Near-Infrared Driven Gold Nanoparticles-Decorated g-C3N4/SnS2 Heterostructure through Photodynamic and Photothermal Therapy for Cancer Treatment

Introduction

Recently, cancer is the preeminent cause of mortality worldwide.1,2 Several strategies have been implemented to treat cancer. Photodynamic therapy (PDT) has garnered widespread attention owing to its various advantages, including good applicability, high selectivity, non-invasiveness, intense repeatability, and low toxicity.3–9 When exposed to light irradiation, a specific photosensitizer (PS) can produce cytotoxic reactive oxygen species (ROS) that lead to cellular apoptosis (destruction of DNA and protein).10–13 PSs react with biological molecules of substrates that may interact with triplet oxygen (3O2) or H2O in Type-I PDT, resulting in the production of O2−˙ and OH˙ radicals.14 Moreover, PSs can initiate a Type-II PDT pathway to release 1O2 by directly transferring energy to 3O2. The combined Type-I and II PDT pathways have attracted considerable attention for clinical applications. Photothermal therapy (PTT) converts near-infrared (NIR) light energy into hyperthermia at the tumor site, resulting in tumor ablation.15,16 PTT has attracted considerable interest in cancer therapy owing to its high photothermal stability, spatial and temporal resolution, enhanced conversion efficiency, minimal invasiveness, high selectivity, good biocompatibility, and non-toxicity.17–24 Heat generation in localized tissues through PTT can boost blood flow for improved O2 delivery, resulting in a synergistic effect with PDT. The synergistic strategies of PDT and PTT have enormous potential in cancer treatment to improve therapeutic efficiency and overcome complications.4

Photocatalytic therapies have garnered considerable interest owing to their favorable chemical and physical functions, strong light absorption, distinct structures, and promotion of photoinduced electron-hole pair separations.25–27 The design of semiconductor heterostructure photocatalytic materials can improve the photocatalytic efficiency with enhanced electron-hole pair separation under light irradiation, which has received attention for cancer treatment. Graphitic carbon nitride (g-C3N4) is a two-dimensional (2D) semiconductor material with various advantages, including enhanced chemical and thermal stability, a unique layered structure, high specific surface area, low cost, low toxicity, good biocompatibility, and intense photocatalytic activity.28–32 It possesses a moderate band gap (2.7 eV) that can respond to the ultraviolet (UV) and visible regions and has a stronger reduction ability to generate ROS with the activation of molecular oxygen.33 Furthermore, g-C3N4 nanosheets (NSs) can act as PSs to inhibit cancer cells, leading to an improved PDT.34,35 However, g-C3N4 NSs have a fast recombination rate of photoexcited charge carriers and low photon absorption ability, which hinder their application.28,29,36,37 The manufacturing of g-C3N4-based heterostructure nanocomposites using metal oxides, noble metal nanoparticles, and semiconductor materials is an effective strategy that can improve photogenerated charge carrier separation, inhibit the recombination rate, and enhance light absorption efficiency.28,36 Tin disulfide (SnS2) is a n-type semiconductor with a band gap of 2.1–2.4 eV and has been extensively studied in various applications including sensors, batteries, photocatalysis, and optoelectronics owing to its improved surface-to-volume ratio, non-toxicity, chemical stability, low cost, and good photocatalytic reduction activity.29,36,38–42 Furthermore, SnS2 NSs exhibit enhanced photocatalytic performance and good biocompatibility, and can be utilized for biological applications.40 SnS2 can be utilized as an NIR-activated material because of its slight absorption of NIR light and its photothermal activity.43,44 The incorporation of 2D heterojunctions with g-C3N4 materials enhances the charge carrier separation, which improves the photocatalytic activity and increases the efficiency of light absorption.

Plasmonic nanomaterials, particularly Au nanoparticles accompanied by semiconductor nanostructures, have attracted considerable attention for biomedical applications owing to their intense NIR light absorption, good biocompatibility, enhanced physiochemical properties, catalytic activities improved photothermal performance, controlled reduction, facile synthesis controllable changing morphology, shape size, excellent bioimaging, drug delivery, and strong localized surface plasmon resonance effects.5,45–48 The integration of plasmonic and semiconductor-based nanostructures acts as an electron mediator that can intensify the interfacial electron transfer from the adjacent heterojunction semiconductor materials of the conduction band, promote the separation of electron-hole pairs, enhance photocatalytic activity, and improve light absorption in the NIR region.49,50 Moreover, combined plasmonic metal and semiconductor heterostructure nanomaterials can promote PDT and PTT effects, which can induce cell apoptosis in cancer treatment. The combination of semiconductor heterostructure nanomaterials and plasmonic metal has limited investigation for cancer treatment.

Zhang et al28 designed Ti3C2/g-C3N4 heterostructure with modification of triphenylphosphonium bromide (TPP) to form Ti3C2/g-C3N4-TPP NSs, which exhibited intense PDT and PTT effects under the NIR light irradiation. Yang et al fabricated Bi2Se3/Au (BS/Au) heterostructure, and these heterostructure was later modified using poly (ethylene glycol) methyl ether-block-poly (lactide-co-glycolide) (PLGA-PEG) for improved solubility and biocompatibility.10 Finally, doxorubicin (DOX) was loaded onto the BS/Au@PLGA-PEG to generate BS/Au@PP-DOX. These nanocomposites enhanced the multimodal synergistic effects of PTT and chemotherapy in cancer treatment.

Herein, we designed a 2D heterostructure (g-C3N4/SnS2), in which the surface was decorated with Au nanoparticles to generate g-C3N4/SnS2@Au nanoparticles. The synthesized nanoparticles PDT and PPT effects was explored under NIR laser irradiation in details. Moreover, nanoparticle’s biocompatibility, cytotoxicity, and antitumor efficacy have been extensively discussed through both In vitro and in vivo investigations. The synthesized nanoparticles can be considered promising candidates for cancer treatment through synergistic therapeutic effects with NIR laser irradiation. The schematic representation of g-C3N4/SnS2@Au nanoparticles with synergistic PDT/PTT effects for the cancer treatment is shown in Scheme 1.

Scheme 1 Schematic diagram for synthesis of g-C3N4/SnS2@Au nanoparticles and its synergistic PDT/PTT effects for cancer therapeutics.

Materials and Methods

The materials information, and characterizations details are available in the Supplementary Information.

Synthesis of g-C3N4 Nanosheets

Urea (30 g) was placed in a sealed alumina crucible and calcinated to 550°C (4 h) under muffle furnace. The resultant yellow solid powder was then heated to 500°C (2 h) in order to generate g-C3N4 nanosheets.

Synthesis of g-C3N4/SnS2

g-C3N4/SnS2 was synthesized via hydrothermal process. Briefly, SnCl4.5H2O (2.2 g) and TAA (0.88 g) was added into deionized (DI) water (80 mL). After that, the aforementioned solution was supplemented with the appropriate quantity of g-C3N4. The solution was stirred for 15 min. Then mixture solution was transferred into the autoclave and heated (180°C, 24 h), then cool down at ambient temperature. Then the obtained precipitated was centrifuged, rinsed with DI and ethanol for various times. Lastly, the resulting yellow precipitated was dried (80°C, 12 h).

Synthesis of g-C3N4/SnS2@Au Nanoparticles

The synthesized g-C3N4/SnS2 (30 mg) was suspended in 30 mL DI water and then agitated for 30 min. Subsequently, Au nano seeds (300 µL) were added above into the solution, and gently stirred. The 10 mM HAuCl4 solution and sodium citrate (0.04 M) were added into the aforementioned mixture solution while constant stirring. Subsequently, ascorbic acid (0.1 M) was mixed, and the solution was reacted for 30 min. The resulting precipitated solution was centrifuged and rinsed with DI water. Lastly, the g-C3N4/SnS2@Au nanoparticles were dried at 60°C in the oven overnight.

Photothermal Effect of Nanoparticles

The photothermal effect of g-C3N4/SnS2@Au nanoparticles was evaluated at various concentrations by irradiation of NIR laser (1 W/cm2, 10 min). The photothermal stability was investigated over three rounds of turning the laser on and off, and the nanocomposites’ temperature fluctuations were measured. The aqueous nanoparticles (1 mg/mL) were subjected under 808 nm laser for 600 s to determine their photothermal conversion efficiency (η). Afterwards, the laser was switched off, allowed to cool down at ambient temperature. The “η” for nanoparticles was determined from our previous studies.5

Extracellular ROS Generation

The g-C3N4/SnS2@Au nanoparticles were immersed with methylene blue (MB) solution (10 µg/mL) and IPA. The sample was exposed to 808 nm laser light at several time durations of 0, 10, 20, and 30 min. The OH. was detected at 664 nm wavelength by UV-Vis spectroscopy. The DPBF as a ROS probe was used for the detection of 1O2 generation. Firstly, stock solution DPBF (0.5 mg/mL) in DMSO was prepared. Consequently, an aqueous solution of g-C3N4/SnS2@Au (1 mg/mL) was mixed into the DPBF solution followed by ultrasonication treatment. This reaction was carried out in dark conditions. The mixture solution was subjected to an NIR laser at different time intervals. Finally, the samples’ absorbance was calculated at 410 nm wavelength using UV-Vis spectroscopy. For the detection of extracellular ROS, the DCFH-DA ROS probe was employed. The DCFH-DA (0.5 mL, 1 mM) solution was dissolved methanol and mixed thoroughly. The aforementioned mixture solution was then mixed with 10 mM NaOH solution, followed by stirring for 30 min in dark atmosphere. Subsequently, PBS (pH = 7.4, 10 mM) was added to the mixture to make it neutral. The aforementioned DCFH-DA solution was immersed with g-C3N4/SnS2@Au nanoparticle solution (1 mg/mL). The mixture solution was subjected to NIR laser for different time intervals (0, 5, and 10 min), respectively. The samples fluorescence intensity at 426 nm wavelength was collected through photoluminescence spectra.

Cytotoxicity Studies

Normal fibroblast (L929) and human liver carcinoma cancer (HepG2) cell lines were cultivated in a 96-well plate (24 h). After that, several concentrations of nanoparticles were added. The cells were subjected under 808 nm laser (1 W/cm2, 5 min). Cell cytotoxicity in HepG2 was examined using the Cell Counting Kit-8 (CCK-8) test. The absorbance of cells was calculated at 450 nm wavelength by an ELISA (Thermo fisher scientific, Finland) reader. The cell lines used in this study were purchased from ATCC cell bank.

Cellular Uptake Analysis

The cellular uptake analysis of g-C3N4/SnS2@Au nanoparticles was performed using inductively coupled plasma-mass-spectrometry (ICP-MS). HepG2 cells (3 × 105) were seeded in a 35 mm culture petri dishes and incubated at 37°C for 24 h. Then culture medium was changed and the cells were washed with PBS. Subsequently, the g-C3N4/SnS2@Au nanoparticles were added inside the cell solution. Further, the cells with nanoparticles were incubated for 1 and 4 h. After incubation, the cells were further treated with hydrochloric acid. Then cellular uptake analysis was performed g-C3N4/SnS2@Au nanoparticles in the cells were determined using ICP-MS.

In vitro Detection of ROS

A ROS probe, DCFH-DA was used to identify the intracellular ROS, which quickly oxidized to DCF products. HepG2 cells (3 × 105) were grown overnight in a culture dish. The g-C3N4/SnS2@Au (250 µg/mL) nanoparticles were added after the medium was aspirated, and PBS was used to wash cells. The cells were stained with nuclei marker 4’,6-diamidino-2-phenylindole (DAPI, 10 µM). Furthermore, the dish was incubated (30 min) after the addition of 10 µM of DCFH-DA. The NIR laser was subjected to the cell solution. Fluorescence microscopy was used to detect ROS.

Animal Experiment

HepG2 cells (2 × 106) were subcutaneously injected into Balb/c mice (4-week-old). Afterwards, the growing tumors were separated into three groups: control, g-C3N4/SnS2@Au (250 μg/mL, 100 µL), and g-C3N4/SnS2@Au nanoparticles (250 μg/mL, 100 µL) irradiated under 808 nm laser (0.75 W/cm2) for 10 min. Tumor volume and body weight were recorded throughout the treatment periods. The following equation was used to determine the tumor volumes was as follows: Tumor volume where “L” denotes tumor’s length, and “W” stands as the width of the tumor. The mice were euthanized after 14 days of treatment. Their major organs, such as the heart, lungs, kidneys, liver, and spleen, as well as tumors were accumulated and immersed in formalin. Hematoxylin and eosin (H&E) were used to stain tissue slices for histological analysis. All animal experiments were conducted according to the protocols and approval of the Institutional Animal Care and Use Committee of Taipei Medical University (TMU) (document number: LAC2022-0445).

Statistical Analysis

The SPSS software 18.0 (Chicago, USA) was used to do the statistical calculations for all the experimental data. For statistical significance, p<0.05 is denoted by the notation “*”.

Results and Discussion Characterization of g-C3N4/SnS2@Au Nanoparticles

The transmission electron microscopy (TEM) images of the g-C3N4, g-C3N4/SnS2 and g-C3N4/SnS2@Au nanoparticles are presented in Figure 1A–C. g-C3N4 clearly appeared as a 2D sheet structure (Figure 1A). SnS2 was uniformly attached to the g-C3N4 surface (Figure 1B). The average particle size of SnS2 was approximately calculated as 8 nm. The growth of SnS2 was shown as a sheet and an ellipsoid-shaped structure that covered the g-C3N4 surface. The different morphologies of SnS2 may depend on the solvent used, which plays an important role in controlling the morphology of SnS2.39 Au nanoparticles were then coated onto the surface of g-C3N4/SnS2 (Figure 1C). The Au nanoparticles appeared spherical in shape with average particle size about 15 nm (Figure S1). The high-resolution TEM (HRTEM) images of g-C3N4/SnS2@Au are shown in Figure S2, and the lattice d-spacing of SnS2 assigned to the (100) and (101) planes was approximately 0.28 and 0.315 nm, respectively. Moreover, the d-spacing of the Au nanoparticles was 0.24 nm, which corresponded to the (111) crystal plane (Figure S2). The EDS mapping in Figure 1D shows the presence of C, N, Sn, S, and Au without any impurities, indicating the successful synthesis of g-C3N4/SnS2@Au nanoparticles.

Figure 1 TEM images of (A) g-C3N4. (B) g-C3N4/SnS2. (C) g-C3N4/SnS2@Au nanoparticles. (D) EDS mapping of g-C3N4/SnS2@Au nanoparticles.

The crystalline structure of samples was evaluated using X-ray diffraction (XRD) patterns and the results are presented in Figure S3. Two diffraction peaks appeared at 13.06° and 27.75° which correspond to the characteristic planes (100) and (002) of g-C3N4.27 The diffraction peaks at 15.11°, 28.37°, 32.49°, 46.44°, 50.01°, 55.86°, 58.79o, 59.80 o, 63.43 o, and 70.55 o corresponded to (001), (100), (101), (102), (110), (111), (200), (201), (202), and (113) planes of SnS2 (JCPDS No. 23–0677). The deposition of Au nanoparticles appeared at 2θ angles of 38.27°, 44.41°, 64.59° and 78.33 o which attributed to crystal planes (111), (200), (220) and (311), respectively, indicating the face-centered cubic structure (JCPDS No. 04–0783). This suggests that the Au nanoparticles were successfully deposited onto g-C3N4/SnS2. The g-C3N4 and SnS2 diffraction peaks well matched with their standard patterns. These results indicate the successful synthesis of g-C3N4/SnS2@Au nanoparticles. Further chemical structures of all the samples were identified by Fourier-transform infrared spectroscopy (FTIR), as presented in Figure 2A. The absorption band at 3000–3400 cm−1 was attributed to the stretching vibration of the N-H group bound to the O-H group, the characteristic peaks at 1634 and 1545 cm−1 were attributed to the C=N stretching vibration, and the characteristic peaks at 1407, 1318, and 1233 cm−1 were ascribed to the C-N stretching vibration modes of g-C3N4. Furthermore, the peaks at 811 cm−1 corresponded to the s-triazine ring modes.36 The absorption peak at 591 cm−1 was attributed to Sn-S bond of SnS2. The remaining characteristic peaks did not alter for g-C3N4/SnS2, which indicated the growth of SnS2 on g-C3N4. For the g-C3N4/SnS2@Au nanoparticles, no extra vibrational peaks appeared for the Au-O bond because the Au-O vibrational peak overlapped with the out-of-plane bending modes of the CN heterocycles.37 Moreover, the peaks at 812 cm−1 had reduced intensity as compared to g-C3N4/SnS2 which confirmed the presence of Au nanoparticles on the surface of g-C3N4/SnS2. A slight shift in peak was observed at 3151 cm−1 for g-C3N4/SnS2@Au nanoparticles, which attributed to N-H stretching vibration with O-H bond. However, the other peaks did not change for the g-C3N4/SnS2@Au nanoparticles, indicating the successful fabrication of g-C3N4/SnS2@Au nanoparticles. The UV spectra of all samples are presented in Figure 2B. Pure g-C3N4 and SnS2 exhibited strong absorption at 450 and 550 nm, respectively. The corresponding band gaps of g-C3N4 and SnS2 were evaluated and its value were 2.7 eV and 2.1 eV, respectively, as presented in Figure 2C. g-C3N4/SnS2 exhibits a strong absorption peak intensity due owing to the hybridization of g-C3N4 and SnS2.39 Moreover, after decoration with Au nanoparticles, the g-C3N4/SnS2@Au nanoparticles exhibited a broad NIR light absorption region with increased absorption peak intensity, which could enhance cancer therapeutic treatment. These nanoparticles could be considered as a promising photothermal therapeutic agent and displayed improve photocatalytic activity by signifying charge carrier separation.

Figure 2 (A) FTIR spectra of g-C3N4, SnS2, g-C3N4/SnS2, and g-C3N4/SnS2@Au nanoparticles. (B) UV-Vis-NIR absorption spectra of g-C3N4, SnS2, g-C3N4/SnS2, and g-C3N4/SnS2@Au nanoparticles. (C) The corresponding band gap of g-C3N4 and SnS2.

The chemical compositions and valence states of the g-C3N4/SnS2@Au nanoparticles were investigated using X-ray photoelectron spectroscopy (XPS) (Figure 3). The C 1s spectrum showed two peaks at 284.2 and 287.5 eV which were attributed to SP2 hybridized C-C bond and N-C=N bonds of g-C3N4, respectively (Figure 3A). The N 1s spectra exhibited four distinct peaks at 398.9, 399.91, 400.1, and 404.2 eV which were attributed to the C-N=C, C-N-C, N-(C)3, and π-excitation that arise due to the generation of amino C-N-H bond, respectively (Figure 3B).51 Two peaks in the Sn 3d spectrum at 485.6 and 494.2 eV corresponded to Sn 3d3/2 and Sn 3d5/2, respectively (Figure 3C). The S 2p spectrum exhibited two peaks at 160.5 and 161.6 eV which corresponded to S 2p3/2 and S 2p1/2, respectively, indicating the presence of sulfur anion in SnS2 (Figure 3D). The Au 4f spectrum exhibited two peaks at 83.1 and 86.7 eV due to the presence of Au 4f5/2 and Au 4f7/2, respectively, concluding Au coating on the surface of g-C3N4/SnS2 (Figure 3E). Hence, the aforementioned findings suggest the successful synthesis of g-C3N4/SnS2@Au nanoparticles.

Figure 3 XPS spectra of g-C3N4/SnS2@Au nanoparticles for (A) C 1s. (B) N 1s. (C) Sn 3d. (D) S 2p. (E) Au 4f.

Photothermal Properties, and ROS Detection of g-C3N4/SnS2@Au Nanoparticles

The photothermal properties of the g-C3N4/SnS2@Au nanoparticles were evaluated and are presented in Figure 4A and B. Different concentrations (0.25, 0.5, and 1 mg/mL) of the composite nanoparticles were subjected to NIR laser irradiation (Figure 4A). The temperature of the nanoparticles increased with increasing sample concentration. These nanoparticles exhibited 41 °C temperature at 1 mg/mL concentration. In contrast, the temperature of control group (water) was raised to 25 °C. Thus, the nanoparticles enhanced the PTT effect owing to the presence of a prominent Au nanoparticles as photothermal agent. The photostability of g-C3N4/SnS2@Au nanoparticles was evaluated (Figure 4B). No notable temperature changes were observed after three laser on/off cycles, indicating that these nanoparticles had enhanced photothermal stability. The η value of nanoparticles was 41%, suggesting an excellent photothermal conversion performance. Thus the above findings indicate that these nanoparticles can be utilized as intense photothermal agents to inhibit cancer cells. Hence, these nanoparticles can serve as potent PTT agents for cancer treatment. The degradation activity of the g-C3N4/SnS2@Au nanoparticles was assessed using methylene blue (MB) under laser irradiation. The intensity of the absorption peak at 664 nm for the g-C3N4/SnS2@Au nanoparticles decreased significantly with increasing irradiation time (Figure 4C). After 30 min of laser irradiation, the MB was completely degraded. The above results indicate that the g-C3N4/SnS2@Au nanoparticles can enhance hydroxyl radical (OH˙) formation under 808 nm laser irradiation, thereby improving photocatalytic activity for ROS generation towards MB degradation. Furthermore, these nanoparticles suggesting that the enhance the electron-hole pair separation and declined the recombination to promote the photocatalytic activity through 808 nm laser irradiation. Thus, these nanoparticles can improve the PDT effect because g-C3N4 can be utilized as a promising PS under laser irradiation to induce cancer cell death.52 ROS formation was monitored using the dichloro-dihydro-fluorescein diacetate (DCFH-DA) fluorescent probe (Figure 4D). The ROS generation ability of the g-C3N4/SnS2@Au nanoparticles was irradiated using an 808 nm laser. The fluorescence intensity of the g-C3N4/SnS2@Au nanoparticles increased continuously with increasing irradiation time due to enhancement of ROS generation with respect to time. Here, ROS generation are responsible in the presence of g-C3N4, as an intense photosensitizing agent. These nanoparticles enhanced ROS generation by varying irradiation time. Therefore, g-C3N4/SnS2@Au nanoparticles intensified ROS generation, which can lead to the inhibition of tumor cells by PDT. DPBF served as a ROS probe for investigating singlet oxygen (1O2). The g-C3N4/SnS2@Au nanoparticle solutions were laser irradiated, as shown in Figure 4E. The absorbance of the sample solution decreased drastically with increasing irradiation time. After 10 min of irradiation, the absorbance intensity of the DPBF solution containing g-C3N4/SnS2@Au nanoparticles with standard characteristic peaks at 410 nm gradually decreased under laser irradiation, suggesting intense ROS generation due to the g-C3N4 used as a photosensitizer.35 Therefore, these nanoparticles enhanced the PDT effect under laser irradiation, inducing cell apoptosis.

Figure 4 (A) The photothermal properties of g-C3N4/SnS2@Au nanoparticles at various concentrations exposed to 808 nm laser. (B) The photothermal stability of g-C3N4/SnS2@Au nanoparticles exposed to 808 nm laser over three on/off cycles. (C) The MB activity of g-C3N4/SnS2@Au nanoparticles measured at various exposure times. (D) ROS detection monitored using DCFH-DA fluorescence spectra treated with different irradiation times of g-C3N4/SnS2@Au nanoparticles (808 nm, 1 W/cm2). (E) Absorbance spectra of DPBF mixed with g-C3N4/SnS2@Au nanoparticles for various laser irradiations.

In vitro Synergistic Therapy

The viability of the L929 cells cultured with g-C3N4/SnS2@Au nanoparticles at various concentrations are shown in Figure 5A. Even at a higher concentration (1000 µg/mL), no toxicity was observed in normal cells. The cell viability of g-C3N4/SnS2@Au nanoparticles was greater than 97%, even at higher concentrations. Thus, the g-C3N4/SnS2@Au nanoparticles exhibited good biocompatibility. The cell viability of g-C3N4/SnS2@Au nanoparticles against HepG2 cells irradiated with laser group was decreased as compared to the both control group and unirradiated laser group (Figure 5B). Without laser irradiation group, the cell viability of nanoparticles was over 85%, however with laser irradiation the cell viability was 20%. The HepG2 cells treated with g-C3N4/SnS2@Au nanoparticles under laser irradiation exhibited higher cytotoxicity than the unirradiated and control groups. The cell viability of HepG2 cells treated with g-C3N4/SnS2@Au nanoparticles decreased to 20% under an 808 nm laser owing to synergistic effects of PDT and PTT. The improved PDT and PTT effects occurred due to the intense photosensitizer (g-C3N4) and photothermal agent (Au nanoparticles) that can lead to effective cellular apoptosis. Moreover, the intense photosensitizer under exposure to light irradiation produced ROS, which killed the HepG2 cancer cells. As a result, PDT effect occurred. Light absorption converts optical energy into heat energy using the photothermal agent, resulting in cancer cell death to prompt the improved PPT effect. Hence, the concurrent treatment of PDT and CDT can lead to intensified cellular damage as compared to monotherapy treatment. Therefore, g-C3N4/SnS2@Au nanoparticles with laser treatment exhibited higher cellular apoptosis due to a synergistic therapeutic effect. Therefore, these nanoparticles possess intense therapeutic efficiency and can induce 80% cell apoptosis through combinational therapeutic effects for cancer treatment. The cellular uptake behavior of the g-C3N4/SnS2@Au nanoparticles was investigated using fluorescence microscopy (Figure 5C). HepG2 cells incubated with g-C3N4/SnS2@Au nanoparticles for various incubation times were observed. These nanoparticles can be effectively internalized into cells through endocytosis. Therefore, these nanoparticles possessed higher cellular uptake, which could be beneficial for intense therapeutic applications. Furthermore, ICP-MS technique was used to measure the internalized quantities of g-C3N4/SnS2@Au nanoparticles for HepG2 cells under various incubation time intervals (1 h and 4 h) and resultant data presented in Figure S4. The uptake amount of Au in HepG2 cells is significantly increased with increase in the incubation time period. This suggests that the variable incubation times can allow g-C3N4/SnS2@Au nanoparticles to penetrate HepG2 cells. The g-C3N4/SnS2@Au nanoparticles possessed three times higher cellular uptake for 4 h as compared to the 1h incubation time period. The above results proved that, the g-C3N4/SnS2@Au nanoparticles possessed higher cellular uptake which can effectively internalized in the cells through endocytosis. Furthermore, the HepG2 cells were stained with DAPI that can binds to cell nuclei (Figure 5D). It exhibited a weak blue fluorescence signal at 0.5 h incubation. Blue fluorescence intensity gradually and consistently increased with increasing incubation time. Thus with an increase in incubation time, these nanoparticles showed intense blue fluorescence, which could bind directly to nuclei and obstruct DNA replication. Hence, these nanoparticles can induce cellular apoptosis through an intense therapeutic effect. ROS generation was examined using DCFH-DA as a fluorescent probe in cells, which could liberate DCF products and enhance green fluorescence emission. HepG2 cells treated with g-C3N4/SnS2@Au nanoparticles via NIR laser irradiation exhibited an intense green fluorescence signal, as shown in Figure 5E. Conversely, g-C3N4/SnS2@Au nanoparticles exhibited weak fluorescence signals similar to those of the control groups. The laser-induced cytotoxicity of g-C3N4/SnS2@Au nanoparticles generated efficient ROS production that resulting the PDT therapeutic efficacy. Thus, g-C3N4/SnS2@Au nanoparticles under laser irradiation generated intensify ROS generation as g-C3N4 acts as a suitable PS. Therefore, these nanoparticles exhibit an improved PDT effect that can inhibit cancer cells.

Figure 5 (A) Viability of normal fibroblast cells (L929) at different concentrations of g-C3N4/SnS2@Au nanoparticles. (B) Cytotoxicity of human liver carcinoma cancer (HepG2) cells treated with g-C3N4/SnS2@Au nanoparticles at various concentrations with or without 808 nm laser irradiation (1 W/cm2, 5 min). (C) Bright field images of HepG2 incubated with g-C3N4/SnS2@Au nanoparticles for various incubation times (1) 0.5 h, (2) 1 h, and (3) 4 h. (D) Cellular uptake of HepG2 cells treated with g-C3N4/SnS2@Au stained with DAPI for different incubation times (1) 0.5 h, (2) 1 h, and (3) 4 h. (E) Fluorescence images of HepG2 cells stained with DCFH-DA (1) control, (2) g-C3N4/SnS2@Au, and (3) g-C3N4/SnS2@Au nanoparticles with 808 nm laser irradiation (*** denote p < 0.001 and ns denotes no significant difference).

In vivo Antitumor Effect

The antitumor effects of nanoparticles were evaluated in HepG2 tumor-bearing mice. The g-C3N4/SnS2@Au nanoparticles were intratumorally injected into mice. The tumor temperature was measured using an infrared thermal imaging camera. The tumor site temperature of g-C3N4/SnS2@Au nanoparticles was raised to 42.9°C compared to the control group (36.3°C) after 5 min laser irradiation (Figure 6A). These findings suggest that the g-C3N4/SnS2@Au nanoparticles exhibit an enhanced PTT effect in vivo which can damage tumor cells. The tumor volume of g-C3N4/SnS2@Au nanoparticles under laser irradiation exhibited an intense tumor ablation effect. Conversely, the control and non-irradiated groups showed no remarkable tumor inhibitory effects (Figure 6B). The body weights of the mice did not change during the treatment period, indicating that there were no side effects of the g-C3N4/SnS2@Au nanoparticles (Figure 6C). Therefore, g-C3N4/SnS2@Au nanoparticles with 808 nm laser irradiation possessed superior antitumor effects owing to the combined PDT and PTT effects. The g-C3N4/SnS2@Au nanoparticles group treated under irradiation of NIR laser demonstrated intense tumor growth suppression as compared to control group as represented digital photograph images of mice bearing tumors (Figure S5A and B). Figure 6D shows the hematoxylin and eosin (H&E)-stained images of the tumor tissue for various treatment groups. The g-C3N4/SnS2@Au nanoparticles under laser irradiation group showed severe tumor cell apoptosis as compared to the non-irradiated g-C3N4/SnS2@Au nanoparticle group, whereas no obvious damaged tumor cells were found in the control. Hence, the above results demonstrated that these nanoparticles exhibit superior anticancer effects with an 808 nm laser by a combination of therapeutic effects.

Figure 6 (A) Infrared imaging of tumor-bearing mice for control and g-C3N4/SnS2@Au nanoparticles subjected with an 808 nm laser. (B) Tumor volume and (C) body weight analysis of mice with different treatment groups control, g-C3N4/SnS2@Au and g-C3N4/SnS2@Au under 808 nm laser irradiation. (D) H&E staining images of tumor after various treatment groups control, g-C3N4/SnS2@Au and g-C3N4/SnS2@Au with irradiation of 808 nm laser (*** denote p < 0.001, scale bar = 100 µm).

H&E-stained images of the main organs are shown in Figure 7. As shown in Figure 7, no abnormal inflammation was observed after 14 days of treatment. Thus, these nanoparticles possessed good biocompatibility and enhanced antitumor efficiency through synergistic therapeutic PDT and PTT effects.

Figure 7 H&E-stained images of the main organs from various treatment groups (scale bar = 100 µm).

Conclusions

In summary, g-C3N4/SnS2@Au nanoparticles were successfully developed. The synthesized photocatalytic heterostructure nanomaterials exhibited high efficiency for photogenerated charge carrier separation and improved enhanced photocatalytic activity performance. The nanoparticles exhibited enhanced ROS formation by PDT pathways (Type-I and Type-II) through irradiation with an NIR laser because of the promising PS, g-C3N4. Moreover, these nanoparticles exhibited an intense PTT effect, which was derived from the Au nanoparticles through NIR laser irradiation. Both in vitro and in vivo results indicated that the g-C3N4/SnS2@Au nanoparticles exhibited high biocompatibility, efficient cancer cell apoptosis, and excellent tumor inhibition through synergistic PDT and PTT effects. The results proved that these nanoparticles have great potential as a combinatorial effect under 808 nm laser irradiation for cancer treatment.

Acknowledgments

The authors are grateful for the financial support provided by the National Science and Technology Council of Taiwan (NSTC 112-2221-E-027-038-MY3). We also would like to acknowledge the technical assistance from the Precision Analysis and Material Research Center of the National Taipei University of Technology (Taipei Tech).

Disclosure

The authors declare no known competing financial interests or personal relationships that could have influenced the work reported in this paper.

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