Tao
Jia‡
a,
Jiating
Xu‡
a,
Shuming
Dong
a,
Fei
He
*a,
Chongna
Zhong
a,
Guixin
Yang
a,
Huiting
Bi
a,
Mengshu
Xu
a,
Yingkui
Hu
a,
Dan
Yang
a,
Piaoping
Yang
*a and
Jun
Lin
*b
aKey Laboratory of Superlight Materials and Surface Technology, Ministry of Education, College of Materials Science and Chemical Engineering, Harbin Engineering University, Harbin, 150001, P. R. China. E-mail: hefei1@hrbeu.edu.cn; yangpiaoping@hrbeu.edu.cn
bState Key Laboratory of Rare Earth Resource Utilization, Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130021, P. R. China. E-mail: jlin@ciac.ac.cn
First published on 31st July 2019
Long-term tumor hypoxia has always been a huge obstacle for oxygen dependent photodynamic therapy (PDT) and anticancer drug chemotherapy. Herein, a hollow-structured biophotocatalyst was developed by coating mesoporous cerium oxide (mCeOx) on upconversion nanoparticles (UCNPs, NaGdF4:Yb,Tm@NaGdF4), and it can be initialized with a near-infrared (NIR) laser to achieve PDT with O2 compensation by decomposing the endogenous H2O2 in the tumor microenvironment. A NIR laser with a long wavelength has low phototoxicity to biotissue, and the core–inert shell structured UCNPs can efficiently convert the NIR photons into ultraviolet (UV) light, which can further trigger CeOx to produce reactive oxygen species (ROS). Moreover, the internal space of UCNPs@mCeOx is ideal for storing chemotherapeutic doxorubicin (DOX), and adequate O2 plays a key role in alleviating drug fastness via chemotherapy in hypoxic tumors, thereby strengthening the synergy between PDT and chemotherapy. After being injected into tumor-bearing mice intravenously, the nanomedicine was able to reach the tumor via an enhanced permeability and retention (EPR) effect. In addition, the capability to use the developed nanosystem in computed tomography (CT), magnetic resonance (MR) and upconversion luminescence (UCL) imaging was validated. Significantly, the NIR laser irradiated nanomedicine exhibits an excellent anticancer effect, implying promising theranostic applications.
Suitable photosensitizers (PSs), excitation light sources, and oxygen (O2) are prerequisites for PDT.10–12 In the process of PDT, antitumor activity from reactive oxygen species (ROS) can oxidize lipids, amino acids and proteins in cell membranes or organelles (including the mitochondria, Golgi apparatus, and endoplasmic reticulum) resulting in irreversible cell damage.13–15 They are generated from molecular O2 by an excited photosensitizer upon local illumination for tumor cell ablation.16–18 However, solid tumors in the process of rapid proliferation, which results in insufficient blood supply and O2 sites in the tumor microenvironment (TME), will not only reduce the effect of traditional tumor treatment methods such as chemotherapy and radiotherapy, but will also have a significant impact on the therapeutic effect of PDT.19–21
At the same time, after the photosensitizer is exposed to light during the PDT process, the O2 at the tumor site will be rapidly consumed, causing the partial pressure of O2 to rapidly decline and fail to be supplemented, thus further limiting the killing effect of PDT.22–24 Therefore, improving the characteristics of hypoxic tumor sites is an urgent challenge to be addressed for PDT.
During the past few years, various strategies have been proposed for the use of microcarriers to deliver O2 to overcome tumor hypoxia.25–27 Chen et al. prepared a nano-pharmaceutical drug based on catalase (HAOP NP) that mainly included a PS, methylene blue (MB), a catalyst (CAT), cyclopentapeptide c(RGDfK) and quencher-linked polymers (BHQ-3) with a shell composition.28 The nano-pharmaceuticals could be specifically assimilated into tumor cells. Under the action of the CAT, H2O2 was converted into O2, which improves the efficiency of ROS production and overcomes the problem of tumor hypoxia. Luo's group used lipopolymers, hemoglobin (Hb) and indocyanine green (ICG) to prepare a nanodrug capable of carrying O2 that can increase the O2 content of tumor hypoxic tissue and strengthen the PDT therapeutic effect.29 Other researchers achieved the transportation of O2 by encapsulating Hb and a second-generation PS (ZnPc) in a micelle formed by a triblock copolymer.30,31 Hb as an O2 carrier provides a special method for overcoming tissue hypoxia, which makes use of the high reactivity and catalytic effect of manganese dioxide (MnO2) particles on endogenous hydrogen peroxide in the TME to produce O2. Separately, some researchers have combined hyperbaric O2 therapy with PDT to strengthen the therapeutic effect, further demonstrating the key role of tissue O2 in the efficacy of PDT therapy.32,33
However, to obtain effective micro-carriers with O2 release and PDT functions, several barriers need to be overcome: the combination of an O2 carrier and PDT requires the combination of an O2 catalyst and an organic photosensitizer,34 leading to a very complicated carrier structure, and some photosensitive molecules that do not adsorb strongly on the surface of the carrier are easily shed in the blood. In addition, there are many reported organic photosensitizers that may suffer severe damage during light exposure and lose their long-lasting photodynamic effects.35,36 Consequently, it is necessary to find a photocatalyst with high optical stability to prevent photodamage.
Cerium oxide nanoparticles (NPs) have attracted increasing attention owing to their enzyme-like activity. They have superior redox properties and can be used as a catalyst with the ability to reversibly transform from Ce4+ to Ce3+ while converting H2O2 to H2O and to O2 even in the absence of light irradiation. Hence, cerium oxide NPs can achieve O2 compensation to continuously generate O2 and provide an O2 environment for PDT and chemotherapy, thus improving cancer treatment efficiency.37–39 As a semiconductor catalyst, cerium oxide has a relatively unusual specific surface area, which effectively enhances the light capturing ability of the material. The defects on its grain surface and abundant O2 vacancies further enhance its catalytic ability and the use of visible light.40–42 Furthermore, cerium oxide has a strong UV absorption and has a high refractive index and diffusibility, which are extremely pivotal for the degradation of contaminants and microorganisms.43–45 Therefore, combining photocatalytically effective cerium oxide and PDT is highly attractive for cancer therapy. When cerium oxide is applied for the treatment of PDT, the main hindrances include UV injury and the penetration distance in the tissue when UV light is directly irradiated.46–48
In this study, we designed a mesoporous core–shell structure by coating hollow cerium oxide on UCNPs (denoted as UCNPs@mCeOx), which is capable of achieving in situ O2 generation and NIR light-triggered PDT for efficient PDT simultaneously. UCNPs@mCeOx is able to efficiently and stably break down endogenous H2O2 to O2 at physiological pH or in a weakly acidic tumor microenvironment owing to its characteristics, such as its ability to act like a catalase,49–51 thus producing sufficient O2 to enhance the PDT effect and chemotherapy. Additionally, UCNPs are energy converters that can transform low-energy photons to high-energy photons and exhibit strong upconversion (UC) fluorescence.52–55 Compared to downconversion NPs, UCNPs can assimilate NIR light with a relatively high tissue penetration depth.56–58 Under these conditions, upon NIR 980 nm laser irradiation, Yb3+ and Tm3+-doped UCNPs (NaGdF4:Yb,Tm@NaGdF4, by coating a homogeneous NaGdF4 inert layer, the activator is far away from the surface of the NPs, which can considerably inhibit the annihilation of the luminescence caused by the surface defects of the material) can continuously convert NIR light into UV emission, which will trigger a cerium oxide-based photocatalytic reaction to generate an electron–hole (e−–h+) pair, and efficiently decompose H2O and O2 to hydroxyl radicals (˙OH) and superoxide radicals (˙O2−), inducing apoptosis in tumor cells.59–61 The sufficient O2 produced via the decomposition of H2O2 by cerium oxide significantly increases the yield of ˙O2−, thus improving the efficacy of PDT. Moreover, after the silica shell is etched, its hollow structure can be used as a carrier for the delivery of the chemotherapy drug DOX through the mesoporous channel.62,63 The surface water-solubility and surface potential of the NPs can be changed by modifying the surface of UCNPs@mCeOx with phosphoserine and mPEG to better combine with DOX and provide simultaneous treatment via PDT and chemotherapy. In addition, the developed nanosystem has multiple imaging capabilities, including use with UCL, MRI and CT, which have great potency in the cancer diagnosis field.
Scheme 1 Schematic illustration for the formation and transport of PEG/UCP-DOX in blood vessels, EPR-mediated tumor accumulation, proposed PDT mechanism, and multiple imaging functions. |
The core NPs (OA-NaGdF4:Yb,Tm) and core–shell structured NPs (OA-UCNPs) were synthesized by the RE(oleate)3 thermal decomposition method in accordance with a prior study.64Fig. 1a–d present the TEM images of the OA-NaGdF4:Yb,Tm, OA-UCNPs, UCNPs@mSiO2, and UCNPs@mCeOx, respectively. Fig. 1a shows that the OA-NaGdF4:Yb,Tm NPs are composed of homogeneous and monodisperse particles (approximately 20 nm in diameter). To keep the activator away from the surface defects and the surface-related high-frequency vibrations of the material, a homogeneous inert layer of NaGdF4 was evenly coated on the core using an external extension growth method. As shown in the TEM photo (Fig. 1b), the dispersion and orderliness of OA-UCNPs were well maintained, and the average particle size was enhanced to 31 nm. Before coating the silica shell, the UCNPs were mixed with cetyltrimethylammonium bromide (CTAB) and stirred for approximately 12 h. The sol–gel technique was used to prepare the UCNPs@SiO2 nanospheres. Fig. 1c shows that the UCNPs@mSiO2 is composed of uniform particles with an average size of 46 nm. In contrast, careful observation showed the presence of worm-like tunnels on the siliceous shell. Then the cerium oxide was coated on the silica shell, and the shell was etched to obtain UCNPs@mCeOx. As shown in Fig. 1d, for UCNPs@mCeOx (approximately 48 nm in diameter), a hollow structure was evident with spherical UCNPs inside and an outer layer of CeOx composed of tiny particles. As presented in Fig. 1e, the elemental mapping provided evidence of the constituent elements and well-dispersed CeOx on the UCNPs. As displayed in Fig. 1f, the cross-sectional compositional line profiles validate the core–shell structure of the UCNPs@mCeOx. Notably, the dispersibility and uniformity of the UCNPs@mCeOx were well maintained after coating CeOx, which was confirmed by the SEM images shown in Fig. 1g–i. The energy-dispersive spectrum (EDS) (Fig. 1j) shows the basic elements of UCNPs@mCeOx, verifying the successful coating of CeOx, which is consistent with Fig. 1e. The particle size change for the prepared samples was also confirmed by dynamic light scattering (DLS) measurements. Such a size could promote better aggregation of the nanomedicine at a tumor site via an EPR effect.65–67 As displayed in Fig. S1,† the particle size of UCNPs@mCeOx changed from 82 nm to 103 nm owing to the polymer coating, the etching of the mesoporous silica shell and the adsorbed water molecules on the NP surface. Moreover, as shown in Fig. S2,† after CeOx modification, the zeta potential of the UCNPs@SiO2 NPs changed from negatively charged (−17 mV) to positively charged (+1.64 mV), confirming the successful surface modification of UCNPs. The UCNPs@mCeOx was then modified with phosphoserine and further modified with mPEG to form PEG/UCP, which strengthened its water-solubility and can prolong the blood recurrence period in a living system. After it was further modified with PEG, the zeta potential of the final PEG/UCP sample changed to −3.17 mV. The hydrodynamic size of the polymer after modification was approximately 110 nm, showing excellent stability in physiological solutions. We also studied whether pure cerium oxide can produce ROS in the absence of a laser. As presented in Fig. S3,† even after prolonged mixing of NPs in DPBF solution, the absorption curve of DPBF hardly changed, confirming that the NPs did not produce ROS in the absence of the laser. Furthermore, Fig. 7b shows the cell viability of HeLa cells incubated with different concentrations of PEG/UCP, and almost no change was found compared with the control group (natural growth), implying that PEG/UCP did not enable the PDT effect without laser irradiation. The colloidal stabilities of the NPs in PBS (pH 7.4), FBS, serum and culture medium were also investigated. After the PEG/UCP NPs were shocked softly in different solutions for various times (0, 6, 12, 24, and 48 h) at 37 °C, the particle size was measured using dynamic light scattering (DLS). As presented in Fig. S4,† the particle size of PEG/UCP did not show any significant change in the different solutions for various periods, indicating the excellent stability of the PEG/UCP in biological mimicking systems.
The XRD patterns for the OA-UCNPs and UCNPs@mCeOx, and the standard lines for hexagonal NaGdF4 (JCPDS no. 27-0699), CeO2 (JCPDS no. 43-1002) and Ce2O3 (JCPDS no. 44-1086) are shown in Fig. 2a. As shown, the diffraction peak for pure β-NaGdF4 remains well formed for these samples. Comparing UCNPs@mCeOx with UCNPs reveals that there are several sharp peaks at approximately 2θ = 28.5°, 2θ = 31.5°, 2θ = 47.5° and 2θ = 58.6° assigned to CeOx, which implies the existence of crystalline CeOx. The FT-IR spectra (Fig. 2b) of OA-UCNPs, UCNPs@mSiO2, UCNPs@mCeOx and PEG/UCP were measured to confirm the successful modification. As displayed in Fig. 2b, OA-UCNPs show a band associated with carboxyl groups at 1463 and 1564 cm−1, and the wide band at 3450 cm−1 is ascribed to the O–H telescopic vibration. The strong bands at 2924 and 2854 cm−1 are mainly derived from symmetric and asymmetric stretching vibrations of –CH2. For UCNPs@mSiO2, the broad peaks at 3432 and 947 cm−1 indicate that there is considerable OH (–OH groups and Si–OH) on the surface, and the peaks at 802 and 1087 cm−1 are associated with Si–O–Si vibrations. The FT-IR spectrum of UCNPs@mCeOx is analogous to that of UCNPs@mSiO2 because of the identical functional groups on the particle surface, apart from a vibration band of Ce–O–Ce at 1400 cm−1. After surface modification of UCNPs@mCeOx with PEG, an intensive C–O stretching vibration in PEG was found in contrast to the vibrations for UCNPs@mCeOx. For PEG/UCP-DOX, the additional bands at 1250–1750 cm−1 are related with the loaded DOX numerators (Fig. S5†). The pore size distribution profile and the N2 adsorption/desorption isotherm of UCNPs@mCeOx are displayed in Fig. 2c and d.
The sample exhibits a representative type IV isotherm, indicating a mesoporous silica channel. Additionally, the sample has a Brunauer–Emmett–Teller (BET) surface area of 164.26 m2 g−1, an average pore size of 2.83 nm, and a total pore volume of 0.42 cm3 g−1. After it was modified with L-O-phosphoserine and mPEG-NH2, the corresponding values for the sample decreased to 156.64 m2 g−1, 2.24 nm, and 0.35 cm3 g−1, respectively (Fig. S6a and b†). The final PEG/UCP-DOX had a lower BET surface area of 107.26 m2 g−1, an average pore diameter of 2.16 nm and a smaller pore volume of 0.29 m2 g−1 (Fig. S6c and d†), which may be due to the DOX loading.
In general, the cerium chemical valence state on the periphery of the UCNPs@mCeOx is a blended valence state. In Fig. S7,† the X-ray photoelectron spectroscopy (XPS) spectrum shows the trivalent and tetravalent Ce ions (Ce3+/Ce4+ = 1/3).
This special valence combination endows UCNPs@mCeOx with catalase-like activity; thus, Ce4+ and Ce3+ can react as follows:
H2O2 + 2Ce4+ → 2H+ + O2 + 2Ce3+ | (1) |
H2O2 + 2Ce3+ + 2H+ → 2Ce4+ + 2H2O | (2) |
The UC emission spectra for NaGdF4:Yb,Tm, UCNPs and UCNPs@mCeOx excited by the 980 nm NIR laser (a power density of 0.72 W cm−2) are displayed in Fig. 3a. The emissions at 361, 453, 475, and 640–670 were assigned to 1D2 → 3H6, 1D2 → 3F4, 1G4 → 3H6 and 1G4 → 3F4 Tm3+ ion transitions, respectively. The NaGdF4 inert layer was coated on the core particles to achieve ultra-bright UC under low excitation power. Obviously, the UC emission intensity of the UCNPs is much stronger than that of pure core NPs. Thus, the NaGdF4 layer can protect the activators of Tm3+ from surface-related high-frequency non-radiative decay vibrations, thus improving the emission intensity of the core NPs. Compared to that of UCNPs that have a core–shell structure, the UC emission intensity of UCNPs@mCeOx drastically decreased in the UV region, which was perhaps caused by the efficient energy transfer between the UCNPs and the CeOx shell. In Fig. 3b, the ultraviolet-visible-infrared (UV-vis-IR) diffuse reflectance spectrum of UCNPs@mCeOx demonstrates a high UV absorption. When excited by 980 nm light, only the blue UC emission (1G4 → 3H6 transition) was present in the emission spectrum of UCNPs@mCeOx. Compared to that of the UCNPs, the decrease in the UV range (1I6 → 3F4 transition) of UCNPs@mCeOx showed that the emitted UV light excites the photo-generated electrons in the valence band to the conduction band of mCeOx, resulting in the formation of a photo-induced electron–hole (e−–h+) pair (Fig. 3b).
Compared to that of the UCNPs, the luminescence intensity of UCNPs@mCeOx is considerably reduced perhaps owing to the quenching effect of cerium oxide and the strong absorption of cerium oxide in the UV region. In accordance with theory, the luminescence intensity of a luminescent donor decreases with the combination of energy receptors of the photosensitizer. This is consistent with the lifetime measurement shown in Fig. S8.† As displayed, the decay lifetime of Tm3+ at 475 nm decreased from 964.14 μs to 277.74 μs after coating with CeOx, confirming the effective energy transfer between UCNPs and CeOx. Fig. 3d and e show the DOX standard profile, and the absorption spectra of the DOX original solution and the supernatant of PEG/UCP-DOX at 480 nm, respectively. On the basis of the Lambert–Beer method (A = Kbc), the DOX loading rate was calculated to be 47.52%. In Fig. 3f, the UV-vis absorption spectrum of PEG/UCP-DOX shows a distinct absorption band at 460–500 nm, which is mainly caused by DOX loading.
To assess the catalytic capability of the UCNPs@mCeOx, the O2 produced by depleting H2O2 at different time periods was measured upon 980 nm laser irradiation (Fig. 4a and b). The quantity of O2 produced reaches 2.97 mg L−1 in H2O2 solution under physiological pH conditions (pH 7.5) within 30 min, and the O2 production is decreased to 2.06 mg L−1 and 1.32 mg L−1 at pH values of 5.5 and 4.5, respectively. These results agree with prior reports.68,69 Moreover, the catalytic capability of UCNPs@mCeOx in the absence of laser irradiation was also measured. Fig. S9† shows that the O2 production decreased slightly, while the rates of H2O2 decomposition became lower than the corresponding values in the presence of NIR light irradiation. This result can be explained by the fact that NIR light separates electrons and holes. The holes have a strong oxidation capability that can cause H2O2 to decompose to O2, resulting in an increased decomposition of H2O2 and an enhanced production of O2. Although some O2 will change to superoxide radicals (˙O2−), the trend of increased production of O2 and decomposition of H2O2 is predominant overall. In addition, it is noteworthy that at pH 6.5, the O2 production still reaches 2.73 mg L−1, indicating that endogenous H2O2 can be efficiently converted to O2 in the weakly acidic microenvironment of a tumor site upon laser irradiation. Fig. 4c shows the change in absorbance of DPBF solutions of UCNPs@mCeOx at different time periods upon 980 nm laser irradiation. Clearly, the absorption peak for DPBF decreased at 350–470 nm, demonstrating that the ROS yield increases gradually with irradiation time. Furthermore, the intracellular ROS production of PEG/UCP as measured with 2,7-dichlorofluorescein-diacetate (DCFH-DA) was studied. DCFH-DA could be absorbed by the cells and did not fluoresce. After intracellular esterase hydrolysis to DCFH, non-fluorescent DCFH could be oxidized by ROS to form 2,7-dichlorofluorescein (DCF), which emitted green fluorescence upon 488 nm light irradiation. Fig. 4d shows the CLSM photos of HeLa cells with fluorescence of DCF, and the more intense green fluorescence illustrates the efficient ROS production in PEG/UCP upon 980 nm light irradiation.
The NIR light excited photocatalytic performance of UCNPs@mCeOx was studied. The hydroxyl radicals and superoxide radicals generated in aqueous solutions upon 980 nm laser irradiation were detected via electron spin resonance (ESR) (Fig. 4e). The spin trap dimethyl pyrroline N-oxide (DMPO) is a capture agent that is used to react with generated hydroxyl radicals and superoxide radicals to form different detection signals. The four peaks assigned to ˙OH were trapped by DMPO, which illustrated the production of ˙OH (Fig. 4e), and the sextet ESR signal indicated the existence of superoxide radicals (˙O2−) (Fig. S10†). Furthermore, MB is a dye that can be decolorized by ˙OH and was chosen to test the generation of ˙OH at an absorbance wavelength of 662 nm. In Fig. 4f, with the extension of the 980 nm laser irradiation time, a significant decrease occurred, proving that UCNPs@mCeOx can produce ˙OH upon NIR light irradiation. Moreover, the stability of MB under 980 nm laser irradiation was studied, and the pure MB solution exhibited almost no change after irradiation with the 980 nm light for 30 min, certifying that MB has excellent stability under irradiation. Additionally, the drug release properties of PEG/UCP-DOX were studied. As presented in Fig. 4g, the PEG/UCP-DOX has a pH-responsive release behavior in PBS. The DOX release progressively increased upon increasing the solution acidity, and finally reached a value of approximately 42% at pH 4.5 after 25 h, which illustrated that the release of DOX from the nanosystem was favorable under acidic conditions. The results show the possibility of DOX release in the acidic tumor microenvironment.
To study the cell uptake behavior of the resulting nanosystem, HeLa cells were cultured with PEG/UCP-DOX at 37 °C for 0.5, 1 and 3 h, respectively, and the related CLSM images are shown in Fig. 5a. 4′,6-Diamidino-2-phenylindole (DAPI) has the ability to emit blue fluorescence to label the cell nucleus. The loaded DOX can radiate red fluorescence when stimulated by a 488 nm laser, and the corresponding merged channels of DAPI and DOX are subsequently shown. As indicated, after 0.5 h of incubation, there was a small section of red fluorescence, indicating that a small proportion of PEG/UCP-DOX NPs were internalized by the HeLa cells. With an increase in incubation time, the red fluorescence signal became more intense, demonstrating that more NPs were internalized by the cells. These results confirmed that the NPs can be efficiently assimilated by tumor cells. It is worth noting that the ingestion of the nanomedicine did not produce morphological changes in the cells, confirming the excellent biocompatibility of the as-synthesized nanosystem. To verify that the acquired sample could be used as a UCL imaging contrast agent, HeLa cells were cultured with PEG/UCP for 0.5, 1 and 3 h, separately. As demonstrated in Fig. 5b, upon irradiation with 980 nm light, the particles in the cells showed upconverted blue emission, and the intensity became brighter as the incubation time increased. Interestingly, no fluorescence signal was detected outside the cell, indicating that the as-prepared particles were internalized in the cell instead of just being dyed on the membrane surface. The cell uptake of free DOX was also studied. As presented in Fig. S11a and b,† the red fluorescence intensity increased with the extension of incubation time, and free DOX was mainly located in cell nuclei, which was due to the rapid diffusion mechanism of small molecules. Furthermore, the UCL signal was mainly situated in the cytoplasm, confirming that the particles passed through the cell membrane under endocytic and lysosomal effects. The above results imply that PEG/UCP is an efficient UCL imaging contrast agent with a negligible background.
It is known that Gd3+-doped nanomaterials can positively enhance the properties of T1-MRI signals; thus, we assume that NaGdF4-based UCNPs should have favorable T1 MRI imaging performance.70 This was performed in a non-invasive way to obtain high function information and soft tissue comparison. MRI has superior space resolution (tens of microns) and high penetration depth. The signal was positively enhanced over a broad concentration range from 0 to 0.8 mM (Fig. 6a), and the longitudinal relaxivity (r1) value was calculated to be 2.481 mM−1 s−1 (Fig. 6b). The in vivo T1-weighted MRI performance of PEG/UCP was also detected. As shown in Fig. 6c, the mouse injected with the sample in the tumor showed significant T1-weighted signal enhancement compared to the tumor without injection, demonstrating that PEG/UCP can be used as a T1 MRI contrast agent. It is known that CT imaging provides high credibility because it supplies high resolution 3D structural details and deep tissue penetration.71,72 Yb3+-doped materials have been widely investigated as CT imaging contrast agents. Fig. 6d presents in vitro CT imaging of PEG/UCP. As shown, in accordance with the sample concentration increase, the CT signal significantly strengthened. Additionally, the CT value positively increased relative to the concentration with a steep slope of 52.17 (Fig. 6e). In vivo CT imaging is shown in Fig. 6f. The CT value for the tumor site after injection of the NPs with saline was 472.3 Hounsfield units (HU), which is significantly higher than that without injection (78.5 HU).
Prior to actual application, non-cancerous L929 fibroblast cells were used to characterize the in vitro safety of PEG/UCP to normal cells. A typical 3,4,5-dimethylthiazol-2-yl-2,5-diphenyl tetrazolium bromide (MTT) cell survey was carried out on the L929 fibroblast cells. As Fig. 7a shows, the activity of the L929 cells was maintained above 90% after incubation with DMEM for 24 h with different concentrations of PEG/UCP, showing no significant toxic effects over a wide concentration range. This superior biocompatibility shows its potential as a photoactive drug for bio-applications. Additionally, the sample blood compatibility was assessed to ensure its in vivo application (Fig. S12a†). Obviously, there was no appreciable hemolysis phenomenon when different amounts of PEG/UCP were added, indicating a high blood compatibility. And the materials' coagulation was also tested, and the results are shown in Fig. S12b.† As displayed, the coagulation times of PBS (as a control) and different concentration samples (PEG/UCP) were evaluated by activated partial thromboplastin time (APTT), prothrombin time (PT) and thrombin time (TT). It can be clearly seen that with the increase of sample concentration, there is no obvious extension of coagulation time of APTT, PT and TT, demonstrating that the designed nanoparticles have a negligible effect on coagulation time. The in vitro cytotoxicity to HeLa cells under different treatment conditions was assessed by the MTT measurement method. Media containing PEG/CUP and PEG/UCP-DOX NPs were placed in specific wells with different treatments and then incubated for an additional 24 h. As shown in Fig. 7b, the cancer cells seeded with PEG/UCP-DOX with the 980 nm laser irradiation could be substantially inhibited in the entire concentration range. The control group (PEG/UCP) showed negligible toxicity to the cancer cells, while PEG/UCP + NIR exhibited remarkable anti-cancer activity, implying that pure CeOx cannot generate a ROS-induced PDT effect, although it can produce O2 in the absence of NIR light.
The key function of NIR light was also confirmed by the MTT test using the DOX loaded sample. As shown in Fig. 7b, the HeLa cells treated with PEG/UCP-DOX + NIR (t test, P = 1.8 × 10−4versus control) exhibited much lower viability than those treated with PEG/UCP-DOX (t test, P = 2.1 × 10−3versus control). In addition, PI is capable of staining red dead cells with a red emission and was used to prominently label the dead cells under different conditions to illustrate the cell killing efficacy. As Fig. 7c points out, there were almost no red cells treated only with culture medium and only the 980 nm laser, illustrating that NIR irradiation alone has no significant killing efficacy on HeLa cells. Approximately 70% of red cells were observed in the PEG/UCP + NIR treatment group compared to that with only NIR irradiation. This result demonstrates that PDT has a significant effect. For the cells cultivated with PEG/UCP-DOX, almost half of the cells were killed, which means that the nanomaterial successfully released the loaded DOX. As expected, the bottom right image of the group treated with PEG/UCP-DOX + NIR shows the largest number of dead cells. CLSM photos and in vitro viability assays confirmed that PEG/UCP is effective at delivering DOX to cancer cells and exerting excellent anticancer effects. In addition, the related flow-cytometry apoptosis assay (sample concentration: 50 μg mL−1) and vitamin C dyeing experiments certify the cell apoptosis. As shown in Fig. 7d, the percentages of cell apoptosis for treatment with NIR, PEG/UCP + NIR, PEG/UCP-DOX and PEG/UCP-DOX + NIR were 1.4%, 49.7%, 25.5, and 88.7%, respectively, which was consistent with the above MTT results. Vitamin C was used to react with ROS generated by PEG/UCP nanoparticles, which could be utilized to detect the cell cytotoxicity. As displayed in Fig. S13a and b,† with the extension of irradiation time, more and more cells died, certifying the consumption of vitamin C and generation of ROS. The corresponding in vivo UCL images of pork tissue (Fig. S14a†) and a tumor-bearing mouse (Fig. S14b†) indicate that the up-conversion fluorescence of the sample excited by the 980 nm laser could be clearly visualized at a depth of approximately 8 mm, implying the feasibility of its clinical application as an imaging probe.
To clarify the advantages of mCeOx compared with other mesoporous PDT catalysts, we designed UCNPs@mSiO2@mTiO2 (on the basis of the synthesis of UCS, APTES was used to aminate the surface, and 2 mL of ethanol solution containing 20% TBOT was added dropwise to UCS-NH2 and stirred under reflux for 2 h. Then, the obtained NPs were added into a 150 mL reactor and refluxed at 180 °C for 24 h to obtain a crystalline TiO2 shell. After it was treated with ethanol several times, the final mesoporous UCNPs@mSiO2@mTiO2 (denoted as UCST) was obtained. The subsequent modification with PEG and the loading of the drug are also similar to those of the mCeOx based samples). The corresponding XRD patterns, TEM image and EDS spectrum are provided in Fig. S15a–c.† The pore size distribution profile (Fig. S15d†) and N2 adsorption/desorption isotherm (Fig. S15e†) indicate that UCST is a mesoporous material. As displayed in Fig. S15f,† the absorption curve for DPBF gradually decreased with the extended irradiation time, showing that UCST has the ability to generate ROS. Moreover, a typical MTT test was performed on L929 fibroblast cells to verify the in vitro viability of PEG-modified UCST (denoted as PEG/UCST), and it showed no significant toxic effects over a wide concentration range. The in vitro cytotoxicity to HeLa cells subjected to different conditions was assessed by using the MTT method, and Fig. S15i† shows the CLSM images of HeLa cells with the fluorescence of DCF. As shown, the more intense green fluorescence illustrates efficient ROS production in PEG/UCST upon 980 nm laser irradiation. Compared to that indicated by Fig. S15h,†Fig. 7b indicates that PEG/UCP exhibits better PDT (lower cell viability of HeLa cells) at the same sample concentration because cerium oxide has the catalytic ability to decompose endogenous H2O2 into H2O and O2, thereby increasing the level of intracellular O2 to enhance PDT. Moreover, the forbidden bandwidth of cerium oxide is at 2.89 eV, while that of titanium dioxide is at 3.2 eV, which means that cerium oxide can absorb more UV photon energy to generate electron–hole pairs, implying a better PDT effect.
To assay the O2 generation capability from H2O2 with PEG/UCP, 4-hydroxy-3-methoxyphenylacetic acid (HVA) was chosen as the H2O2 probe to react with hydrogen peroxide in the presence of peroxidase to produce a strongly fluorescent substance excited by 312 nm light. As presented in Fig. S16a,† the luminescence gradually weakened with reaction time, which means that H2O2 gradually decomposed. Meanwhile, as the O2 probe, bis(triphenylphosphine) ruthenium(II) dicarbonyl chloride ([Ru(dpp)3]Cl2) was chosen to test the production of O2, and it was oxidized by dissolved O2 and faded when excited by the 488 nm laser. In Fig. S16b,† the progressively attenuated emission intensity in the [Ru(dpp3)Cl2] channel shows evidence of production of O2.
Inspired by the in vitro results, U14 tumor (murine cervical carcinoma) xenografts were injected into female Kunming mice for treatment. In order to study the in vivo performances of the PEG/UCP NPs, U14 tumor-bearing mice that had an i.v. injection of PEG/UCP NPs were imaged using a Bruker In-Vivo F PRO small-animal imaging system. As shown in Fig. S17a,† the fluorescence signal of the PEG/UCP NPs rapidly increased owing to the EPR effect at the tumor sites with the maximum at ≈12 h, indicating that 12 h post injection of the PEG/UCP NPs is the optimal time for in vivo PDT treatment. Moreover, to assess the residual amount of the PEG/UCP NPs in vivo, the major organs were collected from the U14-tumor-bearing mice at different time intervals post injection of the PEG/UCP NPs and then imaged. Fig. S17b† clearly shows that PEG/UCP NPs were highly accumulated in the tumor 12 h post injection compared to the accumulation in the other major organs. Although the liver and lung exhibited high fluorescence intensity because of the macrophage uptake in the reticuloendothelial system, the PEG/UCP NPs steadily decreased over time 48 h postinjection. Next, the Ce level in the major organs at different time intervals after i.v. injection was measured using ICP-MS. As presented in Fig. S17c,† the trends and biodistribution are consistent with FL imaging. The above results show that the designed nanoparticles can be utilized in biosystems to guide PDT therapy.
The therapeutic effect was evaluated by injecting PEG/UCP-DOX intravenously and the equivalent dose of DOX was 2 mg kg−1. Fig. 8a shows the average and relative mice tumor volume for every group during the 14 day treatment period. As expected, PEG/UCP-DOX + NIR showed excellent tumor inhibition performance. Similar to the in vitro results, the tumor growth of the PEG/UCP-DOX + NIR treated group (t test, P = 3.6 × 10−4versus control) was more suppressed than that of the PEG/UCP-DOX treated group (t test, P = 3.5 × 10−3versus the control), suggesting the key role of the NIR light irradiation. To determine the biodistribution of PEG/UCP, the concentration of Ce in the tumors was determined by ICP-MS after injection, and the accumulation of PEG/UCP NPs in the tumors was also tested. As demonstrated in Fig. S18a,† high concentrations of Ce were observed in the tumors after 12 h owing to the EPR effect, and 12 to 48 h was the relatively slow clearance period of PEG/UCP according to Fig. S18b.† After 2 weeks of treatment, tumor growth was slightly inhibited for the group treated with only 980 nm laser irradiation. As displayed in Fig. 8b, the images of tumors from representative mice also confirmed that the PEG/UCP-DOX + NIR-treated group had the smallest tumor volume, proving its superior anti-tumor effect. Meanwhile, Fig. 8c shows clearly that the weights of the tumors after PDT significantly reduced in contrast to those for the control group, while the tumor weights for the PEG/UCP-DOX + NIR-treated group (PDT plus chemotherapy) were the lowest, indicating that the combination of the two therapies had a better effect than treatment with only PEG/UCP-DOX (t test, P = 2.3 × 10−3versus PEG/UCP-DOX). In Fig. 8d, the H&E stained images show the most serious cell necrosis in the PEG/UCP-DOX + NIR treated group, which agrees with the results shown in Fig. 7c. The H&E staining photos of the liver, lung, kidney, heart and spleen (Fig. S19†) confirmed that there was no significant organ damage in any of the groups, revealing the outstanding in vivo biocompatibility of the as-prepared nanomedicine. In addition, complete blood count assessment and serum biochemistry assay were performed after two weeks of treatment, as shown in Table S1,† and the biochemical results including those for alanine transaminase, creatinine, blood urea nitrogen, total protein, and aspartate transaminase, which are closely related to the function of the liver and kidney, were checked. There was no obvious injury to the liver or kidney when compared with the control group. Furthermore, the complete blood tests showed that there was no evident interference of physiological regulation of haem or the immune response in the PEG/UCP-treated mice. In summary, the obtained nanoparticles exhibited high safety when used for in vivo antitumor application.
After it was heated for approximately 10 min, the solution was stirred at room temperature overnight until transparent; then 6 mL of ethanol, 40 mL of water and 300 μL of NaOH (2 M) were mixed into the system, and it was heated to 70 °C. Then 200 μL of TEOS solution was added dropwise and the temperature maintained for 10 min. After centrifuging three times with ethanol, the final centrifugation product was added to 50 mL of ethanol and 0.3 g of NH4NO3, and the mixture was stirred for 2 h at 60 °C, and then centrifuged with deionized water and ethanol in that order. Finally the UCNPs@mSiO2 was obtained.
Footnotes |
† Electronic supplementary information (ESI) available: Dynamic light scattering (DLS) of UCNPs@mSiO2, UCNPs@mCeOx and PEG/UCP; the changes of zeta potentials for nanoparticles obtained for each step; the in vitro detection of ROS with UCNPs@mCeOx; FT-IR spectra of the DOX loaded PEG/UCP-DOX samples; Brunauer–Emmett–Teller (BET) test and the corresponding pore size distribution curves of PEG/UCP and PEG/UCP-DOX samples; the XPS spectra of typical element Ce 2p; decay curves for 1G4–3H6 emission (475 nm) of Tm3+ in UCNPs and UCNPs@mCeOx; the test of O2 production rate and H2O2 decomposition rate catalyzed by UCNPs@mCeOx in the absence of NIR light irradiation; EPR spectra of ˙O2− in the UCNPs@mCeOx aqueous solution; the in vitro UCL imaging of PEG/UCP in pork tissue and a mouse; hemolytic percentage of PEG/UCP to human red blood cells; the corresponding characterization and supplementary data of UCNPs@mSiO2@mTiO2; the confocal laser scanning microscopy (CLSM) images of the degradation of H2O2 and production of O2 at various time periods; ICP-MS of Ce in tumor-bearing mice after injecting PEG/UCP; and H&E stained images of the liver, lung, kidney, heart and spleen achieved from different groups after 14 days of treatment. See DOI: 10.1039/c9sc01615e |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2019 |