Shuming
Dong
a,
Jiating
Xu
a,
Tao
Jia
a,
Mengshu
Xu
a,
Chongna
Zhong
a,
Guixin
Yang
a,
Jiarong
Li
a,
Dan
Yang
a,
Fei
He
a,
Shili
Gai
*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: gaishili@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 6th March 2019
ZnFe2O4, a semiconductor catalyst with high photocatalytic activity, is ultrasensitive to ultraviolet (UV) light and tumor H2O2 for producing reactive oxygen species (ROS). Thereby, ZnFe2O4 can be used for photodynamic therapy (PDT) from direct electron transfer and the newly defined chemodynamic therapy (CDT) from the Fenton reaction. However, UV light has confined applicability because of its high phototoxicity, low penetration, and speedy attenuation in the biotissue. Herein, an upconversion-mediated nanoplatform with a mesoporous ZnFe2O4 shell was developed for near-infrared (NIR) light enhanced CDT and PDT. The nanoplatform (denoted as Y-UCSZ) was comprised of upconversion nanoparticles (UCNPs), silica shell, and mesoporous ZnFe2O4 shell and was synthesized through a facile hydrothermal method. The UCNPs can efficiently transfer penetrable NIR photons to UV light, which can activate ZnFe2O4 for producing singlet oxygen thus promoting the Fenton reaction for ROS generation. Besides, Y-UCSZ possesses enormous internal space, which is highly beneficial for housing DOX (doxorubicin, a chemotherapeutic agent) to realize chemotherapy. Moreover, the T2-weighted magnetic resonance imaging (MRI) effect from Fe3+ and Gd3+ ions in combination with the inherent upconversion luminescence (UCL) imaging and computed tomography (CT) from the UCNPs makes an all-in-one diagnosis and treatment system. Importantly, in vitro and in vivo assays authenticated excellent biocompatibility of the PEGylated Y-UCSZ (PEG/Y-UCSZ) and high anticancer effectiveness of the DOX loaded PEG/Y-UCSZ (PEG/Y-UCSZ&DOX), indicating its potential application in the cancer treatment field.
The newly defined chemodynamic therapy (CDT) may be a good method to enhance the efficiency of PDT, especially when mediated by a special material which can realize both therapies in a tumor microenvironment.18,19 It is known that solid tumors can produce abundant H2O2 (from 10 to 50 μM) because of the abnormal metabolism of tumor cells.20–23 Accordingly, CDT will employ the iron-initiated Fenton reaction to induce the apoptosis of tumor cells by transferring endogenous H2O2 into the highly toxic hydroxyl radical (˙OH). Thus, integration of PDT and CDT from the Fenton reaction to develop a ROS-mediated therapeutic nanoplatform is a promising method for enhancing the antitumor efficacy. Importantly, the irradiation of UV light has been acknowledged as a feasible strategy to improve the Fenton reaction.24–26
Among various materials, the spinel ferrite was chosen in this work on account of its narrow band gap, high stability, magnetic properties and promise for both PDT and CDT agents. Many research groups have done a lot of work on ferrite for cancer treatment.27–32 Recently, Zhang and co-workers successfully prepared copper ferrite nanoparticles with enhanced ROS production in the presence of a 650 nm laser.14 However, biotissues have higher absorptivity in the shorter-wavelength-light range, thus the 650 nm light has intrinsic drawbacks including limited tissue penetration depth and potential overheating issues. Similarly, for the UV-light-excited spinel ferrite, non-negligible problems of lower penetration depth, potential tissue damage and speedy attenuation still impose restrictions on its application in treating deep-seated tumor below the skin. In other words, it's urgent to find other light sources. Alternatively, it was revealed that near-infrared (NIR) light lying in the biological window (700–1000 nm) has the distinctive advantages of deep photon penetration, enhanced image contrast, and minimal damage to living organisms, all of which are quite essential for biomedical applications.33–38 Fortunately, lanthanide-doped upconversion nanoparticles (UCNPs) have made tremendous progress in photon upconversion, which provides an alternative way to transform longer wavelength NIR laser into shorter wavelength light (UV or Vis light).39–45 Thus, Yb3+/Tm3+-codoped UCNPs have been constructed to serve as an effective UV-Vis source in this article.46–48 Besides, Gd3+/Yb3+ co-doped nanoparticles have been certified as superb CT contrast agents thanks to their high atomic number and the strong X-ray attenuation of the dopants, which are of great significance for cancer diagnosis.49–52
Based on these analyses, for the first time, we have developed a multifunctional theranostic platform based on a yolk mesoporous nanostructure (Y-UCSZ) for multimodal therapy (PDT, CDT and chemotherapy) under the guidance of trimodal imaging, so as to attain tumor-specific enhanced antitumor efficacy and diagnosis. In this system, the NIR-excited and Yb3+/Tm3+-codoped UCNPs served as the UV-Vis source, in the place of direct UV radiation. The coated mesoporous ZnFe2O4 shell with a redox pair (Fe2+/Fe3+) can efficiently produce more virulent ˙OH through the Fenton reaction after absorbing UV light, realizing an excellent photo-enhanced CDT.14,26 As an effective photocatalyst, on the one hand, cytotoxic ˙OH can be produced by a photogenerated electron/hole pair of ZnFe2O4.53–57 On the other hand, the ZnFe2O4 nanoparticles converted oxygen into highly toxic 1O2 after absorbing UV light energy upon the irradiation of NIR light. Meanwhile, the yolk nanostructures with mesoporous shells and large cavities provide an excellent amount of DOX loading. And the nanocarriers can release DOX in response to the tumor microenvironment (chemotherapy), further enhancing the antitumor efficacy. For further biological applications, PEGylation endows the Y-UCSZ nanotheranostics with high biocompatibility, making them selectively accumulate in tumor regions via the enhanced permeability and retention effect (EPR).58,59 Hence, a superb in vivo synergistic therapeutic effect is then achieved after incorporating chemotherapy with PDT and CDT under the imaging-guidance (UCL, MRI, CT), suggesting its promising clinical application under the accurate observation of nanoparticles in tumor sites.
Fig. 1a–d exhibit the TEM photographs of β-NaGdF4:Yb,Tm, UCNPs, UCS and Y-UCSZ, respectively. As shown in Fig. 1a, the uniformity and monodispersity of NaGdF4:Yb,Tm particles were well maintained (mean diameter: 20 nm). Fig. 1b shows the TEM image of UCNPs, and the sample consists of discrete and uniform nanoparticles, and the average size is about 29.1 nm. Before the mesoporous silica shell coating, CTAB was used to modify UCNPs so as to obtain hydrophilic nanoparticles. The TEM photograph presented in Fig. 1c shows that the UCNPs@mSiO2 particles maintain good dispersity, and the size of UCPZ-PEG is about 42.1 nm. Afterward, a mesoporous ZnFe2O4 shell was further coated on the SiO2 shell through a facile hydrothermal method to obtain the yolk-structured nanoparticles (Y-UCSZ) with a mean size of 178.5 nm (Fig. 1d). X-ray photoelectron spectra (XPS) measurement was carried out to investigate the basic elements. The XPS measurement of Y-UCSZ in Fig. 1e demonstrates that the sample contains O, Zn and Fe elements, indicating that the ZnFe2O4 shell was coated on the UCS successfully. Fig. S1† exhibits two main peaks at 1022.4 and 1044.8 eV, which can be attributed to Zn 2p3/2 and Zn 2p1/2, respectively. Besides, the XPS spectra of Fe 2p treated with H2O2 are presented in Fig. 1f. The spectrum shows two main peaks at 723.9 and 710.5 eV, originating from Fe 2p1/2 and Fe 2p3/2 respectively, which are the typical oxidation states of iron in ZnFe2O4. Besides, there are four peaks at 709.1, 710.5, 711.6 and 714.3 eV, which can be assigned to Fe 2p3/2 after reacting with H2O2. According to a previous report, the peak at 709.1 eV could be attributed to Fe2+, and the other three peaks can be attributed to Fe3+. In particular, the ratio of Fe2+ and Fe3+ was calculated to be 0.21, indicating the occurrence of the Fenton reaction when treated with H2O2 and the radiation of 980 nm laser. Moreover, the EDS spectrum of Y-UCSZ in Fig. 1g describes the elemental composition of Y-UCSZ, directly certifying the successful synthesis of Y-UCSZ.
The XRD patterns of the NaGdF4:Yb,Tm, UCNPs, UCS, Y-UCSZ, the standard card of hexagonal β-NaGdF4 (JCPDS no. 27-0699) and ZnFe2O4 (JCPDS no. 22-1012) are displayed in Fig. 1h. The diffraction peaks of the as-fabricated NaGdF4:Yb,Tm and UCNP nanoparticles were consistent with the diffraction peaks of standard β-NaGdF4. In the XRD pattern of UCS, a new shoulder at 2θ = 22–28° apart from the representative peaks of UCNPs emerges from the silica coated on the UCNPs. Besides, the XRD pattern of Y-UCSZ can not only be fitted for the ZnFe2O4 phase (JCPDS no. 22-1012), but also be indexed to the normative β-NaGdF4 phase (JCPDS no. 27-0699), which demonstrates the successful synthesis of UCSZ.
The FT-IR spectra of UCNPs, UCS, Y-UCSZ and PEG/Y-UCSZ were observed to study the functional groups on the surface of nanoparticles, providing convincing results for the successful modification in every step. As displayed in Fig. 1i, the UCNPs capped with oleic acid display bands at 1463 and 1564 cm−1 associated with the vibrations of the carboxylic groups. And the intense transmission bands at 2854 and 2924 cm−1 derive from the asymmetric and symmetric stretching vibrations of –CH2. The peaks at 802 and 1088 cm−1 in the spectra of UCS are attributed to the vibration of Si–O–Si bands. After coating the ZnFe2O4 shell, the bands at 572 and 452 cm−1 can be assigned to the Fe–O and Zn–O bands, respectively.56 When the Y-UCSZ was modified with DA, an obvious peak at 1465 cm−1 in the spectrum is caused by the amino groups (–NH2–). The FT-IR spectrum of PEG/Y-UCSZ shows an obvious peak at 1638 cm−1, which is derived from the stretching vibrations of –CO–NH–. As for the PEG/Y-UCSZ&DOX sample, the new peaks at 1000–1800 cm−1 are caused by the loaded DOX (Fig. S2†). Zeta potentials of Y-UCSZ, DA/Y-UCSZ, and PEG/Y-UCSZ are exhibited in Fig. S3.† After reacting with DA, it can be obviously observed that the zeta potential changes from 4.62 to 20.3 mV, demonstrating the successful conjunction between DA molecules and Y-UCSZ nanoparticles. Afterwards, mPEG–COOH was utilized to connect the –NH2 from ZnFe2O4–DA with the corresponding potential of the samples transformed from 20.3 to −16.4 mV after PEGylation, implying that the surface modification is successfully achieved on the as-obtained Y-UCSZ. Besides, the size distributions of the samples in the different PEGylated steps were investigated by dynamic light scattering (DLS). As displayed in Fig. S4,† the sizes of the nanoparticles increase gradually in the process of PEGylation, demonstrating that the DA and mPEG–COOH connect to the Y-UCSZ nanoparticles successfully.
The upconversion emission spectra of β-NaGdF4:Yb,Tm, UCNPs, UCS, Y-UCSZ nanoparticles and UV-Vis absorption spectrum of ZnFe2O4 nanoparticles are shown in Fig. 2a. According to the theory, when combined with the energy receptor of the photosensitizer, the luminescent promoter would show a decline in the emission intensity. As displayed, there are apparent overlaps in the UV-Vis region of UCS and the absorbance peaks of ZnFe2O4. In particular, the UV-Vis emissions of UCNPs at 475 nm (1G4–3H6), 450 nm (1D2–3F4), 361 nm (1D2–3H6), and 345 nm (1I6–3H6) overlap with the UV-Vis absorption spectrum of ZnFe2O4. In comparison with UCS, after coating ZnFe2O4, the upconversion fluorescence intensity decreased remarkably in the UV-Vis region, implying that the UV radiation derived from UCNPs can be absorbed by the ZnFe2O4 shell to produce 1O2 and ˙OH. Besides, to further testify the energy transfer between UCS emission and Y-UCSZ upon the irradiation of a 980 nm laser, we investigated the emission decay curves of 1G4–3H6 (475 nm) in UCS and Y-UCSZ. As displayed in Fig. S5,† the markedly declined lifetime of Y-UCSZ compared to UCS (668.40 to 301.24 μs at 475 nm emission) demonstrates that the UV emission radiated from UCNPs can be efficiently absorbed by ZnFe2O4.
Hence, a key question whether the transferred energy could activate the ZnFe2O4 should be seriously investigated. In Fig. 2b, the relevant energy levels of Yb3+/Tm3+ coupled Y-UCSZ are exhibited to present the proposed energy transfer mechanism and the possible UV-Vis-driven reaction mechanisms for the production of ROS by ZnFe2O4 nanoparticles in the presence of UV-Vis light. When irradiated by UV-Vis light, electrons in the valence band (VB) of ZnFe2O4 can be photo-excited to the conduction band (CB) to produce electron–hole pairs. Then photogenerated holes (h+) in the VB of ZnFe2O4 can react with the surface-adsorbed H2O or OH− to generate the highly reactive ˙OH. H2O2 can seize the electrons to generate ˙OH simultaneously. Besides, the Fe3+ on the ZnFe2O4 shell can react with electrons in the CB to obtain Fe2+, and the Fe2+ can be recovered from Fe3+ efficiently upon the radiation of a UV laser. As a result, more Fe2+ can react with H2O2 to generate more toxic ˙OH upon the irradiation of UV light. Meanwhile, the ZnFe2O4 nanoparticles converted oxygen into the highly toxic 1O2 after absorbing UV light energy. As displayed in Fig. 2c, the absorbance of DPBF solution mixed with PEG/Y-UCSZ under the 980 nm laser irradiation for diverse times decreases gradually as time goes on at the wavelength of 350–460 nm, indicating the efficient generation of 1O2. As a comparison, the absorption intensity of DPBF solution without PEG/Y-UCSZ just shows a slight decline under the 980 nm laser irradiation for 10 min (Fig. S6a†), which implies that the NIR contributes to some extent to the production of 1O2. Besides, we studied the ˙OH-generating activity of PEG/Y-UCSZ with or without NIR irradiation further. Methylene blue (MB), which can be degraded by ˙OH, was used to monitor the generation of ˙OH. As given in Fig. 2d and e, a distinct decrease of absorbance was noticed when MB was incubated with PEG/Y-UCSZ under 980 nm laser irradiation, and when incubated with PEG/Y-UCSZ and different concentrations of H2O2, which can be ascribed to the production of ˙OH. Notably, the decline rate of MB absorbance in Fig. 2f is faster than those in Fig. 2d and e, which indicate that the PEG/Y-UCSZ nanoparticles have higher ˙OH generation efficacy in the presence of H2O2 and NIR radiation, owing to the collaboration between PDT and photo-enhanced Fenton reaction. No obvious change in the MB absorbance was observed when the MB solution alone was treated with NIR radiation (Fig. S6b†), which illustrates the influence of the 980 nm laser. In addition, to further testify the generation of ROS, DCFH-DA, which could be oxidized to DCF with a green fluorescence upon irradiation of a 488 nm laser, was employed to detect intracellular ROS. Fig. 2g exhibits the CLSM images of HeLa cells cultured with PEG/Y-UCSZ for 1, 3, 5 and 7 min as well as after reaction with DCFH-DA upon the radiation of a 980 nm laser. The intensity of green fluorescence increases markedly, which also demonstrates the significant ROS production of PEG/Y-UCSZ with 980 nm laser irradiation.
Electron paramagnetic resonance (EPR) was performed to testify 1O2 and ˙OH produced by Y-UCSZ nanoparticles (Fig. S7a and b†), using TEMP (0.15 M) and DMPO (0.03 M). According to a previous report, TEMP can react with 1O2 to produce 2,2,6,6-tetramethyl-4-piperidone-N-oxyl and result in an EPR pattern which consists of three lines with equivalent intensity. As shown in Fig. S7a,† the EPR spectrum was in accordance with the above features, indicating the production of 1O2. Besides, DMPO can specifically capture ˙OH and form a DMPO–OH spin adduct further, thereby giving rise to four resolved peaks (Fig. S7b†).64,65
The N2 adsorption/desorption isotherm and the relevant pore-size distribution of Y-UCSZ are presented in Fig. 3a and b. As exhibited, Y-UCSZ shows a representative type IV isotherm, indicating the mesoporous structure of the nanoparticles. The Brunauer–Emmett–Teller (BET) surface area of the sample is measured to be 198.98 m2 g−1 with a high pore volume of 0.62 cm3 g−1 and corresponding average pore size of 6.88 nm. Notably, the nanoparticles with mesopores and large surface area are beneficial to load the chemotherapy drug DOX. Although the final sample (PEG/Y-UCSZ&DOX) still possesses a mesoporous structure, the BET surface area is reduced to 34.16 m2 g−1 coupled with a pore volume of 0.20 cm3 g−1 (Fig. S8a†), owing to that the DOX molecules are loaded into the mesoporous channels. Fig. 3c and d display the normative curve of DOX observed at 480 nm and the absorption spectra of the DOX solution before and after the loading procedure employing PEG/Y-UCSZ nanoparticles. Based on the Lambert–Beer law, the DOX loading rate of PEG/Y-UCSZ was calculated to be as high as 70.87% according to the standard curve and the absorbance intensity of DOX solution. Particularly, the UV-Vis absorption spectrum of PEG/Y-UCSZ&DOX has a distinct absorption peak consistent with the one of DOX in the range of 430 to 560 nm (Fig. S8b†), indicating that DOX is successfully loaded onto the nanoparticles. As reported, the tumor microenvironment has a higher temperature and lower pH value compared with normal tissue cells, which is caused by its abnormal metabolism. Herein, the tumor microenvironment-responsive release properties were investigated. As displayed in Fig. S9a,† PEG/Y-UCSZ&DOX shows a temperature-responsive drug release, exhibiting a positive increase with increasing temperature. The DOX release was also investigated by diluting PEG/Y-UCSZ&DOX in PBS with various pH values (Fig. S9b†). It can be noticed that the DOX release at 25 °C is about 8.6%, whereas the release rate respectively increases to 17.2% and 25.5% at temperatures of 37 and 50 °C. In addition, the drug release displays a much intensive effect in an acidic environment at 37 °C (Fig. S9c†). When the temperature is 37 °C and the pH value is 7.4, the release rate within 24 h is just 14.9%, while the release rate is as high as 36.6% at a pH value of 6.5, indicating that there is a distinct pH responsive release course.
It is necessary to verify the cellular uptake behavior of the synthetic nanodrugs before in vitro anticancer application. Herein, the PEG/Y-UCSZ&DOX nanoparticles were added to the culture medium incubated with HeLa cancerous cells for 0.5, 1, and 3 h at 37 °C, and the corresponding CLSM photographs are shown in Fig. 4a. DAPI, an organic dye that can emit blue light in the presence of a 488 nm laser, was employed to mark the cell nuclei. And the DOX loaded in the nanoparticle radiates red emission upon the radiation of a 488 nm laser. Accordingly, the overlay photographs of the above two channels are exhibited. As displayed, there is only feeble red fluorescence in the first 0.5 h, demonstrating that only a small amount of PEG/Y-UCSZ&DOX has been swallowed by cells. With increase in incubation time, the intensity of the red signal becomes enhanced, indicating that more nanoparticles are located in the cells. The above results prove that the as-synthesized nanoparticles can be easily internalized by HeLa cells.
The upconversion luminescence radiated by PEG/Y-UCSZ nanoparticles could be employed to monitor the location of the nanodrug in the cells (Fig. 4b). To conceivably prove the phagocytosis of particles, PEG/Y-UCSZ nanoparticles were allowed to react with HeLa cells for 0.5, 1, and 3 h, respectively. As shown, the intensity of the blue emission shows positive enhancement with increase in the incubation time, which implies that the nanoparticles were swallowed by cells. In particular, the blue upconversion fluorescence is derived from PEG/Y-UCSZ NPs excited by the 980 nm laser. Significantly, most of the UCL signal is observed at the intracellular area, indicating that the nanoparticles have been internalized into the cells rather than just adhering to the surface of cell membranes. These results indicate that the PEG/Y-UCSZ nanoparticles are promising UCL imaging contrast agents with a negligible background.
As accepted, the CT imaging technology can provide details of high-resolution three dimensional structures and deep tissue penetration. Besides, nanomaterials with lanthanide doping have been extensively studied for X-ray attenuation owing to the high atomic number of lanthanide elements. In this research, the in vitro and in vivo CT imaging properties of the Gd3+/Yb3+ doped PEG/Y-UCSZ sample were studied. As exhibited in Fig. 5a, when the concentrations of PEG/Y-UCSZ are boosted, the attenuation of X-ray increases markedly. Additionally, in Fig. 5b, the CT values show a linear dependence on sample concentrations, and the corresponding slope is calculated to be 56.009. To investigate the in vivo CT imaging performance of PEG/Y-UCSZ, the tumor-bearing mice without and with PEG/Y-UCSZ injection were imaged using a CT imaging instrument. Obviously, the tumor site without sample injection has a much lower CT value (52.5 HU, Fig. 5c) than the tumor site with injection (395.4 HU, Fig. 5d). Furthermore, the CT value profiles on the cross-sectional line of the tumor sites were investigated, and the corresponding results are displayed in Fig. 5e and f. Obviously, the CT value of the experimental group shows a fluctuation compared with the straight line of the control group. All of these results demonstrate that the PEG/Y-UCSZ nanoparticles can be employed as an efficient CT imaging contrast agent. According to previous reports, the Fe3+ and Gd3+ ions show positive enhancing capabilities of the T2 MRI signal,26,66 so we envisage that the integration of the ZnFe2O4 shell and the NaGdF4-based UCNPs can achieve a superior T2 MRI imaging outcome. Herein, the T2-weighted MRI effect of PEG/Y-UCSZ dispersed in PBS was investigated. As shown in Fig. 5g, the T2-weighted images demonstrate a clear concentration-dependent darkening efficacy. In Fig. 5h, the measured intensity of the r2 (1/T2) signal exhibits a linear increase with the total concentrations of Fe3+ and Gd3+ changing from 0 to 4 mM, with a high transverse relaxivity (r2) of 45.094 mM−1 s−1. In other words, the PEG/Y-UCSZ can generate the MR contrast on a transverse photon relaxation-time-weighted sequence to effectively shorten the T2 relaxation time. Afterwards, the in vivo T2-weighted MRI effect of PEG/Y-UCSZ nanoparticles was studied. As shown in Fig. 5i and j, there is an obvious T2-MR signal attenuation effect for the tumor with sample injection compared with the tumor without injection, indicating the great promise of PEG/Y-UCSZ as a T2 MRI contrast agent.
As acknowledged, the biocompatibility of the as-obtained nanoparticles ought to be firstly evaluated before actual application. The viabilities of L929 cells after incubating with PEG/Y-UCSZ at different concentrations for 12 and 24 h are exhibited in Fig. 6a. The sample displays a high viability of 86.5–88.7% in the overall concentration limit even at 500 μg mL−1 after 24 h incubation, implying that the nanosystem has low toxicity. Besides, as displayed in Fig. 6b, the in vitro cytotoxicity of NIR, PEG/Y-UCSZ + NIR, PEG/Y-UCSZ&DOX and PEG/Y-UCSZ&DOX + NIR against HeLa cells was assessed by MTT measurement. In order to compare the anticancer effects of the obtained nanodrugs, the HeLa cells were subjected to different conditions and then cell viabilities were quantitatively measured employing the MTT method. The cell viability radiated with the 980 nm laser demonstrates that the 980 nm light displays no obvious toxicity to the cells. After PEG/Y-UCSZ incubation and then 980 nm laser irradiation, numerous HeLa cells are killed with clearly lower viability than that treated with NIR radiation only, owing to the coupling of PDT with a small Fenton effect. In addition, the viabilities of PEG/Y-UCSZ and NIR laser treated group are higher than those in the PEG/Y-UCSZ&DOX treated group, suggesting a PDT and photo-enhanced CDT effect. Obviously, the PEG/Y-UCSZ&DOX and 980 nm laser treated group shows the lowest cell viabilities, which indicates that the yolk-structured PEG/Y-UCSZ&DOX could actively collaborate PDT and CDT with chemotherapy to achieve the best therapeutic effect. In order to testify the cell-killing efficacy of various treatments, propidium iodide (PI), which can precisely dye dead cells with a red color, was used to differentiate cancerous cells (Fig. 6c). The results are well consistent with the above MTT anticancer assay. Especially in PEG/Y-UCSZ&DOX and NIR treated group, almost all cells are dead, implying the highest cancer killing effect of PEG/Y-UCSZ&DOX with NIR irradiation. Furthermore, the hemolysis results of PEG/Y-UCSZ are displayed in Fig. S10.† Inappreciable hemolysis can be observed with the highest hemolytic rate of about 5.03%, indicating mild toxicity to the normal cells of PEG/Y-UCSZ nanoparticles.
Inspired by the aforesaid in vitro therapy results, female mice were implanted with a U14 tumor xenograft and then subjected to in vivo therapeutic experiment. In particular, the tumor-bearing mice were treated under various conditions: control; NIR; PEG/Y-UCSZ + NIR, PEG/Y-UCSZ&DOX, and PEG/Y-UCSZ&DOX + NIR. The tumor size was recorded every two days after the initial treatment. As displayed in Fig. 7a, the relative tumor volumes (V/V0) are then drawn as a function of treated time. The tumor growth in mice exposed to the 980 nm laser was slightly inhibited over two weeks of treatment, possibly owing to the heat effect caused due to the absorbance of laser irradiation by hemoglobin. At the same time, the mice injected with the PEG/Y-UCSZ nanoparticles upon the radiation of 980 nm laser display a much smaller tumor size than the NIR-irradiated group, which may be caused by the PDT effect and photo-enhanced performance of PEG/Y-UCSZ. The tumor growth on PEG/Y-UCSZ&DOX treated mice is restrained to some extent after two weeks, which may be caused by the chemotherapy effect of DOX and a small Fenton effect. Especially, the mice treated with PEG/Y-UCSZ&DOX injection and NIR irradiation have the highest anticancer efficacy among all the groups, perhaps due to the superior therapy effect of the synergistic cooperation between PDT and chemotherapy. Besides, the weights of excised tumors corresponding to the mice belonging to the various treatment groups are displayed in Fig. 7b, directly demonstrating the high inhibition efficacy of the nanoparticles. To explain the potential toxicity in vivo more clearly, the pictures of representative mice and excised tumors also show that the tumor size treated with PEG/Y-UCSZ and NIR radiation was the smallest as shown in Fig. 7c, which illustrates that it has the greatest antitumor effect among different experimental groups. The experimental results are well consistent with the in vitro cell experiments. As shown in Fig. 7d, H&E stained photographs of tumor sections testify that the group treated with the PEG/Y-UCSZ injection and NIR irradiation shows the highest degree of tumor damage. H&E stained photographs of the major organs including heart, liver, spleen, lung and kidney are presented in Fig. S11.† The normal organs in five groups show no obvious damage, implying the high in vivo biocompatibility of PEG/Y-UCSZ&DOX.
Footnote |
† Electronic supplementary information (ESI) available: XPS spectra of typical elements Zn 2p; FT-IR spectra of the DA/Y-UCSZ and DOX loaded PEG/Y-UCSZ samples; the changes of zeta potentials for nanoparticles obtained at each PEGylated step; decay curves for 1G4–3H6 emission (475 nm) of Tm3+ in UCS, Y-UCSZ; EPR spectra of 1O2 and ˙OH in the PEG/Y-UCSZ aqueous solution; DOX release efficiency from PEG/Y-UCSZ&DOX in PBS at varied temperatures and pH values; the hemolytic percentage of PEG/Y-UCSZ in human red blood cells; H&E stained images of liver, lung, kidney, heart and spleen obtained from different groups after 14 days treatment. See DOI: 10.1039/c9sc00387h |
This journal is © The Royal Society of Chemistry 2019 |