Rapid synthesis of a Bi@ZIF-8 composite nanomaterial as a near-infrared-II (NIR-II) photothermal agent for the low-temperature photothermal therapy of hepatocellular carcinoma

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快速合成Bi@ZIF-8复合纳米材料作为近红外二区光热剂用于肝细胞癌低温光热治疗

作者 Jinghua Li; Daoming Zhu; Weijie Ma; Yang Yang; Ganggang Wang; Xiaoling Wu; Kunlei Wang; Yiran Chen; Fubing Wang; Wei Liu; Yufeng Yuan 期刊 Nanoscale 发表日期 2020 ISSN 2040-3364 DOI 10.1039/d0nr03907a 类型 原创研究 (Original Research)

📄 英文摘要 English Abstract

EN

Hepatocellular carcinoma is the fourth leading cause of cancer-related deaths globally. Advanced nanomaterials have emerged as effective approaches to liver cancer therapy such as photothermal therapy. However, limited penetration depth of photothermal agents (PTAs) activated in the NIR-I bio-window and thermoresistance due to heat shock proteins restrict the therapeutic efficacy of PTT in HCC. Herein, we prepared a Bi@ZIF-8 (BZ) nanomaterial by a simple one-step reduction method. Then, gambogic acid, a natural inhibitor of Hsp90, was efficiently loaded onto the BZ nanomaterial via physical mixing. The characterization of the nanomaterial and release of GA due to pH change or NIR-light irradiation were separately studied. Photothermal conversion efficiency was calculated, and therapeutic studies were carried out in vitro and in vivo. This nanomaterial exhibited a significantly enhanced drug release rate when the temperature was increased under acidic conditions and had good light stability under laser irradiation and a photothermal conversion efficiency of about 24.4%. In addition, this novel nanomaterial achieved good therapeutic effects with less toxicity in vitro. The BZ nanomaterial loaded with GA caused tumor shrinkage as well as disappearance and effectively downregulated Hsp90 expression in tumors in vivo. Moreover, this novel nanomaterial exhibited good biocompatibility and potential for application in low-temperature PTT with excellent tumor destruction efficacy.

📄 中文摘要 Chinese Abstract

中文
肝细胞癌是全球癌症相关死亡的第四大原因。先进的纳米材料已成为肝癌治疗的有效手段,例如光热治疗。然而,在NIR-I生物窗口激活的光热剂(PTA)的穿透深度有限,以及热休克蛋白引起的热抗性限制了光热疗法在肝细胞癌中的治疗效果。目前可用的PTA,如金、银和钯纳米颗粒,已被广泛研究。然而,这些金属稀有且昂贵,限制了其临床大规模应用。具体而言,铋(Bi)作为一种典型的半金属元素,已引起科研人员的极大兴趣。铋是一种众所周知的"绿色金属",无毒且价格低廉。

📋 英文结构化总结 English Structured Summary

全文整理

EN

Background:

Hepatocellular carcinoma is the fourth leading cause of cancer-related deaths globally. Advanced nanomaterials have emerged as effective approaches to liver cancer therapy such as photothermal therapy. However, limited penetration depth of photothermal agents (PTAs) activated in the NIR-I bio-window and thermoresistance due to heat shock proteins restrict the therapeutic efficacy of PTT in HCC. The currently available PTAs, such as Au, Ag, and Pd nanoparticles, have been extensively investigated. However, these metals are rare and expensive, limiting their clinical large-scale application. Specifically, bismuth(Bi), a typical semi-metal element, has aroused great interest from scientific researchers. Bismuth is a well-known “green metal” that is nontoxic and inexpensive.

Methods:

Herein, we prepared a Bi@ZIF-8 (BZ) nanomaterial by a simple one-step reduction method. Then, gambogic acid, a natural inhibitor of Hsp90, was efficiently loaded onto the BZ nanomaterial via physical mixing. The characterization of the nanomaterial and release of GA due to pH change or NIR-light irradiation were separately studied. Photothermal conversion efficiency was calculated, and therapeutic studies were carried out in vitro and in vivo.

Results:

This nanomaterial exhibited a significantly enhanced drug release rate when the temperature was increased under acidic conditions and had good light stability under laser irradiation and a photothermal conversion efficiency of about 24.4%. In addition, this novel nanomaterial achieved good therapeutic effects with less toxicity in vitro. The BZ nanomaterial loaded with GA caused tumor shrinkage as well as disappearance and effectively downregulated Hsp90 expression in tumors in vivo. Moreover, this novel nanomaterial exhibited good biocompatibility and potential for application in low-temperature PTT with excellent tumor destruction efficacy.

Data Summary:

The photothermal conversion efficiency of the Bi@ZIF-8 composite nanomaterial was about 24.4%. In the clinical background, portal vein tumor thrombosis (PVTT) has been reported in about 35–50% of patients.

Conclusions:

This novel nanomaterial exhibited good biocompatibility and potential for application in low-temperature PTT with excellent tumor destruction efficacy.

Practical Significance:

This strategy offers a novel nanomaterial for the future clinical transformation of hepatocellular carcinoma treatment methods, enabling effective low-temperature photothermal therapy with reduced toxicity and deeper penetration using the NIR-II bio-window.

📋 中文结构化总结 Chinese Structured Summary

中文

背景:

肝细胞癌是全球癌症相关死亡的第四大原因。先进的纳米材料已成为肝癌治疗的有效手段,例如光热治疗。然而,在NIR-I生物窗口激活的光热剂(PTA)的穿透深度有限,以及热休克蛋白引起的热抗性限制了光热疗法在肝细胞癌中的治疗效果。目前可用的PTA,如金、银和钯纳米颗粒,已被广泛研究。然而,这些金属稀有且昂贵,限制了其临床大规模应用。具体而言,铋(Bi)作为一种典型的半金属元素,已引起科研人员的极大兴趣。铋是一种众所周知的"绿色金属",无毒且价格低廉。

方法:

在此,我们通过简单的一步还原法制备了Bi@ZIF-8(BZ)纳米材料。随后,将藤黄酸(一种天然的Hsp90抑制剂)通过物理混合高效负载到BZ纳米材料上。分别研究了纳米材料的表征以及由pH变化或近红外光照射引起的GA释放。计算了光热转换效率,并进行了体内外治疗研究。

结果:

该纳米材料在酸性条件下温度升高时表现出显著增强的药物释放率,且在激光照射下具有良好的光稳定性,光热转换效率约为24.4%。此外,这种新型纳米材料在体外实现了良好的治疗效果且毒性较低。负载GA的BZ纳米材料在体内导致肿瘤缩小甚至消失,并有效下调了肿瘤中Hsp90的表达。此外,这种新型纳米材料表现出良好的生物相容性,在低温光热治疗中具有应用潜力,并具备优异的肿瘤破坏效果。

数据总结:

Bi@ZIF-8复合纳米材料的光热转换效率约为24.4%。在临床背景下,约35-50%的患者中报告存在门静脉癌栓(PVTT)。

结论:

这种新型纳米材料表现出良好的生物相容性,在低温光热治疗中具有应用潜力,并具备优异的肿瘤破坏效果。

实际意义:

该策略为未来肝细胞癌治疗方法的临床转化提供了一种新型纳米材料,利用NIR-II生物窗口实现有效的低温光热治疗,降低毒性并增强穿透深度。

📖 英文全文 English Full Text

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Rapid synthesis of a Bi@ZIF-8 composite nanomaterial as a near-infrared-II (NIR-II) Cite this: Nanoscale, 2020, 12, 17064 photothermal agent for the low-temperature photothermal therapy of hepatocellular carcinoma Jinghua Li,†a Daoming Zhu, †b Weijie Ma,a Yang Yang,b Ganggang Wang,a Xiaoling Wu,a Kunlei Wang,a Yiran Chen,a Fubing Wang, *d Wei Liu *b,c and Yufeng Yuan *a Hepatocellular carcinoma is the fourth leading cause of cancer-related deaths globally. Advanced nanomaterials have emerged as effective approaches to liver cancer therapy such as photothermal therapy. However, limited penetration depth of photothermal agents (PTAs) activated in the NIR-I bio-window and thermoresistance due to heat shock proteins restrict the therapeutic efficacy of PTT in HCC. Herein, we prepared a Bi@ZIF-8 (BZ) nanomaterial by a simple one-step reduction method. Then, gambogic acid, a natural inhibitor of Hsp90, was efficiently loaded onto the BZ nanomaterial via physical mixing. The characterization of the nanomaterial and release of GA due to pH change or NIR-light irradiation were separately studied. Photothermal conversion efficiency was calculated, and therapeutic studies were carried out in vitro and in vivo. This nanomaterial exhibited a significantly enhanced drug release rate when the temperature was increased under acidic conditions and had good light stability under laser Received 21st May 2020, Accepted 23rd July 2020 DOI: 10.1039/d0nr03907a rsc.li/nanoscale

irradiation and a photothermal conversion efficiency of about 24.4%. In addition, this novel nanomaterial achieved good therapeutic effects with less toxicity in vitro. The BZ nanomaterial loaded with GA caused tumor shrinkage as well as disappearance and effectively downregulated Hsp90 expression in tumors in vivo. Moreover, this novel nanomaterial exhibited good biocompatibility and potential for application in low-temperature PTT with excellent tumor destruction efficacy.

Introduction

Hepatocellular carcinoma (HCC) is the fourth most common cancer and ranked as one of the leading causes of cancerrelated deaths globally.1 Chronic HBV and HCV infections are the main causes of HCC and account for 80% of the HCC global cases.2 Treatment of the disease depends on the stage of the HCC. Due to the limited aggressiveness of early-stage HCC, clinical guidelines recommend surgical therapies as the first line treatment.3,4 However, for most patients in the middle and advanced stages, no effective treatment is available as they are often unfit for surgery. These patients mainly

Department of Hepatobiliary and Pancreatic Surgery, Zhongnan Hospital of Wuhan University, Wuhan 430071, China. E-mail: yuanyf1971@whu.edu.cn b Key Laboratory of Artificial Micro- and Nano-Structures of Ministry of Education School of Physics and Technology, Wuhan University, Wuhan 430071, China c Wuhan University Shenzhen Institution, Shenzhen 518057, China d Department of Laboratory Medicine, Zhongnan Hospital of Wuhan University, Wuhan 430071, China † These authors contributed equally.

17064 | Nanoscale, 2020, 12, 17064–17073 receive palliative treatments such as transhepatic arterial chemoembolization (TACE), radiofrequency ablation (RFA), and percutaneous ethanol injection (PEI). However, these treatments have limited efficacy and can exacerbate underlying liver disease partly due to HCC. In addition, portal vein tumor thrombosis (PVTT) has been reported in about 35–50% of patients. This is characterized by a strong negative prognostic factor owing to high malignancy in bloodstream, resulting in limited treatment options and high recurrence risk of HCC.5,6 Therefore, an effective and harmless treatment of hepatocellular carcinoma is urgently required. As promising emergent strategies, photothermal therapy (PTT) and photodynamic therapy are currently under intensive research in preclinical and clinical cancer treatments where high temperature is generated to kill tumor cells.7–9 The damaged tumor cells stimulate the immune system of the patient; this leads to the proliferation and differentiation of immune cells as well as induction of tumor cell necrosis and apoptosis.10,11 These therapies play a role in killing tumors and have good application prospects in the treatment of cancer. Recently, in PTT, photothermal agents (PTAs) have

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Nanoscale been extensively explored under near-infrared (NIR) laser irradiation for tumor hyperthermia ablation.12–14 Most importantly, the wavelength of the NIR light is located in the “biological window”, and NIR light is negligibly absorbed by the blood and soft tissues; this causes its deep penetration in tissues.13,15,16 In addition, most of the PTAs are active in the first NIR (NIR-I) region, and the restricted penetration depth of the laser affects the therapeutic efficacy of these PTAs.17 Alternatively, using a laser with two near-infrared zones (NIR-I (750–1000 nm) and NIR-II (1000–1350 nm)), especially within 1000–1100 nm, deeper penetration and higher maximum allowable exposure (MPE) of PTAs can be achieved as compared to the case of the laser with only the NIR-I bio-window (750–1000 nm). This significantly improves the light-to-heat conversion efficiency of PTAs.18,19 In PTT, to achieve thorough tumor ablation, rigorous photothermal heating to over 50 °C is required to induce complete cell necrosis.20 Furthermore, high-temperature tumor ablation under strong laser irradiation may cause damage to normal organs near the tumor due to laser-induced nonspecific heating.21,22 Moreover, cell damage (e.g. apoptosis) due to heating at lower temperatures (e.g. 45 °C) can be repaired with the aid of heat shock proteins (Hsp).23 However, the delivery of sufficient heat to the internal part of large tumors or deeply located tumors might not be possible, leading to the possible survival of tumor cells after the PTT and their subsequent spread to other organs.24 Therefore, the development of NIR-II photothermal therapy strategies to effectively destroy tumors under low-temperature heating is important for the future clinical transformation of hepatocellular carcinoma treatment methods. The currently available PTAs, such as Au,25–27 Ag,28–30 and 31–33 Pd nanoparticles, have been extensively investigated. However, these metals are rare and expensive, limiting their clinical large-scale application. Specifically, bismuth(Bi), a typical semi-metal element, has aroused great interest from scientific researchers.34–36 Bismuth is a well-known “green metal” that is nontoxic and inexpensive.37 The recent discovery of plasmonic properties that originate from the semimetal-to-semiconductor transition (also called nanoconfinement effects) of Bi at nanoscale has extended the possible applications of Bi-based nanomaterials (traditionally used as thermoelectric materials, catalysts, and sensors) as cancer therapeutic agents in nanomedicine.38,39 Studies have demonstrated that Bi can also be used as a radiosensitizer and contrast agent in computed tomography (CT).40,41 Due to these potential biomedical applications, bismuth nanoparticles can be fabricated as photothermal agents for the effective treatment of HCC. Herein, we designed a novel strategy to synthesize a nanomaterial containing bismuth nanodots embedded in ZIF-8 nanoparticles (BZ). ZIF-8 was used as an excellent reaction container that quickly encapsulated the bismuth nanodots and acted as a small-molecule drug carrier with outstanding drug loading efficiency.42,43 Furthermore, BZ was loaded with gambogic acid (GBZ), a natural inhibitor of heat-shock protein 90 (Hsp90), for NIR-II low-temperature photothermal therapy.44 Since Hsp90 is a key protein that induces thermoresistance in

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Paper cells under hyperthermia,45 the inhibition of Hsp90 by GA delivered using BZ effectively induced the apoptosis of cancer cells under low-temperature heating (e.g. 43 °C). To the best of our knowledge, to date, no study has been reported on the photothermal properties of Bi nanoparticles and GA in hepatocellular carcinoma treatment and the further development of Bi nanoparticles and GA for biomedical applications. The composite nanomaterials prepared herein successfully expanded the application of Bi in the treatment of hepatocellular carcinoma and provided more opportunities for the successful clinical application of PTT.

2. Results and discussion 2. 1. Characterization of GBZ At first, we prepared ZIF-8 nanoparticles coated with bismuth nanodots via a simple reduction method and then loaded gambogic acid onto them through physical mixing. The entire synthesis step did not require complicated conditions, and the products were synthesized in large quantities. Subsequently, we characterized the products using electron microscopy. Our results revealed that the particle size of GBZ was approximately 100 nm. The small size of GBZ was due to the short reaction time and fast stirring speed. In addition, there were apparent black nanodots in GBZ; this indicated that the bismuth nanodots were successfully fixed on ZIF-8 (Fig. 1A). Scanning electron microscopy results also indicated that the nanoparticles were synthesized in large quantities (Fig. 1C). To demonstrate that the bismuth nanoparticles were successfully immobilized onto ZIF-8, we performed element analysis (Fig. 1B) and energy spectrum analysis (Fig. 1D). Our analysis results revealed that bismuth was present in ZIF-8. The loading content of gambogic acid (LC) was calculated to be 31.4%. XRD (Fig. 1E) results showed that the synthesized GBZ atlas match the ZIF-8 and Bi standard atlas. The hydrodynamic diameter of the GBZ nanoparticles was approximately 100 nm (Fig. 1F). Overall, GBZ was successfully synthesized in large quantities and was used in subsequent experiments. 2.2. In vitro photothermal properties of the GBZ nanoparticles We verified the photothermal conversion efficiency of GBZ in vitro. The UV-vis-NIR absorption spectrum (Fig. 2A) indicated that gambogic acid has a relatively strong absorption peak near 240 nm, whereas GBZ has a strong absorption peak at 240 nm, which indicated that the drug was successfully loaded onto the nanoparticles. Moreover, we found that GBZ has a relatively optimal absorption in the near-infrared second region. The ZIF-8, BZ, and GBZ groups were irradiated using a 1064 nm laser for 1 min, 2 min, and 3 min, respectively. Consequently, the infrared thermal phase diagram (Fig. 2B) revealed that the BZ and GBZ groups attained a higher temperature of approximately 40 °C in a short period of time. The infrared camera detected the temperature changes of the GBZ solution at different concentrations (50, 100, and 200 μg mL−1)

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Fig. 1 (A) i. High-magnification transmission electron microscopy image of ZIF-8 nanoparticles, scale bar: 30 nm; ii. high-magnification transmission electron microscopy image of GBZ nanoparticles, scale bar: 30 nm; iii. low-magnification transmission electron microscopy image of GBZ nanoparticles, scale bar: 100 nm; (B) elemental mapping images of Zn and Bi, scale bar: 1 μm; (C) scanning electron microscopy image of the GBZ nanoparticles, scale bar: 150 nm; (D) energy spectrum analysis of BZ; (E) powder XRD pattern of BZ; and (F) hydrodynamic diameter of the GBZ nanoparticles measured via DLS.

Fig. 2 (A) Absorbance spectra of GA, ZIF-8, BZ, and GBZ. (B) The infrared thermal images of (i) ZIF-8, (ii) BZ, and (iii) GBZ nanoparticles (containing 100 μg mL−1 BZ) irradiated for 1–3 min (1064 nm, 1 W cm−2); (C) temperature rise curve of the GBZ solution at different concentrations (50, 100, and 200 μg mL−1) irradiated by a 1064 nm laser at 1 W cm−2 for 5 min; (D) the photothermal response of a 200 μg mL−1 GBZ nanoparticle aqueous solution analyzed using a NIR laser (1064 nm, 1 W cm−2); then, the laser was turned off, and the process was repeated three times; (E) the photothermal response of an aqueous solution containing 200 μg mL−1 GBZ nanoparticles measured using a NIR laser (1064 nm, 1 W cm−2), and then, the laser was shut off; and (F) linear time data versus −ln θ obtained from the cooling period shown in (E).

and water under 1064 nm laser irradiation (Fig. 2C). With an increase in the nanoparticle concentration and irradiation time, the trend of the curve increased significantly. In the case 17066 | Nanoscale, 2020, 12, 17064–17073

of the GBZ solution at a concentration of 200 μg mL−1, the temperature increased to approximately 42 °C after 150 s, implying that the GBZ solution had profound light stability This journal is © The Royal Society of Chemistry 2020

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Nanoscale under laser irradiation. To confirm that the GBZ solution had profound photothermal cycling stability and high photothermal conversion efficiency (Fig. 2D), the 200 μg mL−1 GBZ solution was subjected to heating and cooling cycles, and it remained stable after three cycles of heating and cooling. Fig. 2E shows the recorded temperature change of the GBZ solution under continuous irradiation of a 1064 nm laser. Based on the experimental data and the method reported in previous studies (Fig. 2E), the photothermal conversion efficiency of GBZ was approximately 24.4% (Fig. 2F), which was lower than that of the recently reported bismuth-based nanomaterials (30%),34 but was higher than those of some photothermal agents such as Au nanodots (21%)46 and Cu2−xSe (22%).47 Overall, these data indicated that GBZ is a profound nanomaterial for photothermal treatment. 2.3.

Verification of the GBZ drug release characteristics

Next, we verified the GBZ drug release characteristics. Our findings revealed that under no-light conditions, the ZIF-8 nanomaterial had a profound pH response, and the GBZ drug release rate was markedly faster than that under neutral and acidic conditions (Fig. 3A). After light exposure, faster drug release rates were observed because of the increase in the temperature of the nanomaterial. These results demonstrated that the BZ nanomaterials are suitable for drug loading and release, which are crucial for PTT. 2.4.

Based on the profound photothermal conversion efficiency of GBZ, we further verified its ability in apoptotic cancer cells in vitro. The CCK-8 experiment (Fig. 3B) validated the toxicity

Paper of Huh7 cells in each group under light conditions. With an increase in material concentration under light, the rate of cell survival further decreased. GBZ hindered cell growth at approximately 85% when compared with the case of the PBS group. The inhibitory effect of BZ on cell growth under light was about 60%. Moreover, GA had some anti-tumor ability. In the absence of light irradiation, whether the nanomaterials have an apoptotic effect on normal cells or tumor cells is unclear. We further investigated the toxicity of BZ in normal liver cells, immune cells, and tumor cells. Consequently, all types of cells had higher survival rates (over 90%) at each concentration of BZ (Fig. 3C). Therefore, the BZ nanomaterials are less toxic and safe for use in in vivo experiments. To further study the efficacy of GBZ in in vitro treatment, we used 35 mm cell culture dishes to culture Huh-7 cells to 1 × 105 cells per 1 mL followed by the addition of PBS (50 μg mL−1) and BZ solution (70 μg mL−1), respectively. A GA solution (30 μg mL−1) and GBZ solution (containing 70 μg mL−1 BZ and 30 μg mL−1 GA) were co-cultured with Huh-7 cells for an additional 12 h and then irradiated with a 1064 nm laser for 3 min. Then, we stained the cells using fluorescein diacetate (FDA) and propidium iodide (PI) for 5 min. Finally, the fluorescence images were obtained using a fluorescence microscope (Olympus, Japan), as shown in Fig. 3D. Our findings indicated that almost all the Huh-7 cells in the PBS group emitted green fluorescence, implying that an insignificant number of Huh-7 cells were killed. Part of the Huh-7 cells in the BZ group and GA group emitted red fluorescence; in the GBZ group, almost all the Huh-7 cells emitted red fluorescence, implying that all the Huh-7 cells were dead. Overall, these results showed that the combination of BZ with GA has

Fig. 3 (A) NIR-triggered (1 W cm−2) release of GA from GBZ at a pH of 7.4 and 5.5; (B) in vitro cytotoxicity of different nanomaterials against Huh-7 cells in the presence of light irradiation (1064 nm, 1 W cm−2, 5 min), ***p < 0.01; (C) in vitro cytotoxicity of BZ against RAW264.7, L02, MCF-7, and Huh-7 cell lines in the absence of light irradiation; (D) fluorescence images of the Huh-7 cells co-stained with FDA (live cells, green) and PI (dead cells, red) upon the addition of different nanomaterials under irradiation (1064 nm, 1 W cm−2, 3 min). (i) PBS, (ii) GA, (iii) BZ, and (iv) GBZ; scale bar: 50 μm; (E) western blot images: Hsp90 expression levels with GADPH as an internal reference for the cell lysates of Huh-7 cells after various treatments.

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Paper optimal therapeutic effects in vitro. We examined the Hsp90 expression in Huh-7 cells under different experimental treatments via western blot assays (Fig. 3E) using glyceraldehyde 3-phosphate dehydrogenase (GAPDH) as a loading control. The results indicated that the Huh-7 cells under hyperthermia treatment had higher levels of Hsp90 at 43 °C when compared with the case of the untreated control cells. The treatment of the cells with GA-loaded nanoparticles effectively inhibited this elevated expression of Hsp90.

Currently, photothermal therapy is the most extensively researched therapy, and in vivo photothermal efficacy is the most direct validation approach used for assessing suitable nanoparticles for photothermal therapy.48–50 Therefore, we validated the photothermal efficacy of GBZ nanomaterials in vivo. We used an infrared thermal imaging camera to monitor the photothermal effect of these nanomaterials in the body by concurrently plotting the temperature changes at the site of the tumor. Consequently, we found that the temperature at the site of the tumor is positively associated with the irradiation period after the injection of the Bi nanodots.51 However, we did not observe any evident temperature changes in the case of the control mice (Fig. 4A). In Fig. 4B, the temperature in the control group is almost constant. The temperature in the tumor microenvironment of the BZ and GBZ groups increased by approximately 10 °C. This indicated that the nanoparticles have an optimal photothermal conversion efficiency and can be heated to a temperature exceeding the tolerance temperature of the cells (42 °C). Our findings show

Nanoscale that the Bi nanodots can potentially be utilized in the realtime monitoring of thermal dynamics in PTT. We measured the tumor volume and body weight of each group in this study every two days to assess the anti-tumor effect of BZ following the photothermal treatment of tumor sites in mice. Our results revealed rapid tumor growth in the PBS group, and the tumor expanded from about 200 mm3 to 780 mm3 (Fig. 4C and D). Tumor growth in the BZ group was substantially slower than that in the PBS group. Moreover, the tumors in the GBZ group were gradually shrinking or even disappearing. There was no evident variation in the body weight in all the groups under different treatments with prolonged irradiation time, indicating no noticeable systemic toxicity of the proposed photothermal molecule. The mean weights of the excised tumors are shown in Fig. 4E. Notably, the weights and volumes of the tumors exhibited a similar trend. We randomly selected one mouse per group for PET-CT. Consequently, the metabolism at the tumor site was strongest in the case of the PBS group and weakest in the case of the GBZ group (Fig. 5A). Interestingly, the tumor metabolism of the laser-irradiated GBZ group was higher than that of the group without laser irradiation. This could be attributed to individual differences in mice. These results confirmed that GBZ has significant potential as an ideal PTT agent for the in vivo photothermal ablation of tumors. Furthermore, we harvested the tumor tissues in all the groups for histological examinations via H&E, Ki-67, and TUNEL staining. Moreover, we harvested the tumors for immunefluorescence staining to assay the expression levels of Hsp90. The H&E staining results showed that the tumor tissue of the mice treated with both the GBZ injection and laser

Fig. 4 (A) Infrared thermal images and (B) temperature curves of the tumor-bearing mice intravenously injected with PBS (control), BZ, and GBZ, and then irradiated with an 808 nm NIR laser (808 nm, 1 W cm−2) for 5 min; (C) tumor volume of the mice in different groups after various treatments; (D) tumor weight of the mice in different groups after various treatments, ***p < 0.01; and (E) body weight of the mice in different groups after various treatments.

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Fig. 5 (A) In vivo PET-CT and the responding degree of metabolism of mice after intravenous injection of different materials; (B) H&E, Ki-67, and TUNEL staining images of the tumors dissected from different groups, scale bar: 200 μm; (C) HSP immunofluorescence staining image, scale bar: 200 μm; and (D) quantified immunofluorescence Hsp90 expression levels, ***p < 0.01.

irradiation was remarkably damaged (Fig. 5B) followed by the tumor tissue of the mice belonging to the BZ-laser group; however, the residual tumor tissues in the rest of the groups had no evident damage. The TUNEL staining results revealed a similar trend as the H&E staining results, and the tumor cells of the GBZ-laser group showed significant apoptosis. The Ki-67 staining results indicated the proliferation of tumor cells as expected; however, the proliferation of tumor cells in the GBZlaser group was markedly inhibited. We separated the tumors dissected from the various treatment groups for immunofluorescence staining to determine the expression level of Hsp90 in the tumors. The expression of Hsp90 was up-modulated in the tumor after the PTT treatment; this demonstrates that the PTTinduced heating stress enhances the Hsp90 expression in cancer cells in vivo (Fig. 5C). Compared with the expression level of Hsp90 in the GBZ group, the expression level of Hsp90 in the BZ group was almost twice higher (Fig. 5D), which was suppressed by treatment with the GA-loaded nanoparticles. Our results collectively indicated that the GBZ treatment downmodulates the expression of Hsp90 within tumors, resulting in a remarkably reduced thermoresistance of cancer cells during the PTT. This significantly promotes the apoptosis of cancer cells and allows low-temperature PTT with profound tumor destruction efficacy.

Phosphate buffer solution (PBS) and Dulbecco’s modified Eagle’s medium (DMEM, Hyclone, high glucose) were obtained from Thermo-Fisher (Waltham, MA, USA). 1, 2-Distearoyl-sn- This journal is © The Royal Society of Chemistry 2020

glycero-3-phosphoethanolamine-N-[Cy5 ( poly-ethylene glycol)2000] (ammonium salt) (DSPE-PEG-Cy5) was acquired from Avanti Polar Lipids (USA). All aqueous solutions were prepared using deionized (DI) water purified using an experimental water purification system (Direct-Q3, Millipore, USA). Analytical-grade bismuth nitrate pentahydrate (99%) (Bi (NO3)3·5H2O), gambogic acid (GA), zinc nitrate hexahydrate (Zn(NO3)2·6H2O), sodium borohydride (NaBH4), and 2-methylimidazole (MeIm) were purchased from Aladdin-Reagent (Shanghai, China). All the chemicals were of analytical grade and were used without further purification. 3.2.

The human hepatocellular carcinoma cell lines Huh-7, L02, and MCF-7 were cultured in Dulbecco’s modified Eagle’s medium (DMEM) supplemented with 10% bovine serum (FBS) at 37 °C under a humidified 5% CO2 atmosphere. The mouse leukocyte cell line RAW264.7 was cultured in a medium supplemented with 10% FBS at 37 °C and 5% CO2. 3.3. Preparation of Bi nanodot-encapsulated ZIF-8 nanoparticles (BZ) Typically, a mixture of Zn (NO3)2·6H2O (100 mg), Bi (NO3)3·5H2O (70 mg), and 2-methylimidazole (1.94 g) was dissolved in 10 mL of deionized (DI) water. The resulting mixture was stirred for 5 min. Thereafter, 50 mg NaBH4 in 1 mL DI water was quickly added to the abovementioned mixture followed by stirring for 1 min. After the reaction, the products were obtained by centrifugation, washed three times with deionized water, and then vacuum-dried. The content of bismuth was quantified via ICP-AES.

Open Access Article. Published on 05 August 2020. Downloaded on 5/31/2026 1:58:21 AM. This article is licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported Licence. 3.4. Nanoscale Preparation of GA-loaded BZ (GBZ) nanoparticles

The GBZ nanoparticles were prepared as follows: 1 mL GA solution (1 mg mL−1 dispersed in DMSO) was slowly added to 1 mL DMSO containing 1 mg BZ followed by stirring at room temperature for 30 min. The resulting solution was then centrifuged at 8000 rpm for 10 min followed by washing with distilled water. The loading content (LC) was calculated using the following formula: LC = (weight of feeding drug − weight of redundant drug/weight of drug-loaded nanoparticles) × 100%.52 3.5.

Characterization

The crystal structure and phase purity of the product were investigated by powder X-ray diffraction (XRD) using an X-ray diffractometer (D8 Advance, AXS Instruments, Germany). Transmission electron microscopy (TEM) images were obtained by Philips Tecnai-12 (the Netherlands) operated at 120 kV. The composition of the samples was studied using a field-emission scanning electron microscope (FE-SEM, S-4800, Hitachi) equipped with an energy-dispersive X-ray (EDX) spectrometer. UV-vis-NIR spectra were acquired using a UV-3600 spectrophotometer. Hydrodynamic diameters of the nanoparticles suspended in 1× PBS were measured using dynamic light scattering (DLS) (Nano-Zen 3600, Malvern Instruments, UK). 3.6.

A 1064 nm NIR laser (Changchun New Industries Tech. Co., Ltd, China) was used to stimulate BZ at different concentrations (0, 50, 20, 100, and 200 μg mL−1) in the PBS solution. Photothermal images of the BZ nanoparticle-based suspensions were obtained every 30 s during laser irradiation using an infrared thermal imaging system. The NIR laser source was equipped with a 7 mm2 round spot laser module with adjustable power. The photothermal conversion efficiency was calculated using the following equation:41 η¼

where h is the heat transfer coefficient, S is the surface of the container, and Tmax and Tsurr are the equilibrium temperature and ambient temperature, respectively. Q0 is the heat associated with the light absorbance of the solvent, Aλ is the absorbance of the BZ nanoparticles at 1064 nm, and I is the laser power density. According to this equation, the η value of the BZ nanoparticles was determined to be about 24.4%. 3.7.

Drug release

The release of GA due to either pH change or NIR-light irradiation was separately studied. To investigate the timedependent cumulative release profiles of GA-loaded GBZ at various pH values, 5 mg of NPs was dispersed in 20 mL of buffer solution ( pH 7.4 and 5.5, respectively) at 37 °C. The resulting mixture was continuously stirred. At each time point, 1 mL of release medium was sampled, and the concentration

17070 | Nanoscale, 2020, 12, 17064–17073 of GA released into the solution was determined via UV-vis spectrophotometry. Next, the sample was returned to the original release system. Subsequently, the release profiles of DOX under 1064 nm laser irradiation at various pH values were also acquired, and the GA release was measured by UV-vis spectrophotometry as described above. 3.8.

In vitro photothermal ability of GBZ nanoparticles

3.8.1 Live-dead cell staining. The Huh-7 cells were seeded into 6-well plates. After incubation for 24 h, PBS, BZ, GA, and GBZ were separately added followed by incubation for another 24 h. Thereafter, the cells were exposed to laser irradiation (808 nm, 1 W cm−2) for 5 min and co-stained with 1 mg mL−1 propidium iodide (PI) and 5 mg mL−1 fluorescein diacetate (FDA) for 15 min before being washed several times with PBS. The fluorescence microscopy images were obtained using an Olympus IX81 microscope. 3.8.2 CCK-8 and western blot assays. The photothermal ablation cytotoxicity of each nanoparticle group was detected by the Cell Counting kit-8 (CCK-8, Dojindo, Japan) assay. A total of 8 × 103 Huh-7 cells per well were seeded into 96-well plates and cultured. After 24 h, PBS, BZ, GA, and GBZ were separately added and co-cultured with the Huh-7 cells for 0 h, 24 h, and 48 h. Thereafter, the cells were exposed to laser irradiation (808 nm, 1 W cm−2) for 5 min at different times. The CCK-8 solution was added as per the guidelines followed by incubation for another 2 h. The cytotoxicity was calculated by dividing the optical density (OD) values of the treated groups (T ) by the OD values of the control group (C) (T/C × 100, %). Proteins were extracted from the cells to detect the expression level of heat shock protein 90 (Hsp90). 3.8.3 Biocompatibility of the GBZ nanoparticles. We estimated the biocompatibility of the GBZ nanoparticles via the abovementioned CCK-8 assay. The L02, MCF-7, RAW 264.7, and Huh 7 cell lines were seeded into 96-well plates and cultured. After 24 h, GBZ was separately added and co-cultured with these cell lines for 12 h, 24 h, and 48 h. The cytotoxicity was calculated by dividing the optical density (OD) values of the treated groups (T ) by the OD values of the control group (C) (T/C × 100, %). 3.9.

Male BALB/c nude mice were obtained from the Chinese Academy of Medical Science (Beijing, China). The study was performed in strict accordance with the National Regulations for the Administration of Affairs Concerning Experimental Animals and was approved by the Center for Animal Experiments/Animal Biosafety Level 3 Laboratory of Wuhan University. A total of 5 × 106 Huh-7 cells were subcutaneously injected into the flanks of 4-week old male BALB/c-nu mice. Treatments started when the tumor size reached ∼200 mm3. The mice20 were randomly divided into 4 groups: one group was intravenously injected with 200 μL PBS, another group was intravenously injected with BZ, and the remaining two groups were intravenously injected with GBZ. After 24 h, the PBS, BZ, and GBZ group mice bearing tumors were anesthetized, and

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Nanoscale the entire tumors were exposed to laser irradiation (808 nm, 1 W cm−2) for 5 min. The other GBZ group was not exposed to the laser irradiation. During laser irradiation, an infrared thermal imaging camera was used to monitor the temperature changes at the tumor sites. The changes in the tumor volume and body weight post-irradiation were measured daily. The tumor volume V (mm3) was calculated according to the formula: Volume = (tumor length) × (tumor width)2/2. After 14 days of injection, one mouse was selected from each group for PET examination, and other mice were sacrificed. The tumors were then extracted for H&E, Ki-67, and terminal deoxynucleotidyl transferase dUTP nick end labeling (TUNEL) staining. Meanwhile, tumors were also extracted for immunofluorescence staining to detect the expression level of Hsp90. 3.10. Statistical analyses The data are presented as mean values ± SD, and each value represents the mean of the results of at least three repetitive experiments in each group. A non-parametric test was performed using GraphPad Prism 7.0 to assess the significance of the difference between two groups, ***p < 0.01.

In summary, herein, we developed an easily synthesized BZ nanomaterial for use in nanomedicine delivery. The synthetic method improves the efficiency of the synthesis process, showing a broad application prospect. The synthesized nanomaterial had good light absorption potential and photothermal cycling stability in the near-infrared second region and exhibited profound biocompatibility. GA, a natural inhibitor of Hsp90, was then loaded onto the synthesized BZ nanomaterials with high efficiency. Owing to the GA-induced downmodulation of Hsp90 to overcome the thermoresistance of cancer cells, highly effective in vivo apoptosis of tumors was realized using GBZ in the low-temperature PTT at 43 °C.

Conflicts of interest The authors declare no conflict of interest.

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一种Bi@ZIF-8复合纳米材料的快速合成及其作为近红外二区(NIR-II)光热剂用于肝细胞癌低温光热治疗的研究 引用本文:Nanoscale, 2020, 12, 17064

作者:李景华†a,朱道明†b,马伟杰a,杨洋b,王刚刚a,吴晓玲a,王坤磊a,陈怡然a,王福兵*d,刘卫*b,c,袁玉峰*a

肝细胞癌是全球癌症相关死亡原因的第四大常见恶性肿瘤。先进的纳米材料已成为肝癌治疗的有效手段,如光热治疗(PTT)。然而,在NIR-I生物窗口激活的光热剂(PTAs)穿透深度有限,以及热休克蛋白(Hsp)介导的热抗性,限制了PTT在肝细胞癌(HCC)中的治疗效果。本文中,我们通过简单的一步还原法制备了Bi@ZIF-8(BZ)纳米材料,并通过物理混合高效负载了Hsp90的天然抑制剂——藤黄酸(GA)。分别研究了该纳米材料的表征及由pH变化或近红外光照引发的GA释放行为。计算了光热转换效率,并开展了体内外治疗研究。该纳米材料在酸性条件下升温时表现出显著增强的药物释放速率,且在激光照射下具有良好的光稳定性,光热转换效率约为24.4%。此外,该新型纳米材料在体外实验中展现出良好的治疗效果和较低的毒性。负载GA的BZ纳米材料在体内可导致肿瘤缩小甚至消失,并有效下调肿瘤中Hsp90的表达。同时,该材料具有良好的生物相容性,在低温光热治疗中展现出优异的肿瘤消融潜力。

引言

肝细胞癌(HCC)是全球最常见的第四大癌症,也是癌症相关死亡的主要原因之一。1 慢性乙型肝炎病毒(HBV)和丙型肝炎病毒(HCV)感染是HCC的主要病因,占全球HCC病例的80%。2 该病的治疗取决于HCC的分期。由于早期HCC侵袭性较低,临床指南推荐手术疗法作为一线治疗方案。3,4 然而,对于大多数中晚期患者,由于常不适合手术,缺乏有效的治疗手段。这些患者主要接受姑息性治疗,如经肝动脉化疗栓塞术(TACE)、射频消融术(RFA)和经皮乙醇注射(PEI)。然而,这些治疗方法疗效有限,且可能加重潜在的肝脏疾病,部分原因在于HCC本身。此外,约35–50%的患者伴有门静脉癌栓(PVTT),这是一个强烈的负面预后因素,因其在血流中具有高度恶性,导致治疗选择有限且HCC复发风险高。5,6 因此,亟需一种有效且无害的肝细胞癌治疗方法。

作为有前景的新兴策略,光热治疗(PTT)和光动力治疗目前正处于临床前和临床癌症治疗研究的热点,其通过产生高温来杀伤肿瘤细胞。7–9 受损的肿瘤细胞可刺激患者的免疫系统,导致免疫细胞增殖与分化,并诱导肿瘤细胞坏死和凋亡。10,11 这些疗法在杀伤肿瘤方面发挥重要作用,在癌症治疗中具有良好的应用前景。近年来,在PTT中,光热剂(PTAs)在近红外(NIR)激光照射下用于肿瘤热消融的研究已被广泛探索。12–14 最重要的是,NIR光的波长位于“生物窗口”,血液和软组织对其吸收极弱,因此其在组织中具有深层穿透能力。13,15,16 此外,大多数PTAs在第一近红外区(NIR-I)有活性,激光穿透深度受限影响了这些PTAs的治疗效果。17 相比之下,使用包含两个近红外区域(NIR-I:750–1000 nm;NIR-II:1000–1350 nm)的激光,特别是在1000–1100 nm范围内,可实现比仅使用NIR-I生物窗口(750–1000 nm)更深的穿透深度和更高的最大允许曝光量(MPE),从而显著提高PTAs的光热转换效率。18,19 在PTT中,为实现彻底肿瘤消融,通常需要严格的光热加热至超过50 °C以诱导完全细胞坏死。20 此外,在强激光照射下的高温肿瘤消融可能因激光诱导的非特异性加热而对肿瘤附近正常器官造成损伤。21,22 而且,在较低温度(如45 °C)下引起的细胞损伤(如凋亡)可在热休克蛋白(Hsp)的辅助下被修复。23 然而,对于较大或位置较深的肿瘤,可能无法向其内部传递足够热量,导致PTT后肿瘤细胞可能存活并扩散至其他器官。24 因此,开发在低温加热下有效破坏肿瘤的NIR-II光热治疗策略,对于未来肝细胞癌治疗方法的临床转化具有重要意义。

目前可用的PTAs,如金(Au)、25–27 银(Ag)、28–30 和钯(Pd)31–33 纳米粒子,已被广泛研究。然而,这些金属稀有且昂贵,限制了其临床大规模应用。特别地,铋(Bi)作为一种典型的类金属元素,已引起科研人员的极大兴趣。34–36 铋是一种众所周知的“绿色金属”,无毒且价格低廉。37 近年来,纳米尺度下铋从类金属到半导体的转变(也称为纳米限域效应)所引发的等离激元特性的发现,拓展了基于铋的纳米材料(传统上用作热电材料、催化剂和传感器)在纳米医学中作为癌症治疗剂的应用。38,39 研究表明,铋还可作为放射增敏剂和计算机断层扫描(CT)的对比剂。40,41 由于这些潜在的生物医学应用,铋纳米粒子可被制备为光热剂,用于HCC的有效治疗。

在此,我们设计了一种新策略,用于合成一种包含嵌入ZIF-8纳米粒子中的铋纳米点的纳米材料(BZ)。ZIF-8被用作优异的反应容器,可快速封装铋纳米点,并作为小分子药物载体,具有出色的药物负载效率。42,43 此外,将BZ负载藤黄酸(GA)——一种热休克蛋白90(Hsp90)的天然抑制剂——用于NIR-II低温光热治疗。44 由于Hsp90是细胞在高温下诱导热抗性的关键蛋白,45 通过BZ递送的GA抑制Hsp90,可在低温加热(如43 °C)下有效诱导癌细胞凋亡。

据我们所知,迄今为止,尚无关于Bi纳米粒子和GA在肝细胞癌治疗中的光热特性及其进一步生物医学应用开发的研究报道。本文所制备的复合纳米材料成功拓展了Bi在肝细胞癌治疗中的应用,并为PTT的成功临床转化提供了更多机遇。

2. 结果与讨论 2.1. GBZ的表征 首先,我们通过简单的还原法制备了包覆铋纳米点的ZIF-8纳米粒子,然后通过物理混合将藤黄酸负载其上。整个合成步骤无需复杂条件,且产物可大量合成。随后,我们利用电子显微镜对产物进行表征。结果显示,GBZ的粒径约为100 nm。GBZ的小尺寸归因于较短的反应时间和快速的搅拌速度。此外,GBZ中存在明显的黑色纳米点,表明铋纳米点已成功固定在ZIF-8上(图1A)。扫描电子显微镜结果也表明纳米粒子已大量合成(图1C)。为证明铋纳米粒子已成功固定于ZIF-8上,我们进行了元素分析(图1B)和能谱分析(图1D)。分析结果表明,ZIF-8中存在铋元素。藤黄酸(GA)的载药量(LC)计算为31.4%。XRD结果(图1E)显示,所合成的GBZ图谱与ZIF-8和Bi的标准图谱匹配。GBZ纳米粒子的水合粒径约为100 nm(图1F)。总体而言,GBZ已成功大量合成,并用于后续实验。

2.2. GBZ纳米粒子的体外光热性能 我们在体外验证了GBZ的光热转换效率。紫外-可见-近红外(UV-vis-NIR)吸收光谱(图2A)显示,藤黄酸在240 nm附近有较强吸收峰,而GBZ在240 nm处有强吸收峰,表明药物已成功负载于纳米粒子上。此外,我们发现GBZ在近红外二区具有较优的吸收。分别用1064 nm激光照射ZIF-8、BZ和GBZ组1、2、3分钟。红外热成像图(图2B)显示,BZ和GBZ组在短时间内达到约40 °C的较高温度。红外相机检测了不同浓度(50、100和200 μg mL−1)GBZ溶液在1064 nm激光照射下的温度变化(图2C)。随着纳米粒子浓度和照射时间增加,曲线上升趋势显著。对于浓度为200 μg mL−1的GBZ溶液,150秒后温度升至约42 °C,表明GBZ溶液在激光照射下具有优异的光稳定性。为确认GBZ溶液具有优异的光热循环稳定性和高光热转换效率(图2D),对200 μg mL−1 GBZ溶液进行加热-冷却循环测试,经过三次循环后仍保持稳定。图2E记录了GBZ溶液在1064 nm激光持续照射下的温度变化。根据实验数据和先前研究报道的方法(图2E),GBZ的光热转换效率约为24.4%(图2F),低于近期报道的铋基纳米材料(30%),34 但高于某些光热剂,如金纳米点(21%)46 和Cu2−xSe(22%)。47 总体而言,这些数据表明GBZ是一种优异的光热治疗纳米材料。

2.3. GBZ药物释放特性的验证 接下来,我们验证了GBZ的药物释放特性。结果表明,在无光照条件下,ZIF-8纳米材料具有显著的pH响应性,GBZ在酸性条件下的药物释放速率明显快于中性条件(图3A)。光照后,由于纳米材料温度升高,药物释放速率加快。这些结果表明,BZ纳米材料适用于药物负载与释放,这对PTT至关重要。

2.4. GBZ纳米粒子的体外光热能力 基于GBZ优异的光热转换效率,我们进一步验证了其体外诱导癌细胞凋亡的能力。CCK-8实验(图3B)验证了光照条件下各组Huh7细胞的毒性。随着光照下材料浓度增加,细胞存活率进一步下降。与PBS组相比,GBZ在约85%浓度时即抑制细胞生长。光照下BZ对细胞生长的抑制率约为60%。此外,GA具有一定的抗肿瘤能力。在无光照条件下,纳米材料对正常细胞或肿瘤细胞的凋亡作用尚不明确。我们进一步研究了BZ对正常肝细胞、免疫细胞和肿瘤细胞的毒性。结果显示,在所有BZ浓度下,各类细胞的存活率均较高(超过90%)(图3C)。因此,BZ纳米材料毒性较低,可用于体内实验。

为进一步研究GBZ在体外治疗中的效果,我们使用35 mm细胞培养皿培养Huh-7细胞至每毫升1×10^5个,分别加入PBS(50 μg mL−1)和BZ溶液(70 μg mL−1)。将GA溶液(30 μg mL−1)和GBZ溶液(含70 μg mL−1 BZ和30 μg mL−1 GA)与Huh-7细胞共培养12小时后,用1064 nm激光照射3分钟。随后,用荧光素二乙酸酯(FDA)和碘化丙啶(PI)对细胞染色5分钟。最后,使用荧光显微镜(日本奥林巴斯)获取荧光图像,如图3D所示。结果表明,PBS组几乎所有Huh-7细胞均发出绿色荧光,表明极少细胞死亡。BZ组和GA组部分Huh-7细胞发出红色荧光;GBZ组几乎所有Huh-7细胞均发出红色荧光,表明所有细胞均已死亡。总体而言,这些结果表明BZ与GA联用在体外具有最佳治疗效果。

我们通过蛋白质印迹实验(图3E)检测了不同实验处理下Huh-7细胞中Hsp90的表达水平,以甘油醛-3-磷酸脱氢酶(GAPDH)为内参。结果表明,与未处理的对照组相比,在43 °C高温处理的Huh-7细胞中Hsp90水平升高。用负载GA的纳米粒子处理细胞可有效抑制Hsp90的表达上调。

2.5. GBZ纳米粒子的体内光热效果 目前,光热治疗是研究最广泛的疗法,体内光热效果是评估适用于PTT的纳米颗粒的最直接验证方法。48–50 因此,我们验证了GBZ纳米材料在体内的光热效果。我们使用红外热成像仪监测这些纳米材料在体内的光热效应,同时绘制肿瘤部位的温度变化曲线。结果发现,注射Bi纳米点后,肿瘤部位的温度与照射时间呈正相关。51 然而,对照组小鼠未观察到明显的温度变化(图4A)。图4B显示,对照组温度几乎不变,而BZ组和GBZ组肿瘤微环境的温度升高了约10 °C。这表明纳米粒子具有优异的光热转换效率,可加热至超过细胞耐受温度(42 °C)。我们的研究结果表明,Bi纳米点有望用于PTT中热动力学的实时监测。

我们每两天测量各组小鼠的肿瘤体积和体重,以评估BZ在小鼠肿瘤部位光热治疗后的抗肿瘤效果。结果显示,PBS组肿瘤生长迅速,从约200 mm³增长至780 mm³(图4C和D)。BZ组的肿瘤生长速度显著慢于PBS组。此外,GBZ组的肿瘤逐渐缩小甚至消失。在不同处理组中,随着照射时间延长,体重未见明显变化,表明所提出的光热分子无明显系统性毒性。切除肿瘤的平均重量如图4E所示。值得注意的是,肿瘤的重量和体积呈现相似趋势。我们每组随机选取一只小鼠进行PET-CT检查。结果显示,PBS组的肿瘤代谢最强,GBZ组最弱(图5A)。有趣的是,经激光照射的GBZ组的肿瘤代谢高于未照射组,这可能归因于小鼠个体差异。这些结果证实,GBZ作为理想的PTT剂,在体内肿瘤光热消融方面具有巨大潜力。

此外,我们采集各组肿瘤组织进行H&E、Ki-67和TUNEL染色,并进行免疫荧光染色以检测Hsp90的表达水平。H&E染色结果显示,接受GBZ注射并激光照射的小鼠肿瘤组织损伤最为严重(图5B),其次为BZ激光组,其余组的残留肿瘤组织未见明显损伤。TUNEL染色结果与H&E染色趋势一致,GBZ激光组的肿瘤细胞出现显著凋亡。Ki-67染色结果显示肿瘤细胞增殖受到预期抑制,且GBZ激光组的肿瘤细胞增殖被显著抑制。我们将不同治疗组切除的肿瘤分离后进行免疫荧光染色,以检测肿瘤中Hsp90的表达水平。PTT治疗后,肿瘤中Hsp90表达上调,表明PTT诱导的热应激增强了癌细胞中Hsp90的表达(图5C)。与GBZ组相比,BZ组的Hsp90表达水平几乎是其两倍(图5D),而负载GA的纳米粒子治疗可抑制该表达。我们的研究结果表明,GBZ治疗可下调肿瘤内Hsp90的表达,从而显著降低癌细胞在PTT过程中的热抗性,促进癌细胞凋亡,实现具有优异肿瘤消融效果的低温PTT。

3. 实验部分 3.1. 试剂 磷酸盐缓冲液(PBS)和Dulbecco改良Eagle培养基(DMEM,Hyclone,高糖)购自Thermo-Fisher(美国马萨诸塞州沃尔瑟姆)。1,2-二硬脂酰-sn-甘油-3-磷酸乙醇胺-N-[Cy5(聚乙二醇)2000](铵盐)(DSPE-PEG-Cy5)购自Avanti Polar Lipids(美国)。所有水溶液均使用实验用水纯化系统(Direct-Q3,Millipore,美国)纯化的去离子水(DI)配制。分析级五水合硝酸铋(99%)(Bi(NO3)3·5H2O)、藤黄酸(GA)、六水合硝酸锌(Zn(NO3)2·6H2O)、硼氢化钠(NaBH4)和2-甲基咪唑(MeIm)均购自阿拉丁试剂(中国上海)。所有化学试剂均为分析纯,未经进一步纯化直接使用。

3.2. 细胞培养 人肝细胞癌细胞系Huh-7、L02和MCF-7在含10%胎牛血清(FBS)的Dulbecco改良Eagle培养基(DMEM)中,于37 °C、5% CO2湿化气氛下培养。小鼠白细胞细胞系RAW264.7在含10% FBS的培养基中,于37 °C、5% CO2下培养。

3.3. 铋纳米点封装ZIF-8纳米粒子(BZ)的制备 典型步骤:将Zn(NO3)2·6H2O(100 mg)、Bi(NO3)3·5H2O(70 mg)和2-甲基咪唑(1.94 g)的混合物溶解于10 mL去离子水中,搅拌5分钟。随后,将50 mg NaBH4溶于1 mL去离子水中,迅速加入上述混合物,再搅拌1分钟。反应结束后,产物经离心分离,用去离子水洗涤三次,然后真空干燥。铋含量通过ICP-AES定量。

3.4. 负载GA的BZ(GBZ)纳米粒子的制备 GBZ纳米粒子的制备如下:将1 mL GA溶液(1 mg mL−1,分散于DMSO中)缓慢加入1 mL含1 mg BZ的DMSO中,室温搅拌30分钟。随后将混合溶液以8000 rpm离心10分钟,用蒸馏水洗涤。载药量(LC)按以下公式计算:LC =(投药量 − 剩余药量)/ 载药纳米粒子质量 × 100%。52

3.5. 表征 采用X射线衍射仪(D8 Advance,AXS Instruments,德国)通过粉末X射线衍射(XRD)研究产物的晶相和相纯度。透射电子显微镜(TEM)图像由Philips Tecnai-12(荷兰)在120 kV下获得。采用配备能量色散X射线(EDX)光谱仪的场发射扫描电子显微镜(FE-SEM,S-4800,Hitachi)分析样品组成。UV-vis-NIR光谱由UV-3600分光光度计采集。纳米粒子在1× PBS中的水合粒径通过动态光散射(DLS)(Nano-Zen 3600,Malvern Instruments,英国)测量。

3.6. 光热转换效率 使用1064 nm近红外激光器(中国长春新产业光电技术有限公司)照射不同浓度(0、50、100和200 μg mL−1)的BZ PBS溶液。在激光照射期间,每30秒用红外热成像系统获取BZ纳米粒子悬浮液的光热图像。激光器配备7 mm²圆形光斑模块,功率可调。光热转换效率按以下公式计算:41 η = [hS(Tmax − Tsurr) − Q0] / [I(1 − 10^−Aλ)] 其中h为传热系数,S为容器表面积,Tmax和Tsurr分别为平衡温度和环境温度,Q0为溶剂光吸收产生的热量,Aλ为BZ纳米粒子在1064 nm处的吸光度,I为激光功率密度。根据该公式,BZ纳米粒子的η值约为24.4%。

3.7. 药物释放 分别研究了由pH变化或近红外光照引发的GA释放。为考察不同pH值下GA负载GBZ的累积释放曲线,将5 mg纳米粒子分散于20 mL缓冲溶液(pH 7.4和5.5)中,37 °C连续搅拌。在每个时间点取1 mL释放介质,通过紫外-可见分光光度法测定释放至溶液中的GA浓度,随后将样品返回原始释放系统。随后,在1064 nm激光照射下,不同pH值中DOX的释放曲线也通过上述紫外-可见分光光度法测定GA释放量。

3.8. GBZ纳米粒子的体外光热能力 3.8.1 活死细胞染色。将Huh-7细胞接种于6孔板,孵育24小时后,分别加入PBS、BZ、GA和GBZ,继续孵育24小时。随后,细胞接受激光照射(808 nm,1 W cm−2)5分钟,用1 mg mL−1碘化丙啶(PI)和5 mg mL−1荧光素二乙酸酯(FDA)共染色15分钟,PBS洗涤数次。荧光显微镜图像由Olympus IX81显微镜获取。 3.8.2 CCK-8和蛋白质印迹实验。通过Cell Counting Kit-8(CCK-8,日本Dojindo)实验检测各纳米粒子组的光热消融细胞毒性。将8×10^3个Huh-7细胞每孔接种于96孔板并培养。24小时后,分别加入PBS、BZ、GA和GBZ,与Huh-7细胞共培养0、24和48小时。随后,在不同时间点进行激光照射(808 nm,1 W cm−2)5分钟。按说明书加入CCK-8溶液,继续孵育2小时。细胞毒性按处理组(T)与对照组(C)光密度(OD)值之比(T/C × 100%)计算。提取细胞蛋白以检测热休克蛋白90(Hsp90)的表达水平。 3.8.3 GBZ纳米粒子的生物相容性。通过上述CCK-8实验评估GBZ纳米粒子的生物相容性。将L02、MCF-7、RAW 264.7和Huh 7细胞系接种于96孔板并培养。24小时后,分别加入GBZ,与各细胞系共培养12、24和48小时。细胞毒性按处理组(T)与对照组(C)光密度(OD)值之比(T/C × 100%)计算。

3.9. 体内实验 雄性BALB/c裸鼠购自中国医学科学院(北京)。本研究严格按照《实验动物管理条例》执行,并经武汉大学动物实验中心/生物安全三级实验室批准。将5×10^6个Huh-7细胞皮下注射至4周龄雄性BALB/c-nu小鼠侧腹。当肿瘤体积达到约200 mm³时开始治疗。将小鼠随机分为4组:一组静脉注射200 μL PBS,另一组静脉注射BZ,其余两组静脉注射GBZ。24小时后,对PBS、BZ和GBZ组荷瘤小鼠进行麻醉,将整个肿瘤暴露于激光照射(808 nm,1 W cm−2)5分钟。另一GBZ组不接受激光照射。激光照射期间,使用红外热成像仪监测肿瘤部位温度变化。照射后每日测量肿瘤体积和体重变化。肿瘤体积V(mm³)按公式计算:体积 = 肿瘤长度 × 肿瘤宽度² / 2。注射14天后,每组随机选取一只小鼠进行PET检查,其余小鼠处死。提取肿瘤进行H&E、Ki-67和末端脱氧核苷酸转移酶dUTP缺口末端标记(TUNEL)染色。同时,提取肿瘤进行免疫荧光染色以检测Hsp90的表达水平。

3.10. 统计分析 数据以平均值 ± 标准差(SD)表示,每组至少三次重复实验的平均值。使用GraphPad Prism 7.0进行非参数检验,评估两组间差异的显著性,***p < 0.01。

4. 总结 综上所述,我们开发了一种易于合成的BZ纳米材料,用于纳米医学递送。该合成方法提高了合成效率,展现出广阔的应用前景。所合成的纳米材料在近红外二区具有良好的光吸收能力和光热循环稳定性,并表现出优异的生物相容性。随后,将Hsp90的天然抑制剂GA高效负载于所合成的BZ纳米材料上。由于GA可下调Hsp90以克服癌细胞的热抗性,GBZ在43 °C的低温PTT中实现了高效的体内肿瘤凋亡。

利益冲突 作者声明无利益冲突。