Kai Zhang1,2, Zhaofeng Yu1, Xiangdan Meng1,3, Weidong Zhao1, Zhuojie Shi1, Zhou Yang1, Haifeng Dong1, Xueji Zhang3. 1. School of Materials Science and Engineering University of Science & Technology Beijing 30 Xueyuan Road Beijing 100083 P. R. China. 2. Tianjin Key Laboratory of Radiation Medicine and Molecular Nuclear Medicine Institute of Radiation Medicine Chinese Academy of Medical Science and Peking Union Medical College Tianjin 300192 P. R. China. 3. Beijing Key Laboratory for Bioengineering and Sensing Technology Research Center for Bioengineering and Sensing Technology School of Chemistry & Biological Engineering University of Science & Technology Beijing 30 Xueyuan Road Beijing 100083 P. R. China.
Abstract
Hypoxic tumor microenvironment is the bottleneck of the conventional photodynamic therapy (PDT) and significantly weakens the overall therapeutic efficiency. Herein, versatile metal-organic framework (MOF) nanosheets (DBBC-UiO) comprised of bacteriochlorin ligand and Hf6(µ3-O)4(µ3-OH)4 clusters to address this tricky issue are designed. The resulting DBBC-UiO enables numerous superoxide anion radical (O2 -•) generation via a type I mechanism with a 750 nm NIR-laser irradiation, part of which transforms to high toxic hydroxyl radical (OH•) and oxygen (O2) through superoxide dismutase (SOD)-mediated catalytic reactions under severe hypoxic microenvironment (2% O2), and the partial recycled O2 enhances O2 -• generation. Owing to the synergistic radicals, it realizes advanced antitumor performance with 91% cell mortality against cancer cells in vitro, and highly efficient hypoxic solid tumor ablation in vivo. It also accomplishes photoacoustic imaging (PAI) for cancer diagnosis. This DBBC-UiO, taking advantage of superb penetration depth of the 750 nm laser and distinct antihypoxia activities, offers new opportunities for PDT against clinically hypoxic cancer.
Hypoxic tumor microenvironment is the bottleneck of the conventional photodynamic therapy (PDT) and significantly weakens the overall therapeutic efficiency. Herein, versatile metal-organic framework (MOF) nanosheets (DBBC-UiO) comprised of bacteriochlorin ligand and Hf6(µ3-O)4(µ3-OH)4 clusters to address this tricky issue are designed. The resulting DBBC-UiO enables numerous superoxide anion radical (O2 -•) generation via a type I mechanism with a 750 nm NIR-laser irradiation, part of which transforms to high toxic hydroxyl radical (OH•) and oxygen (O2) through superoxide dismutase (SOD)-mediated catalytic reactions under severe hypoxic microenvironment (2% O2), and the partial recycled O2 enhances O2 -• generation. Owing to the synergistic radicals, it realizes advanced antitumor performance with 91% cell mortality against cancer cells in vitro, and highly efficient hypoxic solid tumor ablation in vivo. It also accomplishes photoacoustic imaging (PAI) for cancer diagnosis. This DBBC-UiO, taking advantage of superb penetration depth of the 750 nm laser and distinct antihypoxia activities, offers new opportunities for PDT against clinically hypoxic cancer.
Hypoxia, a quite general feature for most solid tumors (partial oxygen pressure <5 mm Hg), is generally caused by the aggressive proliferation of cancer cells and tumor vasculature distortion.1, 2, 3 Photodynamic therapy (PDT) utilizes a photosensitizer (PS) excited by an appropriate light irradiation to generate reactive oxygen species (ROS); in most of cases, it involves a process that the ground triplet‐state molecular oxygen (3O2) is transformed to the reactive singlet oxygen (1O2) via the type II mechanism extremely dependent on the concentration of oxygen (O2).4, 5, 6, 7 Thus, the O2 shortage in solid tumors significantly limits the anticancer capability of PDT, especially in cases that need continuous treatment.8, 9 To address this issue, various innovative strategies have been developed, such as O2‐replenishing nanosystem to deliver O2 (e.g., hemoglobin and perfluorocarbon)10, 11, 12, 13, 14 or oxygen self‐supplement nanomaterials to generate O2 (e.g., MnO2, Pt, CaO2, and catalase)15, 16, 17, 18, 19 in the tumor microenvironment to elevate the tumorO2 concentration and enhance the PDT efficacy. However, most of these nanocomposite systems undergo tedious fabrication procedures and complex toxicity evaluation owing to the multiple components. Hence, it is highly desirable to develop nanoagents that directly reduce the requirement of O2 in PDT for cancer treatment via type I mechanism (O2‐independent).Superoxide anion radical (O2
−•) produced by charge transfer between the light‐excited PS and adjacent substrates in tumor cells is one of the primary and highly cytotoxic ROS generated from the type I mechanism.20, 21, 22 It reacts with proteins, DNA, or lipids, to achieve irreversible cellular components damage and dysfunction in cell metabolism and even cell apoptosis.23 Moreover, under the intracellular superoxide dismutase (SOD)‐mediated disproportionation reactions, O2
−• molecule further converts to hydrogen peroxide (H2O2) and O2.24, 25, 26 The accumulated H2O2 further transforms into highly cytotoxic hydroxyl radical (OH•) to significantly aggravate the oxidative damage and enhance PDT anticancer efficiency.27, 28 Remarkably, O2 is partially recyclable during this cascade reaction and valuable to ameliorate the hypoxia microenvironment for enhanced PDT efficacy.16, 29, 30 Thus, O2
−• generator would be a promising alternative against hypoxic solid tumor treatment.31 Inorganic and metallic O2
−• generators such as TiO2 and ZnO generally activated by UV‐light suffer from potential side‐effect and low‐penetration.32, 33, 34, 35 Small organic molecular generators undergo water low solubility, and serious aggregation under physiological conditions.36, 37, 38 It still remains a key challenge to develop novel NIR‐trigged O2
−• generators to circumvent the tumor hypoxia.Metal–organic framework (MOF), as a new class of hybrid materials, consists of inorganic building units covalently connected by organic building units.39, 40 Compared to the traditional inorganic/organic nanoparticles, MOF offers adjustable structural and chemical composition at the molecular level together with tunable porosity and chemical stability, which can as transport vehicles for the delivery of imaging agents and biologically active molecules realize accurate diagnosis and treatment of tumors.41, 42 Porphyrins and porphyrin derivatives as photosensitizers are hydrophobic in nature, which not only cause insufficient selectivity to the site of tumor, but also leads to PS polymerization, reducing the efficacy of PDT and making it very attractive for the assembly structure of organic building units of MOF.43 Porphyrin‐based MOF that have been developed so far for potential PDT outcome, however, almost all of them are compounded with other nanoparticles to form new compounds for synergistic treatment (such as PDT‐PTT, PDT‐Radiation therapy),44 the complex structures would reduce the clinical medical value.45 2D nanosheets with large surface area, unique physical, and chemical properties have been widely used as theranostic agents for cancer treatment, such as graphene, transitionmetal dichalcogenides, black phosphorus,46, 47, 48 boron nanosheets,42 accomplishing multimodal imaging‐guided synergistic treatment. Various 2D nanomaterials were used as nanomedicine for cancer therapy via PDT of type II mechanism in normoxia condition.49, 50 However, few 2D MOF nanosheets as PDT agents through type I mechanism were developed at present for cancer therapy overcoming the hypoxia.Herein, we developed a new‐style bacteriochlorin‐based MOFs termed DBBC‐UiO as a NIR laser‐induced O2
−• generator for photoacoustic imaging (PAI)‐guided PDT through synergistic type I and type II mechanism for hypoxia tumor ablation (Scheme
1). The DBBC‐UiOMOF was consisted of 5,15‐di(p‐benzoato)bacteriochlorin (H2DBBC) as blocks and heavy Hf6(µ3‐O)4(µ3‐OH)4 clusters as centers. It is able to act as PS to produce 1O2 under NIR‐laser irradiation via type II mechanism in adequate O2 microenvironment, and also generates considerable O2
−• via type I mechanism under a severe hypoxic microenvironment with a 750 nm NIR‐laser irradiation. The generated numerous O2
−• molecules not only act as cytotoxic anion radical to induce tumor cells apoptosis, but also transform to H2O2 and its downstream highly toxic OH• through SOD‐mediated disproportionation reactions, further promoting the anticancer performance. Meanwhile, the DBBC‐UiO exhibited PAI capability for tumor diagnosis, providing an outstanding strategy for cancer diagnosis with high spatial resolution and deep tissue penetration in clinic. The PAI‐guided striking PDT effect for hypoxic solid tumor ablation under a NIR laser irradiation is promising for clinical hypoxic cancer therapy.
Scheme 1
Schematic illustration of the synthetic procedure and photoinduced PDT mechanism of DBBC‐UiO.
Schematic illustration of the synthetic procedure and photoinduced PDT mechanism of DBBC‐UiO.The H2DBBC block of DBBC‐UiO was prepared by reduction and acidification of 5,15‐di(p‐methyl‐benzoato) porphyrin (Me2DBP) as shown in Figure
1a, and the nuclear magnetism (1HNMR) and mass spectrometry were employed to verify the synthetic procedure and characterize the products in every step (Figures S1–S9, Supporting Information). The transmission electron microscopy (TEM) of DBBC‐UiOMOF revealed a nanosheet morphology with a mean size of about 220 nm and a thickness of 4.6 nm approximately (Figure 1b), and high‐resolution TEM, and fast Fourier transform patterns showed that DBBC‐UiO displayed good crystallinity (inset of Figure 1b). Dynamic light scattering (DLS) results were consistent with the characterization of TEM (Figure 1c). The negligible change of hydrodynamic size for seven consecutive days measurement revealed that DBBC‐UiOMOF presented a good stability in both of PBS (10 × 10−3
m, pH 7.4) and biological media (Figure S10, Supporting Information). The power X‐ray diffraction (XRD) of DBBC‐UiO matched with a framework formula of Zr6O4(OH)4(Zn‐DPDBP)6, indicating UiO‐type MOF structure that Hf6(µ3‐O)4(µ3‐OH)4 secondary building units connected with DBBC bridging ligands (Figure 1d; Table S1 and Figures S11 and S12, Supporting Information).51 The porosity of DBBC‐UiO measured by nitrogen (N2) absorption at 77 K indicated a BET surface area of 198 m2 g−1 and a pore size of 3.1 nm for DBBC‐UiO (Figure 1e). Encouragingly, the synthetic H2DBBC displayed a strong characteristic absorbance peak at the wavelength of 740 nm (Figure S13, Supporting Information). The corresponding peak of the DBBC‐UiOMOF was slightly red‐shifted to 754 nm due to the change of spatial structure and the interaction with Hf4+. The strong and broad NIR absorption provided a great potential for PDT with a deeper tumor tissue penetration (Figure 1f). The weaker fluorescence intensity at 822 nm of the DBBC‐UiO compared to H2DBBC was resulted from the coordination of the H2DBBC ligands to Hf4+ ions (Figure 1g), which led to enhanced intersystem crossing (ISC) responsible to ROS generation.52 The DBBC‐UiO exhibited a slightly shorter fluorescence lifetime of 8.66 ns compared to 8.80 ns of H2DBBC determined by time‐correlated single‐photon counting measurements (Figure 1h).
Figure 1
Synthesis and characterizations of H2DBBC and DBBC‐UiO. a) Synthetic procedure of H2DBBC. b) TEM image, high‐TEM image (insert), and its fast Fourier transform pattern (insert). c) DLS profile of DBBC‐UiO. d) XRD pattern and e) N2 adsorption isotherm of DBBC‐UiO, inset in (e): the pore size distribution of DBBC‐UiO. f) UV–vis absorbance of H2DBBC and DBBC‐UiO. g) Fluorescence spectra of H2DBBC and DBBC‐UiO with excitation at 740 nm, inset in (g): magnified region of DBBC‐UiO from 790 to 860 nm. h) Time‐resolved fluorescence decay traces of H2DBBC and DBBC‐UiO.
Synthesis and characterizations of H2DBBC and DBBC‐UiO. a) Synthetic procedure of H2DBBC. b) TEM image, high‐TEM image (insert), and its fast Fourier transform pattern (insert). c) DLS profile of DBBC‐UiO. d) XRD pattern and e) N2 adsorption isotherm of DBBC‐UiO, inset in (e): the pore size distribution of DBBC‐UiO. f) UV–vis absorbance of H2DBBC and DBBC‐UiO. g) Fluorescence spectra of H2DBBC and DBBC‐UiO with excitation at 740 nm, inset in (g): magnified region of DBBC‐UiO from 790 to 860 nm. h) Time‐resolved fluorescence decay traces of H2DBBC and DBBC‐UiO.1O2 generation efficiency of DBBC‐UiO was first investigated by electron paramagnetic resonance (ESR) using 2,2,6,6‐tetramethylpiperidine (TEMP) as an 1O2 indicator (Figure
2a). The stronger special 1:1:1 triplet characteristic ESR signal assigned to 1O2 was observed for the DBBC‐UiO after irradiation with a NIR laser, indicating 1O2 producing ability of the DBBC‐UiO. The 1O2 luminescence at around 1270 nm that is a characteristic emission peak of 1O2 further confirmed the 1O2 generation ability of DBBC‐UiO (Figure 2b). The characteristic absorption of 1,3‐diphenylisobenzofuran (DPBF) decreased continuously with the time going under the NIR irradiation, future indicating that the good production capacity of 1O2 (Figure 2c; Figure S14, Supporting Information). O2
−• generation of DBBC‐UiO could also be examined using 5,5‐dimethyl‐1‐pyrroline‐N‐oxide (DMPO) as a probe molecule using ESR spectroscopy. As shown in Figure 2d, an obvious characteristic ESR signal of O2
−• was observed compared to DBBC‐UiO in dark and only light irradiation, demonstrating the production of O2
−•. However, in the presence of SOD, corresponding ESR signal was sharply decreased, which resulted from SOD‐catalyzed dismutation of O2
−•. Dihydrorhodamine 123 (DHR123) could react with O2
−• to emit strong green fluorescence with a characteristic peak at 526 nm, which was further applied to monitor the O2
−• production capability. The DHR123 treated with DBBC‐UiO and irradiated with NIR irradiation exhibited strong green fluorescence related to reaction of O2
−• and DHR123, while the addition of the SOD and radical scavenger of Vc induced the sharp decrease of the fluorescence (Figure 2e). The fluorescence intensity of DBBC‐UiO under NIR irradiation showed a 3.18‐fold and 3.3‐fold decrease after addition of Vc and SOD, respectively (Figure 2f). These results confirmed the good 1O2 and O2
−• generation ability of DBBC‐UiO.
Figure 2
a) ESR spectra of DBBC‐UiO in presence of TEMP with or without NIR‐laser irradiation. b) 1O2 emission at around 1270 nm induced by DBBC‐UiO with or without NIR‐laser irradiation. c) Time‐course generation of 1O2 by DBBC‐UiO detecting by the DPBF under NIR laser irradiation. d) ESR signals of DMPO for 1O2 detection. e) Fluorescence response of DHR 123 in different conditions for O2
−• detection. f) The corresponding fluorescence intensity in (e).
a) ESR spectra of DBBC‐UiO in presence of TEMP with or without NIR‐laser irradiation. b) 1O2 emission at around 1270 nm induced by DBBC‐UiO with or without NIR‐laser irradiation. c) Time‐course generation of 1O2 by DBBC‐UiO detecting by the DPBF under NIR laser irradiation. d) ESR signals of DMPO for 1O2 detection. e) Fluorescence response of DHR 123 in different conditions for O2
−• detection. f) The corresponding fluorescence intensity in (e).The cell uptake ability of the resulting DBBC‐UiOMOF nanosheet labeled with FAM was first explored using MCF‐7 as a model. As shown in Figure S15 of the Supporting Information, the DBBC‐UiO was abundant and decentralized in the cells when MCF‐7 cells were exposed to DBBC‐UiO for 4 h, whereas the FAM fluorescence of the lipsome2000 group was comparatively concentrated. This results indicated that the good cell uptake ability of DBBC‐UiOMOF nanosheet, and the high decentralization of the DBBC‐UiO facilitated to the reaction with the substances in living cells, promoting the generation of ROS and accelerating the cell apoptosis. We further examined the ROS generation ability of DBBC‐UiO in living cells under normoxic and hypoxic condition by dihydroethidium (DHE) that react with O2
−•, and the generated product could intercalate with DNA to produce red fluorescence. As shown in Figure
3a, the fluorescence intensity enhanced with the increase of the irradiation time, but after Vc treatment, the red fluorescence sharply reduced due to the O2
−• scavenging effect. Notably, the DHE fluorescence intensity for verifying the O2
−• generation showed negligible change in MCF‐7 cells with NIR irradiation in the hypoxic condition compared to that in the normoxic condition (Figure 3b; Figure S16, Supporting Information), indicating the PDT effect of DBBC‐UiOMOF under hypoxia. No obvious singlet oxygen sensor green (SOSG) signal associated to 1O2 was observed in hypoxic condition, whereas numerous 1O2 was generated in MCF‐7 cells under the normoxic environment (Figure 3b; Figure S16, Supporting Information). 3′‐(4‐hydroxyphenyl) fluorescein (HPF) was used to monitor the OH• generation, and strong fluorescence of HPF was presented in both hypoxic and normoxic conditions after NIR irradiation, which was similar to the O2
−• (Figure 3b; Figure S16, Supporting Information). Furthermore, SOD inhibitor of 2‐methoxyestradiol was employed to characterize the dismutation. As shown in Figure 3c, under NIR irradiation, the DBBC‐UiO‐treated cells exhibited stronger DHE fluorescence intensity compared to that of the cells only incubated with 2‐methoxyestradiol treatment. Notably, the DBBC‐UiO‐treated cells displayed weaker fluorescence intensity compared to that of DBBC‐UiO‐treated cells received 2‐methoxyestradiol incubation under NIR irradiation. Meanwhile, the addition of 2‐methoxyestradiol induced significant reduction of OH• for cells treated with DBBC‐UiO under NIR irradiation (Figure 3d). These results showed that the inactivation of SOD in cells dramatically inhibited the procession O2
−• to OH•.
Figure 3
a) Confocal Laser Scanning Microscope (CLSM) images of MCF‐7 cells exposed on NIR laser at different times with or without Vc treatment. b) CLSM images of ROS in DBBC‐UiO‐treated MCF‐7 cells in normoxia and hypoxia environments using DHE, SOSG, and HPF as O2
−•, 1O2, and •OH detection probe. c) CLSM images of O2
−• and d) OH• for DBBC‐UiO‐treated MCF‐7 cells treated with or without SOD inhibitor 2‐methoxyestradiol. The scale bar is 25 µm.
a) Confocal Laser Scanning Microscope (CLSM) images of MCF‐7 cells exposed on NIR laser at different times with or without Vc treatment. b) CLSM images of ROS in DBBC‐UiO‐treated MCF‐7 cells in normoxia and hypoxia environments using DHE, SOSG, and HPF as O2
−•, 1O2, and •OH detection probe. c) CLSM images of O2
−• and d) OH• for DBBC‐UiO‐treated MCF‐7 cells treated with or without SOD inhibitor 2‐methoxyestradiol. The scale bar is 25 µm.The 3‐(4,5‐dimethyl‐2‐thiazolyl)‐2,5‐diphenyl‐2‐H‐tetrazolium bromide (MTT) assay results indicated that the DBBC‐UiO exhibited no appreciable negative effect on the cell viability in absence of NIR‐laser irradiation both in cancer cells (Figure
4a) or in normal cells (Figure S17, Supporting Information), suggesting the good biocompatibility of DBBC‐UiO. Neither the PBS (10 × 10−3
m, pH 7.4) nor the 750 nm NIR‐laser (1.3 W cm−2) irradiation has obvious effect on the cell viability (Figure 4b). On the contrary, the DBBC‐UiO‐treated MCF‐7 cells presented a cell death rate up to 94% with a 750 nm NIR‐laser (1.3 W cm−2) irradiation at the conditions of normoxia (21% O2) (Figure 4b), which suggested the high anticancer effect. It was worthy to mention that a cell death rate up to 91% was obtained even at the hypoxic condition due to the ROS synergistic effect. As shown in Figure 4c, the Calcien‐AM/PI double staining further suggested the DBBC‐UiO‐transfected cells with NIR‐laser irradiation presented the high cells death rate at the hypoxic (2% O2) condition, showing the consistent performance with the MTT. These results suggested the advanced antitumor efficiency of DBBC‐UiO‐mediated PDT.
Figure 4
a) Cytotoxicity effect of DBBC‐UiO on MCF‐7 and A549 cells (0–200 µg mL−1). b) Relative cell viability of MCF‐7 cells incubated by PBS (10 × 10−3
m, pH 7.4) and DBBC‐UiO with/without a 750 NIR‐laser irradiation for 5 min at conditions of 21% O2 or 2% O2. c) CLSM images of MCF‐7 cells exposed to PBS (10 × 10−3
m, pH 7.4) and DBBC‐UiO with a 750 nm NIR‐laser irradiation for 5 min at conditions of 21% O2 or 2% O2. The scale bar is 100 µm.
a) Cytotoxicity effect of DBBC‐UiO on MCF‐7 and A549 cells (0–200 µg mL−1). b) Relative cell viability of MCF‐7 cells incubated by PBS (10 × 10−3
m, pH 7.4) and DBBC‐UiO with/without a 750 NIR‐laser irradiation for 5 min at conditions of 21% O2 or 2% O2. c) CLSM images of MCF‐7 cells exposed to PBS (10 × 10−3
m, pH 7.4) and DBBC‐UiO with a 750 nm NIR‐laser irradiation for 5 min at conditions of 21% O2 or 2% O2. The scale bar is 100 µm.The intriguing in vitro antitumor performance encouraged us to further investigate the in vivo performance. As shown in Figure
5a, the DBBC‐UiO exhibited good photoacoustic (PA) response, and the concentration‐dependent PA signal intensity increased significantly with the increasing concentration of the DBBC‐UiO (0–1 mg mL−1). Because significant tumor accumulation of DBBC‐UiO resulted from the enhanced permeability and retention (EPR) effects, much stronger PA signal could be observed in the tumor tissue after tail vein injection of DBBC‐UiO into mice for 12 h, which confirmed the feasibility of the DBBC‐UiO for in vivo PA imaging (PAI) (Figure 5b). This good PAI capability of the DBBC‐UiO provided a powerful tool for precise tumor tissue diagnosis.
Figure 5
a) The concentration‐dependent PAI of DBBC‐UiO in vitro. b) In vivo PAI with and without injection of DBBC‐UiO. c) Blood circulation curve of DBBC‐UiO in mice through evaluating the concentration of Hf element in the blood at different time points after the injection of DBBC‐UiO. d) Biodistribution of DBBC‐UiO after tail vein injection. The concentration of Hf element was determined by ICP‐AES. Error bars are basis of the standard deviation (SD) among three mice. e) Relative tumor volumes of mice through different treatments. f) Average weights of tumors harvested after 15 d posttreatment. g) Photographs of tumor‐bearing mice received different treatments after 15 d. h) H&E staining, TUNEL staining, and Ki‐67 of tumor sections from different groups. The scale bar is 100 µm.
a) The concentration‐dependent PAI of DBBC‐UiO in vitro. b) In vivo PAI with and without injection of DBBC‐UiO. c) Blood circulation curve of DBBC‐UiO in mice through evaluating the concentration of Hf element in the blood at different time points after the injection of DBBC‐UiO. d) Biodistribution of DBBC‐UiO after tail vein injection. The concentration of Hf element was determined by ICP‐AES. Error bars are basis of the standard deviation (SD) among three mice. e) Relative tumor volumes of mice through different treatments. f) Average weights of tumors harvested after 15 d posttreatment. g) Photographs of tumor‐bearing mice received different treatments after 15 d. h) H&E staining, TUNEL staining, and Ki‐67 of tumor sections from different groups. The scale bar is 100 µm.The metabolism and biodistribution of DBBC‐UiO were further studied. The blood was extracted from the mice post the injection of DBBC‐UiO at desired time points for measuring quantitatively the Hf element concentrations by inductively coupled plasma atomic emission spectrometry (ICP‐AES). It revealed that blood levels of DBBC‐UiO gradually decreased over time according to a two‐compartment model with t
1 = 0.59/t
2 = 5.57 (Figure 5c). The relative long circulation time of DBBC‐UiO in the blood was favorable for effective tumor tissue accumulation (Figure 5c). High tumor accumulation of DBBC‐UiO at ≈13% ID/g was observed after 24 h injection possibly resulted from the tumor EPR effect (Figure 5d). The high levels of accumulation in liver was observed, which suggested DBBC‐UiO in the main organs of mice could decay rapidly over time.The in vivo PDT antitumor performance of DBBC‐UiO was conducted using nude mice bearing MCF‐7 cells at the right forelimb. It was divided into four groups randomly (n = 5) and given tail intravenous injections with PBS (10 × 10−3
m, pH 7.4) and DBBC‐UiO (5 mg kg−1 for every mouse), respectively, with or without a 750 NIR‐laser (1.3 W cm−2) irradiation. The volume of tumor decreased over the time for the mice received treatment of DBBC‐UiO‐injected and the NIR‐laser irradiation, and it almost completely disappeared in 15 d (Figure 5e,g). All the control groups performed a time‐dependent tumor volume increase, showing more than 10‐fold increment compared to the initial volume and no tumor suppression effect (Figure 5e,g). The mice were scarified and the tumors were explanted in 15 d after treatment, and the average tumor weight and size also confirmed the excellent anticancer performance of the DBBC‐UiO‐mediated PDT (Figure 5g,f). The hematoxylin and eosin (H&E) staining revealed the prominent tissue necrosis and numerous cell apoptosis in the tumor tissues for mice treated with the DBBC‐UiO and NIR‐laser irradiation, while no obvious damage was observed for the tumor tissues of other control groups (Figure 5h). Terminal deoxynucleotidyl transferase dUTP nick end‐labeling (TUNEL) assay demonstrated the largest apoptotic cells in the group treated with DBBC‐UiO and NIR among all groups (Figure 5h). The proliferative activity of tumor cells was further analyzed by immunostaining against ki‐67. The DBBC‐UiO‐treated group under NIR‐laser irradiation displayed least ki‐67 positive cells among the all groups (Figure 5h). The H&E staining of the main organs, including heart, spleen, liver, kidney, and lung collected from the mice after different treatments revealed that no obvious damage could be observed in these organs (Figure S18, Supporting Information). These results suggested the good biocompatibility and excellent anticancer efficiency of DBBC‐UiO.At last, the potential in vivo toxicity of DBBC‐UiO was evaluated by blood routine and biochemical index (Figure 6). As shown in Figure
6a, white blood cells (WBC), red blood cells (RBC), hemoglobin (HB), hematocrit (HCT), mean corpuscular hemoglobin (MCH), mean corpuscular hemoglobin concentration (MCHC), platelets (PLT), and mean corpuscular volume (MCV) as the normal hematology parameters were measured at different time point after the mice were treated with tail vein injection of DBBC‐UiO. In general, this monitored markers had no abnormal changes for 14 d compared with control group, indicating that DBBC‐UiO did not cause significant inflammation or infection in the treated mice. The standard blood biochemical indexes were performed and various makers including alanine transaminase (ALT), aspartate transaminase (AST), total protein (TP), globulin (GLOB), albumin/globulin (A/G), blood ureanitrogen (UREA), creatinine (CREA), and albumin (ALB) were examined (Figure 6b). Hence, the DBBC‐UiO treatment had no obviously negative influence compared with control on the blood chemistry. The hepatic or renal related function markers including ALT, AST, UREA in general had no abnormal changes after the mice treated with DBBC‐UiO for a long time, indicating no significant renal and hepatic toxicity in mice. Nevertheless, our results demonstrated that DBBC‐UiO could act as a nanoplatform for clinical cancer therapy with high biocompatibility
Figure 6
In vivo long‐term toxicity evaluation of DBBC‐UiO. a) Hematological index of the mice including WBC, RBC, HB, HCT, MCH, MCHC, PLT, and MCV. b) Biochemical blood analysis of the mice including ALT, AST, TP, GLOB, A/G, UREA, CREA, and ALB. Untreated healthy mice were used as the control.
In vivo long‐term toxicity evaluation of DBBC‐UiO. a) Hematological index of the mice including WBC, RBC, HB, HCT, MCH, MCHC, PLT, and MCV. b) Biochemical blood analysis of the mice including ALT, AST, TP, GLOB, A/G, UREA, CREA, and ALB. Untreated healthy mice were used as the control.In this work, a novel DBBC‐UiOMOF nanosheet was developed as an NIR‐laser triggered O2
−• generator for PAI‐guided PDT through type I mechanism for selective hypoxia tumor ablation with deep tissue penetration. The DBBC‐UiO enabled to generate abundant O2
−• within a severe hypoxic microenvironment, and partial O2
−• converted into high toxic OH• via SOD‐induced catalytic reactions under 750 nm NIR‐laser irradiation, suggesting that the PDT anticancer capacity of DBBC‐UiO was a complete O2‐independent procedure for highly efficient hypoxic solid tumor suppression. Tumor‐specific PAI was also verified for cancer accurate diagnosis with deep tissue penetration and high resolution. This work contributed to design a new nanoplatform for specific PDT to overcome the hypoxic cancer microenvironment and light tissue penetration depth for clinical cancer therapy.
Experimental Section
For detailed experimental conditions and methods of synthesis, and the additional characterizations, see Figures S1–S14 (Supporting information). All animal experiments were performed according to protocols approved by the Department of Laboratory Animal Science at Peking University Health Science Center.
Conflict of Interest
The authors declare no conflict of interest.SupplementaryClick here for additional data file.