Jing-Lan
Kan†
a,
Fan-Hong
Lv†
a,
Wen-Xiu
Ren†
a,
Qun
Guan
a,
Anqi
Xue
b,
Jie
Feng
*a and
Yu-Bin
Dong
a
aCollege of Chemistry, Chemical Engineering and Materials Science, Collaborative Innovation Center of Functionalized Probes for Chemical Imaging in Universities of Shandong, Key Laboratory of Molecular and Nano Probes, Ministry of Education, Shandong Normal University, Jinan, 250014, P. R. China. E-mail: jiefeng@sdnu.edu.cn
bShandong Analysis and Test Center, Qilu University of Technology (Shandong Academy of Sciences), Jinan 250014, P. R. China
First published on 16th August 2025
Photodynamic therapy (PDT) is a minimally invasive and local light-activated treatment for annihilating tumor tissues. However, it is often limited by the tissue penetration depth of common external light sources. To address this issue, we herein report a self-illuminating ZIF-90 MOF-based composite photosensitive system prepared using a combined one-pot self-assembly and post-synthetic modification (PSM) methodology. The obtained PME@Zn/Fe-ZIF-90-Lum consists of the Fe(II)-doped and luminol-decorated MOF host as well as the protoporphyrin IX dimethyl ester (PME) guest. Under the given conditions, the light, which is generated from the Fe(II)-catalysed luminol oxidation by endogenous H2O2, can in situ activate the encapsulated photosensitizer PME to produce reactive oxygen species (ROS) via a chemiluminescence resonance energy transfer (CRET) process. In the absence of an external light source, antitumor PDT is successfully realized and high phototoxicity is fully evidenced by in vitro and in vivo experiments.
Although several types of nanomaterials, including two-photon excitation nanoparticles (NPs),4 upconversion NPs,5 and near-infrared photosensitizers,6–8 have been used to improve tissue penetration for deep-seated treatment, deep-tissue PDT has not been satisfactorily achieved. It is conceivable that if PDT could be performed in the absence of external light sources, this bottleneck would be broken through.
Besides conventional light sources, light can also be generated from chemical reactions in principle. This chemiluminescence is a heaven-sent chance to fabricate a self-illuminating system which is supposed to activate the coexisting photosensitizers via chemiluminescence resonance energy transfer (CRET) to produce ROS for PDT.
Hitherto, several interesting self-illuminating organic transformations, including lophine autoxidation,9 metal-assisted luminol10 and lucigenin11,12 oxidation, and the peroxyoxalate reaction,13–17 have been found to exhibit chemiluminescence. However, only a few self-illuminating systems have been used for tumor therapy thus far.18–25
Nanoscale metal–organic frameworks (NMOFs) have recently been explored as a promising class of nanoplatforms for tumor therapy due to their low toxicity and good biocompatibility.26–28 Therein, on the one hand, organic photosensitizers can be nanocrystallized by loading them onto the NMOF-carriers via either a one-pot reaction or PSM for PDT. For example, ZIF-MOFs are capable of encapsulating rhodamine B,29 BODIPY30 and phthalocyanine31,32 to afford photosensitizer-loaded host–guest photosensitive systems. On the other hand, the pre-embedded organic groups in NMOFs, such as the –CHO in Zn-ZIF-90, can be further functionalized by PSM,33,34 consequently endowing NMOFs with more functionality.
In this contribution, we report a self-illuminating ZIF-90-based composite photosensitive system for tumor photodynamic therapy. As illustrated in Scheme 1, the synthesized PME@Zn/Fe-ZIF-90-Lum composite consists of an Fe(II)-doped, luminol chemiluminescent emitter-modified ZIF-90 host and a PME photosensitizer guest. Under specific conditions, the light generated by Fe(II)-catalyzed luminol oxidation via endogenous H2O2 can in situ activate the coexisting PME photosensitizer through a CRET process, thereby inducing the production of 1O2. Notably, antitumor PDT is successfully achieved without relying on an external light source, and its high phototoxicity is fully validated by both in vitro assays and in vivo experiments. Compared with the aforementioned studies,24,25 our work has made significant breakthroughs in the synthesis strategy for composite nanomaterials. Firstly, we precisely grafted luminol onto the surface of the MOF via a covalent bonding strategy. This design not only significantly enhances the structural stability of PME@Zn/Fe-ZIF-90-Lum but also effectively reduces the risk of luminol being recognized and cleared by the immune system—owing to the covalent modification, luminol forms a tight chemical bond with the MOF framework, constructing an integrated and stable structure. These innovative designs offer a feasible approach for the development of efficient and stable self-illuminating photosensitive systems, which is critical for improving the therapeutic efficacy of PDT in deep-seated tumors.
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Scheme 1 Schematic illustration of the fabrication of PME@Zn/Fe-ZIF-90-Lum and its working mechanism for self-illuminating PDT. |
Specifically, the Fe(II)-doped PME@Zn/Fe-ZIF-90 host–guest system was prepared as purple-dark crystalline solids by one-pot in situ self-assembly of imidazole-2-carboxaldehyde (IcaH), FeSO4/Zn(NO3)2 (molar ratio 0.42:
1), and PME with trioctylamine (TOA) in DMF at room temperature.30–35 The molar ratio of Fe/Zn in the resulting PME@Zn/Fe-ZIF-90 was found to be ca. 0.27
:
1 based on inductively coupled plasma optical emission (ICP-OES) analysis (Table S1). By mixing PME@Zn/Fe-ZIF-90 and luminol in methanol with the aid of diethylamine (DEA) at room temperature for 4 h, the self-illuminating nanoagent PME@Zn/Fe-ZIF-90-Lum was readily generated as a deep brown crystalline solid (Scheme 1), which was further supported by the model reaction between molecular IcaH and luminol to IcaH-Lum under the same reaction conditions (Fig. S1).
Powder X-ray diffraction (PXRD) experiments were obtained on a D8 ADVANCE X-ray powder diffractometer with CuKα radiation (λ = 1.5405 Å) from 2θ = 5° to 50° with 0.01° increments. Ultraviolet-visible (UV-vis) absorption spectra were recorded with a UV-2600 Jingdao spectrophotometer. Fourier transform infrared (FT-IR) samples were prepared as KBr pellets, and FT-IR spectra were obtained in the 4000–400 cm−1 range using a Thermo Scientific Nicolet iS50 FT-IR Spectrometer. Fluorescence spectra were obtained with an FLS-920 Edinburgh Fluorescence Spectrometer with or without a xenon lamp. Chemiluminescence (CL) spectra were obtained with a GloMaxTM 96 Microplate Luminometer. Scanning electron microscopy (SEM) micrographs were recorded on a SIGMA300 scanning electron microscope equipped with an energy-dispersive X-ray detector (X-MAX-20 EDX). X-ray photoelectron spectroscopy (XPS) spectra were obtained from a PHI VersaProbe II. Inductively coupled plasma (ICP) measurements were obtained on a Varian720 ICP-OES. Dynamic light scattering (DLS) and zeta potentials were obtained on a Malvern Zetasizer Nano ZS90 with water as the solvent at 25 °C. Confocal fluorescence imaging studies were performed with a TCS SP8 confocal laser scanning microscope (Leica Co., Ltd. Germany) with an objective lens (×20).
MCF-7 cancer cells (106 cells) suspended in DPBS (100 μL) were subcutaneously injected into the flanks of each mouse to establish an MCF-7 xenograft model. The length (L) and width (W) of the tumor were determined using digital calipers. The tumor volume (v) was calculated by the formula V = 1/2 × L × W2. When the tumor size reached ∼100 mm3, the nude mice bearing MCF-7 tumors (n = 12) were randomly distributed into 3 groups, as follows: (i) control, (ii) PME@Zn/Fe-ZIF-90, and (iii) PME@Zn/Fe-ZIF-90-Lum. After intratumoral injection (1 mg mL−1, 50 μL), the nude mice were fed for 3 days, and for the treatment group, injection of samples (1 mg mL−1, 50 μL) was performed on the tumor site another three times every 3 days. The tumor volume and nude mouse body weight were recorded every two days during the experimental period. The major organs (e.g., heart, liver, spleen, lung, kidney, and tumor) were collected and sliced for H&E staining.
Different from Zn/Fe-ZIF-90, PME@Zn/Fe-ZIF-90-Lum exhibited one strong peak (463 nm) and four weak peaks (537, 560, 590, and 641 nm) in its UV-vis spectrum, which are associated with the typical porphyrin Soret and Q-band absorptions, respectively. In comparison with free PME, the corresponding absorption bands of the encapsulated PME in PME@Zn/Fe-ZIF-90-Lum were significantly broadened and red-shifted (Fig. 1c), further implying the formation of a host–guest complex rather than the surface adsorption or a simply physical blend.36 The standard curve method revealed that the PME loading amount in PME@Zn/Fe-ZIF-90-Lum is up to ca. 19.0 wt% (Fig. S4). Of note, no absorptions for Zn- and Fe-porphyrin complexes have been found in the UV-vis spectrum,37,38 indicating that the involved metal ions are only located in the MOF framework. In addition, the UV-vis absorption of the covalently grafted luminol was blue-shifted from 358 to 352 nm compared with that of the free luminol molecule (Fig. 1c).
The covalent decoration of luminol on the MOF framework was further confirmed by the Fourier-transform infrared (FTIR) spectra (Fig. S5). The stretching band of CN in PME@Zn/Fe-ZIF-90-Lum at 1634 cm−1 evidenced the formation of the imine linkage.33,34 Meanwhile, the vestigial peak at 1673 cm−1 associated with the aldehyde group suggested that the PSM herein was not quantitative. The amount of luminol decorated in PME@Zn/Fe-ZIF-90-Lum was determined to be ca. 14.4 wt% based on the standard curve method (Fig. S4). As is known, Zn-ZIF-90 possesses a pore size of 11.2 Å in diameter, which is perfectly size-matched to the porphyrin core size (ca. 9.8 Å × 9.8 Å).33 On the other hand, its open pore diameter of 3.5 Å cannot allow luminol (ca. 6 × 7 Å) to get through the ZIF pores to form a host–guest system during the PSM process. Importantly, covalent decoration enables the close chemical binding of luminol to the MOF framework, forming an overall stable structure. This effectively reduces the risk of the luminol being recognized and eliminated by the immune system.39
For tumor therapy, the stability of PME@Zn/Fe-ZIF-90-Lum NPs in aqueous media was examined. The measured PXRD indicated that its crystallinity and structural integrity were well maintained after soaking in PBS solution (pH = 7.4) for 24 h (Fig. S6). Furthermore, no obvious aggregation in PBS or cell culture media (RPMI 1640) was observed after five days (Fig. S7), which is well in accordance with the previous observation for ZIF-based nanoagents.30,39–41 Different from BodipyPhNO2@ZIF-90,30 the ζ potential of the luminol-grafted PME@Zn/Fe-ZIF-90-Lum herein is negative. For example, the measured surface ζ potentials of PME@Zn/Fe-ZIF-90-Lum in aqueous solution with different pH values are ca. −15.6 (pH = 8.0), −13.4 (pH = 7.4), −12.2 (pH = 7.0), −11.6 (pH = 6.5), −9.0 (pH = 6.0), and −8.35 mV (pH = 5.9), respectively (Fig. S8). The negatively charged surfaces of PME@Zn/Fe-ZIF-90-Lum NPs enable the NPs to accumulate in the tumor sites through the enhanced permeability and retention (EPR) effect.42,43
As shown in Fig. 1d, the chemiluminescence emission of IcaH-Lum (380–650 nm, emission maximum at ca. 429 nm) and the electronic absorption of PME (λmax = 405 nm for the Soret band and λ = 504, 539, 575, 631 for four Q bonds) met the spectral overlap requirement for CRET as the donor–acceptor pair.44 So we envisioned that the chemiluminescence energy from IcaH-Lum oxidation could trigger PME emission (λem = 633 nm, Fig. 1e) within the MOF platform. To further prove this CRET process, the fluorescence spectrum of IcaH-Lum/FeSO4/PME/H2O2 was measured in DMF without external light irradiation. As shown in Fig. 1f, two emission maxima at 457 and 634 nm, which are, respectively, assigned to IcaH-Lum and PME, were observed. This result unequivocally indicated that the luminescent acceptor of PME could be activated by the in situ generated light from IcaH-Lum oxidation to emit fluorescence through a CRET process (Scheme 1).
Further study revealed that the PME@Zn/Fe-ZIF-90-Lum fluorescence was H2O2-dependent. To simulate the internal environment of cancer cells, the fluorescence was measured in PBS solution of H2O2 with a concentration range of 1–1000 nM.45–47 As shown, PME@Zn/Fe-ZIF-90-Lum was luminous under the given conditions, and its emission intensity gradually improved with the increasing H2O2 concentration (Fig. S9). In addition, it can be clearly seen that the emission intensity of PME@Zn/Fe-ZIF-90-Lum also increased with elevated pH and incremental MOF concentrations (Fig. S10). All these observations demonstrate that the fluorescence performance of PME@Zn/Fe-ZIF-90-Lum herein is consistent with the molecular luminol emission behavior.10
Besides, Singlet Oxygen Sensor Green (SOSG), which is a specific intracellular green fluorescent probe for 1O2,48 was also used to evaluate the singlet oxygen producing ability of PME@Zn/Fe-ZIF-90-Lum in cells. The fluorescence spectra of Zn/Fe-ZIF-90 (0.7 μg mL−1), PME@Zn/Fe-ZIF-90 (0.9 μg mL−1) and PME@Zn/Fe-ZIF-90-Lum (1.1 μg mL−1) were measured with SOSG (0.08 μM) in the presence or absence of H2O2 (20 μM). Different from Zn/Fe-ZIF-90 and PME@Zn/Fe-ZIF-90, H2O2 can only effectively activate PME@Zn/Fe-ZIF-90-Lum to generate 1O2 under the given conditions (Fig. S11), indicating that the PME photosensitizer and luminol chemiluminescent emitter are essential for this 1O2 production via a CRET process. Then, we used the H2O2 detection kit to detect the H2O2 concentration in MCF-7 cells. The results showed that its concentration was approximately 1.2 nM, which was sufficient to drive the luminescent substrate to generate optical signals and effectively activate the PME photosensitizer, thereby achieving a self-illuminating photodynamic therapeutic effect (Fig. S12).49 Furthermore, its intracellular 1O2 generation was also confirmed using a confocal laser scanning microscope (CLSM). When MCF-7 cells were incubated with PME@Zn/Fe-ZIF-90-Lum (60 μg mL−1) with SOSG (5 μM) for 4 h, green fluorescence was clearly observed in MCF-7 cancer cells (Fig. 2), implying that the self-illuminating PME@Zn/Fe-ZIF-90-Lum can effectively induce 1O2 generation in living cells via the endogenous CRET process. In contrast, negligible changes were observed in a series of control experiments (blank, Luminol/SOSG, PME/SOSG, Zn/Fe-ZIF-90/SOSG, PME@Zn/Fe-ZIF-90/SOSG, PME@Zn/Fe-ZIF-90-Lum and SOSG only) under the same conditions (Fig. 2).
In addition, the localization of PME@Zn/Fe-ZIF-90-Lum NPs in cells was also examined based on the CLSM. As shown in Fig. 3a, the fixed MCF-7 cells were counterstained with 4′,6-diamidino-2-phenylindole (DAPI) and visualized using a blue channel for DAPI (λex = 405 nm, monitored at 425–490 nm) and a red channel for porphyrin species (λex = 514 nm, monitored at 640–750 nm), respectively.36 We noticed that the red fluorescence was mainly located in the cytoplasm, indicating that PME@Zn/Fe-ZIF-90-Lum NPs were principally distributed in the cytoplasm. On the other hand, this test further demonstrated that the PME@Zn/Fe-ZIF-90-Lum nanoagent possesses good membrane permeability. Subsequently, the effect of PME@Zn/Fe-ZIF-90-Lum on the cell viability of normal breast epithelial cells (MCF-10A) was detected through MTT assay. The results showed that even at a concentration of up to 120 μg mL−1, the cell survival rate remained above 90% (Fig. S13), indicating that PME@Zn/Fe-ZIF-90-Lum has no obvious toxicity against normal cells and possesses good biocompatibility.
Encouraged by its novel self-illuminating feature, excellent stability, and prominent biocompatibility, the PDT efficacy of PME@Zn/Fe-ZIF-90-Lum was thus evaluated using MTT assays against MCF-7 cells at various concentrations (0–120 μg mL−1). As shown in Fig. 3b, the in vitro phototoxicity of PME@Zn/Fe-ZIF-90-Lum against MCF-7 cells was rapidly enhanced with its increasing concentration. MCF-7 survival rates of ca. 62, 56, and 30% were observed in the presence of 40, 60 and 80 μg mL−1, respectively. Meanwhile, nonlinear regression fitting was adopted to accurately calculate the half maximal inhibitory concentration (IC50) value of each experimental treatment group. As shown in Fig. S14, PME@Zn/Fe-ZIF-90-Lum exhibited the strongest therapeutic efficacy, with the IC50 value in MCF-7 cells being 68.89 μg mL−1. This observation was further supported by Calcein-AM staining. For example, the proportion of dead MCF-7 cells was up to ca. 70% after incubation with PME@Zn/Fe-ZIF-90-Lum at 80 μg mL−1 for 24 h, which is well in agreement with the MTT results (Fig. S15). Under the given conditions, PME@Zn/Fe-ZIF-90-Lum induced a minimum cell survival rate of ca. 3% at a concentration of 120 μg mL−1, suggesting its excellent in vitro PDT efficiency in the absence of external light irradiation. In contrast, luminol (17.5 μg mL−1, 120.0 μg mL−1PME@Zn/Fe-ZIF-90-Lum equiv.) and PME (17.5 μg mL−1, 120.0 μg mL−1PME@Zn/Fe-ZIF-90-Lum equiv.) were basically nontoxic and they maintained high cell survival rates of ca. 86 and 90%, respectively. On the other hand, Zn/Fe-ZIF-90 (79.9 μg mL−1, 120.0 μg mL−1PME@Zn/Fe-ZIF-90-Lum equiv.) and PME@Zn/Fe-ZIF-90 (102.7 μg mL−1, 120.0 μg mL−1PME@Zn/Fe-ZIF-90-Lum equiv.) exhibited almost the same cytotoxicity towards MCF-7 cells with mortality rates of ca. 23 and 29%, respectively (Fig. 3b). This inconspicuous cytotoxicity might be caused by a tiny amount of hydroxyl radicals (·OH) which were generated from the Fenton reaction of doped ferric ions in the ZIF framework with the endogenous H2O2 under the given conditions.50,51
Based on the above results, we can conclude that our self-illuminating nanoagent PME@Zn/Fe-ZIF-90-Lum enables PDT in the absence of an external light source via an endogenous CRET process to kill cancer cells.
We finally carried out in vivo antitumor experiments on PME@Zn/Fe-ZIF-90-Lum, which were performed on an MCF-7 xenograft model. Twelve nude mice bearing tumors were randomly divided into three groups. Group I was the control group without any treatment. Group II was given PME@Zn/Fe-ZIF-90 at a dose of 50 μL (1 mg mL−1), with administration repeated four times at intervals of 3 days. Group III was given PME@Zn/Fe-ZIF-90-Lum at a dose of 50 μL (1 mg mL−1), with administration repeated four times at intervals of 3 days. As shown in Fig. 4a and b, the tumor volume and weight increased rapidly in control group I. Compared to group I, a slightly slower tumor growth for group II was observed. In contrast, the tumor tissues were significantly eradicated in group III, and the tumor weight was only ca. 35 and 23% of those in groups I and II, respectively. The digital photographs of tumors also showed that the tumor sizes of group III after therapy were much smaller than those of the other groups (Fig. 4c), further confirming that this high self-illumination induced a PDT antitumor effect.
Additionally, by monitoring the weight changes of nude mice for 11 days (Fig. S16), it was found that there was no significant difference between the experimental group and the control group. On further combinination with Hematoxylin & Eosin (H&E) staining to observe the main organs such as the heart, liver, spleen, lung, and kidney, no significant tissue damage or pathological changes were observed (Fig. S17). These results confirmed that PME@Zn/Fe-ZIF-90-Lum has good biocompatibility.
Then, the in vivo distribution of PME@Zn/Fe-ZIF-90-Lum was dynamically monitored using animal fluorescence imaging. The results showed that the fluorescence signal intensity of PME@Zn/Fe-ZIF-90-Lum at the tumor site exhibited a decaying trend over time, and fluorescence enrichment was observed in the liver site (Fig. S18). This indicates that PME@Zn/Fe-ZIF-90-Lum can be gradually cleared through liver metabolism, demonstrating good metabolic safety in the body.
Footnote |
† These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2025 |