of Au nanostructures were calculated using the dielectric constant of bulk Au taken from Johnson and Christy.27
Measurement of 1O2 generation
The probe of Singlet Oxygen Sensor Green reagent (SOSG; Sigma-Aldrich Co.) could emit detectable green fluorescence in the presence of 1O2, and thus SOSG was used to measure 1O2 generation with Au NPs or Au NRs under different conditions. Briefly, 50 μL of Au nanostructure solution with the same gold concentration (2 mM) was mixed with 50 μL of 10 μM PpIX. Then, 50 μL of 10 μM SOSG was added to the mixture under dark conditions with a total volume of 150 μL. Samples in 96-well plates were then irradiated with broadband light, 600 nm long pass (LP) filtered light, and 700 nm LP filtered light for different time durations. The fluorescence intensity was measured 1 min after irradiation using a multimode microplate reader (Synergy HT; BioTek Instruments, Inc.) at an excitation wavelength of 485/20 nm and an emission wavelength of 528/20 nm.
Cell culture and cytotoxicity test
The triple-negative human breast adenocarcinoma cell line MDA-MB-231 (American Type Culture Collection [ATCC], Manassas, VA, USA) was used for cellular PDT tests. MDA-MB-231 cells have been reported for their resistance to traditional chemotherapies, aggressive pathological features, and high rates of metastasis and recurrence, and stand as a suitable in vitro model for evaluating PDT efficiency.28,29 MDA-MB-231 cells were cultured in Leibovitz L-15 Medium (Sigma-Aldrich Co.) supplemented with 10% fetal bovine serum and 1% penicillin/streptomycin in a humidified incubator at 37°C without CO2. Media were refreshed every 2 days and the cells were passaged at a confluence of 70%–80%. For cytotoxicity evaluation, cells were incubated with Au NRs or Au NPs at the same gold concentration (40 μM, 80 μM, and 160 μM, respectively) for 24 h, and the cell viability was determined using the MTT (Sigma-Aldrich Co.) assay. Briefly, cells after different treatments were incubated with MTT (0.5 mg/mL in cell culture medium) for 2 h. The formazan crystals were dissolved with dimethyl sulfoxide (DMSO; Sigma-Aldrich Co.). Absorbance of the extracted solubilized formazan was measured at 570 nm by subtracting the background signal in the 96-well plate with a multimode microplate reader (Synergy HT; BioTek Instruments, Inc.).
Cellular uptake of Au nanostructures and their intracellular distribution
To quantify the cellular uptake of Au nanostructures, Au NRs and Au NPs were respectively suspended in serum-free cell culture medium at the same gold concentration (40 μM) and added into cultured MDA-MB-231 cells with identical density. Upon incubation for 4 h, free particles were removed by washing thoroughly with Hank’s buffered salt solution (HBSS) at least three times. Then, the cells were trypsinized, centrifuged, and washed again with HBSS before collection. The collected cells were lysed with an alkaline buffer consisting of sodium dodecyl sulfate and 1 N sodium hydroxide and the lysates were analyzed by spectrometric assay for Au nanostructure quantification as described previously.16 The normalization was done via the areas under the UV absorbance spectrum (400–800 nm); that is, the area was calculated in the untreated control group and then subtracted from that in Au NP and Au NR groups respectively. Then, the value obtained in the Au NR group was divided by the value in the Au NP group for normalization.
To determine the intracellular destination of different Au nanostructures after uptake, MDA-MB-231 cells incubated with respective Au nanostructures as described above were rinsed with HBSS to remove free particles, trypsinized, washed, and centrifuged into cell pellets. Cell pellets were fixed with 4% paraformaldehyde (EM Sciences, Hatfield, PA, USA) for 2 h at room temperature, postfixed with 1% osmium tetraoxide for 1 h, dehydrated in a graded series of ethanol solutions, and then embedded in epoxy resin. Ultrathin sections (~70 nm) were obtained by a Leica Ultracut Ultramicrotome (Leica Microsystems Inc., Buffalo Grove, IL, USA) and examined with a TEM (Philips CM20; FEI). Monolayer cells cultured on a well plate and treated with different Au nanostructures were also fixed and embedded as above. Then, the Au nanostructure-incubated cells were examined under a focused ion beam scanning electron microscope (Zeiss Auriga Small Dual-Beam FIB-SEM; Carl Zeiss Microscopy, LLC., Thornwood, NY, USA).
Intracellular 1O2 measurement
For the cell-based intracellular 1O2 measurement, SOSG was prepared at a final concentration of 1.33 μM in HBSS according to the manufacturer’s protocol. MDA-MB-231 cells treated with 5-ALA with/without Au nanostructures were incubated with the SOSG solution for 2 h and refreshed with 100 μL HBSS for light irradiation. After irradiation, the cells were further incubated at 37°C in the dark for 20 min and then the fluorescence intensity was measured using the microplate reader with the excitation wavelength at 485/20 nm and the emission wavelength at 528/20 nm.
Cellular photodynamic therapy
The PDT procedure was conducted according to our previous studies.15,22 Briefly, cells were seeded into a 96-well plate at a concentration of 3×104 cells/mL in 200 μL culture medium, and cultured for 24 h prior to PDT treatment. The final cell density is 6,000 cells per well in the 96-well plate, which is within the range of 5×102–5×105 cells per well for the following MTT assay according to the protocol. Afterwards, the culture medium was then replaced with the serum-free medium containing 5-ALA with/without different Au nanostructures. The final concentrations of gold and 5-ALA in all experiments were kept at 40 μM and 1 mM, respectively. Serum-free medium was used as blank controls. After incubation for 4 h in dark, the media were replaced with 100 μL HBSS and the cells were irradiated from the top with a broadband light source using a 150 W halogen lamp (100 mW/cm2, Dolan-Jenner Fiber-Lite MI-150; Dolan-Jenner Industries, Boxborough, MA, USA) for 1 min. For the NIR light irradiation, the same light source but filtered through 600 nm or 700 nm filters (FEL600 and FEL 700; Thorlabs, Inc., Newton, NJ, USA) was applied to cells for 10, 20, and 30 min, respectively. After irradiation, the culture was replaced with complete culture media and incubated for 24 h prior to any further evaluations.
Cell viability assessment
The cell viability upon different treatments was determined by MTT assay as described in the cytotoxicity test above. To confirm the MTT assay results, MDA-MB-231 cells after PDT treatment were also fluorescently stained for viability using a Live/Dead VR Viability/Cytotoxicity kit (Invitrogen, Thermo Fisher Scientific, Waltham, MA, USA). Briefly, cells cultured on glass cover slips after PDT treatment were gently washed with HBSS and then incubated with the Live/Dead VR Viability/Cytotoxicity solution for 30 min. Viable cells were stained green by calcein acetoxymethyl (0.05%), while the nuclei of dead cells were stained red by ethidium homodimer-1 (0.2%). The stained cells were examined under a Nikon Eclipse 80i epifluorescent microscope (Nikon Instruments, Melville, NY, USA). To visualize cell morphology changes after PDT treatment, cultures were fixed with 4% formalin and stained with phalloidin (Alexa FluorH 488 phalloidin; Biotium Inc, Hayward, CA, USA) for filamentous actin and 4,6-diamidino-2-phenylindole (dilactate) for cell nuclei. The stained cells were also examined under the Nikon Eclipse 80i epifluorescent microscope.
All quantitative results were obtained from at least triplicate samples. Data were expressed as the mean ± SD. Unpaired Student’s t-test was used in the statistical analysis of experimental data. p<0.05 was considered statistically significant.
Results and discussion
Characterization of Au nanostructures
Following a similar synthesis procedure as described previously,23 colloidal Au NRs were facilely prepared by galvanic replacement of sacrificial cobalt nanoparticles in gold salt solution with low molecular weight PVP as a stabilizing agent. In contrast to the solid spherical structures of Au NPs, the as-prepared Au NRs exhibited a typical ring-like structure (Figure 1A). Depending on the size of cobalt nanoparticles, Au/Co ratio, and PVP molecular weight, the outer diameter, inner diameter, and height of Au NRs could be tuned.23 For this study, the outer diameter of Au NRs was kept similar to the diameter of Au NPs with an average of ~40 nm as determined by dynamic light scattering measurement. The Polydispersity Index for Au NPs and Au NRs is 0.264 and 0.272, respectively. The exact geometry parameters of Au nanostructures are schematically illustrated in Figure 1. Although PVP was used as the stabilizing agent for both Au NRs and Au NPs, a slightly negative zeta potential (−10 mV) was measured with Au NPs, while Au NRs remained electrically neutral (0 mV). This may come from the short chain of PVP that cannot completely shield the negatively charged citrate. Due to structural difference, Au NRs showed distinctive SPR properties from Au NPs. As shown in Figure 1B, Au NPs had a maximum absorbance wavelength at ~528 nm in the UV–visible absorption spectra, while Au NRs showed a red shift of the SPR peak with a maximum absorbance wavelength at 653 nm.
Simulation of optical spectra and near-field distribution of Au nanostructures
As shown in Figure 1C, the calculated extinction peak at 510 nm for Au NPs and 690 nm for Au NRs through DDA simulation is the net result of absorption and scattering by Au nanostructures, which is in satisfactory agreement with experimental results. Note that a broadening of the SPR band and a slight shift of the peak position were observed in the experimental spectra for both Au NPs and Au NRs. This could most likely be attributed to size variation and interparticle distributions in as-prepared gold nanomaterials. Clearly, the morphology of Au nanostructures has a strong influence on their interactions with light, resulting in a noticeable red shift of the resonance peak towards the NIR region in the case of Au NRs. Due to the presence of SPR, the intensity of the localized EM field near the surface of Au nanostructures would also closely correlate with their morphology. To better understand the differential enhancement of the EM field by Au NPs and Au NRs, theoretical calculation was done using DDA methods. The respective simulation images of EM field distribution for Au NPs and Au NRs at excitation light with different wavelengths (532 nm, 633 nm, and 785 nm) are depicted in Figure 1D. The calculated maximum electric field ratio between Au NPs and Au NRs at each wavelength is 1:1.5, 1:6.4, and 1:5.4, respectively. In consistence with our previous report on the simulation using finite-difference time domain modeling,23 the EM field inside the Au NR cavity was substantially enhanced, which is probably attributed to the significant coupling between the two EM modes of the inner and outer surfaces of the ring structure. Comparison of the EM field enhancement under incident light with various wavelengths shows the maximum field enhancement at 532 nm for Au NPs and 633 nm for Au NRs, suggesting shape-dependent LSPR of Au nanostructures.
Enhanced 1O2 generation induced by Au nanostructure–PS
To determine the contribution of the plasmonic effect of Au nanostructures to 1O2 formation as well as to ascertain the shape-dependent 1O2 enhancement, PpIX, a derivative of 5-ALA, was used as a model PS. PpIX as a commercial PDT drug has shown good success against skin basal cell carcinoma and squamous cell carcinoma.30 Using SOSG as the highly selective fluorescent probe for 1O2,31 we were able to monitor the time-resolved formation of 1O2 from PpIX with the presence of Au nanostructures. By offsetting the contribution of SOSG, Figure 2 shows the time-resolved net 1O2 formation enhanced by Au NPs and Au NRs with the presence of PpIX under various light irradiations. Based on Figure 2A, we calculated the 1O2 enhancement ratio of 1:1.43 between Au NP-PpIX and Au NR-PpIX under the broadband light irradiation. To determine whether such an enhancement would remain for longer wavelengths, especially in the NIR range, broadband light respectively filtered through 600 nm and 700 nm LP filters was used as the irradiation source. Clearly, the Au NR-PpIX-elevated 1O2 generation was continuously observed (Figure 2B and 2C). As calculated, the enhancement ratio between Au NP-PpIX and Au NR-PpIX for 1O2 generation with 600 nm LP filtered light was 1:1.34 after 20 min irradiation and with 700 nm LP filtered light it was 1:1.20. Apparently, these results affirm the shape dependence of Au nanostructure-assisted 1O2 generation, which to a certain degree agrees well with the EM field distribution from the theoretical simulation (Figure 1D). Despite their similar physicochemical characteristics (ie, surface chemistry and size) to solid Au NPs, Au NRs did demonstrate a much higher efficiency in promoting 1O2 formation. It is speculated that when the incident light is in resonance with the SPR of Au NRs, a substantial enhancement of the EM field would occur in the ring cavity besides the inner and outer surfaces, which cannot be seen with solid Au NPs. With a comparable surface area, easy access of PpIX to the central region of Au NRs would lead to more activation of PpIX and consequently more 1O2 formation than that of Au NPs.
As noted in Figure 1, the SPR absorbance of Au NRs is in the NIR range, thus, it would be of great benefit to achieve enhanced 1O2 generation under light irradiation with longer wavelengths (λ>600 nm). For efficient photodynamic reaction, matching the PS absorption with excited light spectra becomes crucial for maximum quantum yield of 1O2. As PpIX itself cannot be irradiated efficiently under the NIR light, we thus postulate that the SPR peak of Au NRs could, at least partially, fit with 600 nm LP and 700 nm LP filtered light to induce an increase of the photonic energy upon light irradiation and subsequently enhance the photocurrent between Au NRs and PpIX. Through nonradiative energy transfer and coupling to the surface plasmons of Au NRs, more PpIX can be excited to their triplet and singlet states and therefore result in more 1O2 generation (Figure 2B and 2C).
Cytotoxicity and cellular uptake of Au nanostructures
Biocompatibility of various Au nanostructures was examined prior to following cell-based PDT tests. As shown in Figure 3A, both Au nanostructures at various concentrations showed negligible cytotoxicity to MDA-MB-231 cells after 24-h incubation. As the amount of Au nanostructures ingested by cells would contribute to the treatment efficiency of PDT, cellular uptake of different Au nanostructures was also evaluated for the possible dependence on morphology. Upon complete release from the collected cells, the amount of Au nanostructures ingested by MDA-MB-231 cells was quantified spectrometrically and no significant difference was observed between Au NPs and Au NRs, indicating that the morphological change of Au NRs may have a minimal effect on the cellular uptake (Figure 3B). Although Au NRs have distinct morphology from solid Au NPs, they both share the circular shape with a similar outer diameter. As evidenced from previous studies, the diameter of Au spheres plays an essential role in regulating their cellular endocytosis and exocytosis and the size of 40–50 nm seems optimal for intracellular accumulation.32 Thus, it is not surprising to see comparable accumulation of Au NPs and Au NRs in MDA-MB-231 cells.
To further understand the intracellular distribution of different Au nanostructures, thin slices of the cell pellets posttreated with respective Au nanostructures were examined under a TEM. Regardless of particle morphology, a majority of Au nanostructures was located in the intracellular vesicles (Figure 3C and 3D). Direct visualization of the cells incubated with Au NRs under a bright-field confocal microscope and the focused ion beam scanning electron microscope examination of the cell cross-sections also confirmed the cellular internalization of Au NRs (see Figure S1). Clearly, minimal cytotoxicity and efficient uptake by breast cancer cells imply the potential of Au NRs in cancer PDT.
Enhanced intracellular 1O2 generation enabled by Au nanostructure–PS
Intracellular elevation of 1O2 production upon light irradiation is a crucial indicator for enhancing the PDT efficacy.33 Intracellular 1O2 formation and corresponding cellular destruction following PDT under various conditions are indicated in Figure 4. Following a similar trend to that of the cell-free study on 1O2 formation, the combination of Au NRs and 5-ALA (Au NRs+5-ALA) yielded the highest intracellular 1O2 level after broadband light irradiation (Figure 4A). More importantly, upon irradiation with a longer wavelength (ie, 600 nm LP and 700 nm LP filtered light), cells treated with 5-ALA and Au NRs still yielded the highest 1O2, significantly higher than the other two groups (Figure 5A and 5B). To ensure the increase of intracellular 1O2 is not from the increase of intracellular accumulation of PS, we quantified the intracellular PS (ie, PpIX) by measuring the fluorescence intensity. Interestingly, no significant difference was identified among all three groups (data not shown). Thus, it is believed that Au nanostructures have minimum effect on the cellular uptake of 5-ALA, or at least the production rate of PpIX, and they may mainly work as the 1O2 enhancer in the present study. Consistent with cell-free conditions, the intensified EM fields in the vicinity of excited intracellular Au nanostructures can activate PS via resonance energy transfer, leading to a higher level of 1O2 generation. Once again, the significant difference in intracellular 1O2 levels found between Au NRs and Au NPs is primarily attributed to their structural distinction; that is, the substantially enhanced EM field of Au NRs would activate more PS trapped in the cavity.
To our interest, under NIR light irradiation, the highest 1O2 level was consistently observed in the cells treated with Au NRs+5-ALA, and discernible in those with Au NPs+5-ALA or 5-ALA alone (Figure 5A and 5B). It is noted that intracellular PpIX alone (maximum absorbance at ~400 nm) could be barely activated by the NIR light,34 as also was seen for the solid Au NPs with a characteristic SPR peak at ~530 nm. On the contrary, Au NRs with resonant absorption at a NIR wavelength will produce an intensified EM field and sufficient energy transfer for PS activation and 1O2 generation. Therefore, great intracellular 1O2 enhancement can still be achieved with the presence of Au NRs with strong SPR absorption under NIR light irradiation.
Au nanostructure–PS assisted cellular PDT
The efficacy of elevated 1O2 in killing cancer cells with the presence of different Au nanostructure–PS combinations was determined by MTT assay. As shown in Figure 4B, under broadband light irradiation for 1 min, both Au NRs and Au NPs could lead to more cell killing than 5-ALA only. In particular, Au NRs+5-ALA yielded the highest destruction of MDA-MB-231 cells (75.5%), accounting for about twofold that from 5-ALA alone (33.9%) and 1.5 times that from a 5-ALA+Au NP combination. This observation was confirmed by fluorescently staining MDA-MB-231 cells for viability (live/dead staining) and morphology (filamentous actin staining) after various PDT treatments. Consistent with MTT results, more dead cells were found in the Au NRs+5-ALA group (Figure 4C and 4D). Considering negligible cytotoxicity and comparable cellular uptake of both Au NRs and Au NPs, the improved cell killing by Au NRs must be from its structural contribution, offering unique SPR properties and a significant increase of intracellular 1O2 generation. Note that the 5-ALA–Au nanostructure-induced cell destruction became less proportional to the elevated levels of 1O2, which may be due to the intrinsic intracellular protection mechanism against 1O2.35 Depending on the dosage and location of 1O2 formation, 1O2-triggered cell killing comprises apoptosis or apoptosis in combination with necrosis, involving multiple signaling pathways, and is further complicated by the anti-apoptotic and pro-apoptotic regulation of the Bcl-2 family in mitochondria.36–38
Similar to the findings of cell-free 1O2 generation, under NIR light irradiation only Au NRs+5-ALA treatment yielded noticeable cell destruction but not the other two groups (Figure 5C and 5D). With either 600 nm LP filtered light for 20 min or 700 nm LP filtered light for 30 min Au NRs+5-ALA led to 40.5% or 31.4% more cell killing than Au NPs+5-ALA, respectively. Consistently with numerical simulation, the concentrated EM field near Au NRs under NIR light exposure may play a key role resulting in an increased population of excited PSs. Meanwhile, photobleaching of PSs could be affected by their easy entry to the center cavity of Au NRs, and more excitation–emission cycles would occur prior to photobleaching of PSs during the excited state; that is, PSs can be activated and generate singlet oxygen more efficiently.39 This finding becomes clinically relevant especially considering that NIR light normally has better tissue penetration depth.40 The use of NIR light for PDT can potentially address the major technical challenge associated with current PDT practice; that is, it is only suitable for superficial tumor tissues due to limited light penetration. The SPR properties of Au NRs in the NIR region hold particular advantages for extending current PDT towards deep tumor treatment.
Both Au NPs and Au NRs have the potential to convert photonic energy into heat especially under intensive light irradiation, which accounts for the photothermal effects as reported elsewhere.41,42 However, it was found that tumor cells usually required relatively high laser energy to be photothermally damaged even with the assistance of Au nanostructures.42 The energy density of the irradiation source in our study (100 mW/cm2) is at least 10 times lower than that employed in photothermal therapy. Therefore, cell destruction caused by the temperature changes due to photothermal effects can be excluded from our study. To affirm this, separate control experiments were performed to compare the cell viability of cells treated with Au nanostructures alone under light irradiation. Negligible cell destruction was detected for both 20-min and 30-min irradiation with 700 nm LP filtered light (Figure S2). In addition, early reports also suggested that the generation of 1O2 can be induced directly by noble metal nanostructures under light irradiation.43–46 However, the formation of 1O2 caused by Au nanostructures alone has also demonstrated great dependence on the dosage and energy density of the irradiating light source. Pulsed lasers rather than a continuous wavelength light source, which was used in the current study, would result in much more significant 1O2 generation relying on Au nanostructures themselves under light exposure.43 We have also confirmed that Au NPs alone did not cause significant enhanced 1O2 generation with or without light irradiation (data not shown). Therefore, the combinative effects of Au nanostructures and PSs should be the major contributor to enhanced intracellular 1O2 and subsequent increased cell death in our present findings.
In this study, shape-dependent SPR properties of different Au nanostructures were characterized and studied for their performance under various PDT conditions. As a result of the unique morphological attributes, Au NRs exhibited plasmonic resonance in the NIR range, exhibiting efficient PS activation and corresponding 1O2 generation for cell destruction with NIR light irradiation. Clearly, cell destruction enabled by NIR-absorbing Au NRs sheds promising light on the efforts to address the depth limitation with current PDT for deep tumor therapy. Although not fully explored, the interior space and outer surface of Au NRs can be separately modified for designated functionality, which offers multifaceted potentials in chemical and biological sensing, drug delivery, and bioimaging.
This work was supported by the Natural Science Foundation of China (Grant Number: 81601532 and 31428007), the Natural Science Foundation of Jiangsu Province (BK20160814), and the Scientific Research Foundation of Nanjing University of Aeronautics and Astronautics (1003-YAH16009). Due to a recent reorganization, the affiliation for Dr Hongjun Wang is now known as Department of Biomedical Engineering, Stevens Institute of Technology, Hoboken, NJ, USA.
The authors report no conflicts of interest in this work.
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