FePt nanoparticles as a potential X-ray activated chemotherapy agent for HeLa cells
Authors Zheng Y, Tang Y, Bao Z, Wang H, Ren F, Guo M, Quan H, Jiang C
Received 12 May 2015
Accepted for publication 5 August 2015
Published 22 October 2015 Volume 2015:10(1) Pages 6435—6444
Checked for plagiarism Yes
Review by Single anonymous peer review
Peer reviewer comments 4
Editor who approved publication: Dr Lei Yang
Yanhong Zheng,1 Yunlan Tang,2 Zhirong Bao,1 Hui Wang,1 Feng Ren,1 Mingxiong Guo,2 Hong Quan,1 Changzhong Jiang1
1Key Laboratory of Artificial Micro- and Nano-structures of the Ministry of Education and Center for Electronic Microscopy and Department of Physics, Wuhan University; 2College of Life Sciences, Wuhan University, Wuhan, People’s Republic of China
Abstract: Nanomaterials have an advantage in “personalized” therapy, which is the ultimate goal of tumor treatment. In order to investigate the potential ability of FePt nanoparticles (NPs) in the diagnosis and chemoradiotherapy treatment of malignant tumors, superparamagnetic, monodispersed FePt (~3 nm) alloy NPs were synthesized, using cysteamine as a capping agent. The NPs were characterized by means of X-ray diffraction; transmission electron microscopy, Physical Property Measurement System, and Fourier transform infrared spectroscopy. The cytotoxicity of FePt NPs on Vero cells was assessed using an MTT assay, and tumor cell proliferation inhibited by individual FePt NPs and FePt NPs combined with X-ray beams were also collected using MTT assays; HeLa human cancer cell lines were used as in vitro models. Further confirmation of the combined effect of FePt NPs and X-rays was verified using HeLa cells, after which, the cellular uptake of FePt NPs was captured by transmission electron microscopy. The results indicated that the growth of HeLa cells was significantly inhibited by FePt NPs in a concentration-dependent manner, and the growth was significantly more inhibited by FePt NPs combined with a series of X-ray beam doses; the individual NPs did not display any remarkable cytotoxicity on Vero cells at a concentration <250 µg/mL. Meanwhile, the FePt NPs showed negative/positive contrast enhancement for MRI/CT molecule imaging at the end of the study. Therefore, the combined results implied that FePt NPs might potentially serve as a promising nanoprobe for the integration of tumor diagnosis and chemoradiotherapy.
Keywords: superparamagnetism, MRI/CT, chemoradiotherapy, intelligent nanoprobe
Cancer is the world’s foremost medical problem, with the number of new cases and cancer-related deaths showing a disturbing increase. In 2012, the People’s Republic of China was recorded as the country having the highest number of newly confirmed cancer cases.1 The past decade has seen improvements in the efficacy of tumor diagnosis and therapy, with treatment no longer limited to a single modality.2–6 While it has become more common to use dual-modal diagnosis and treatment, such as computed tomography/ magnetic resonance imaging (CT/MRI) with chemoradiotherapy and postsurgery radiotherapy, novel nanomaterials applied to medical science are regarded as promising agents for tumor diagnosis and therapy. Specifically, not merely nanocarriers used for drug delivery, but also noble metal and metal oxide nanoparticles (NPs) have revealed their potential in single-modality tumor diagnosis and treatment.7–11 However, tumor treatment faces challenges such as imaging location and complications (radiodermatitis, radiation pneumonia, organ failure, etc). While traditional drug treatments and single-modality nanomaterials are unable to solve these problems, multi-modality agents may promote advancement and reduce adverse side effects of each therapeutic modality. Therefore, the study and exploration of multifunctional nanomaterials for combined various therapeutic modalities of tumor diagnosis and treatment is one of the most urgent affairs in medical research.
It is well known that there are three typical therapeutic methods for tumor diagnosis and treatment: chemotherapy, radiotherapy, and surgery.12 Although they are very useful methods for tumor therapy, they are still limited by several challenges and side effects. For example, surgery cannot always remove a tumor growing near vital organs, most agents used in chemotherapy are also toxic to normal organs and tissues, and radiotherapy cannot distinguish normal cells from tumor cells, thus resulting in complications. Naturally, combination therapy is increasing in popularity in clinical tumor treatment, as it combines the advantages of each of the various therapies, while avoiding the side effects. Nevertheless, the problem with combination therapy is that more drugs are used, and there are still rare agents can function throughout the whole process of combination therapy. Therefore, the research of multifunctional agents for combination therapy is very important and clinically significant. Specifically, the concurrent implementation of chemotherapy and radiotherapy, which is called chemoradiotherapy, has been regarded as an important therapy exemplification in the treatment modality for solid tumors over the past several decades.13–16 Compared with either chemotherapy, radiotherapy or sequential treatment, chemoradiotherapy has not only displayed the ability to consistently local tumor control, but also improve the curative ratio of cancer without surgical operation.13,17 In spite of the significant success that has been achieved, chemoradiotherapy is limited by its additional toxicity. Moreover, the prescription dose of radiation has not been reduced in chemoradiotherapy processes, which may damage normal tissues and organs.18 Therefore, there is an urgent need to improve the therapeutic gain factor of chemoradiotherapy. Promisingly, NPs possess several unique properties. Their excellent high X-ray absorption, control of drug release, enhancement of drug permeability, and retention effect leading to high NP concentration in tumor cells, make them strongly suitable for the improvement of chemoradiotherapy. Additionally, the magnetic properties of NPs could play important roles in tumor imaging contrast enhancement.19–21 Sun et al22 were the first to report the synthesis and characterization of monodisperse FePt NPs. Since then, FePt alloy NPs have attracted much attention due to their fascinating potential in the biomedical science field.23–26 For example, the abilities of NPs to inflict DNA damage in tumor cells, and catalyze oxygen reduction reaction make the NPs of great value in suppressing proliferation of tumor cells.27–29 Furthermore, compared to several commercial MRI/CT contrast agents, the superparamagnetic properties and X-ray absorption abilities of FePt NPs make them potential in vitro and in vivo dual-modality contrast agents (after surface engineering with functional molecules).30–33 Based on the extremely high X-ray mass absorption coefficient of Pt, the hypothesis of the current study was that the NPs may increase the absorbed external beam dose in tumors, with decreased absorption of radiation in normal tissue and organs. Therefore, FePt NPs could be the precursor for CT, MRI, chemotherapy and radiotherapy all within one single agent, acting as a kind of multifunctional nanomedicine.34
In this work, the possibility of using superparamagnetic FePt alloy NPs as CT/MRI dual-modal imaging contrast agents and aforementioned chemoradiotherapy improvement is presented. FePt NPs were synthesized by using a chemical reduction method at a low temperature, and surface coating with cysteamine (Cys) to isolate the amine group for further target material conjugation. The characterizations of the NPs were performed by X-ray diffraction (XRD), transmission electron microscopy (TEM), Fourier transform infrared spectroscopy (FTIR), and comprehensive Physical Property Measurement System (PPMS). After the in vitro cytotoxicity of the NPs was evaluated using Vero cells, the growth inhibition effect of FePt NPs was evaluated by a 5-dimethylthiazol-2-yl-2,5-diphenyl tetrazolium bromide (MTT) assay using HeLa cells with and without X-ray beam. Finally, the NPs’ ability for medical imaging enhancement was measured by MRI/CT. The results indicated that the FePt NPs have potential as multimodality nanomedicine agents, in regard to the diagnosis and treatment of cancerous tumors.
Materials and methods
Analytically pure chloroplatinic acid (H2PtCl6) (Reagent No 1 Factory Of Shanghai, Chemical Reagent Co., Ltd., Shanghai, People’s Republic of China), 98% iron acetylacetonate (Aladdin Industrial Corp.®, CA, USA), Cys (Sigma-Aldrich Co., St Louis, MO, USA) were used in this research. Sodium borohydride (96%), ethanol (analytically pure), anhydrous ethanol (analytically pure), ethylene glycol (analytically pure) were purchased from Sinopharm Chemical Reagent Co., Ltd, Shanghai, People’s Republic of China.
Synthesis of FePt NPs
FePt NPs were prepared by using a chemical reduction method. Briefly, 1.5 mL oleylamine, 1.5 mL oleic acid, 0.1363 g iron acetylacetonate, and 100 mL anhydrous ethanol were mixed into three-necked round-bottomed flasks after 30 minutes of magnetic stirring. Twenty milliliters of H2PtCl6·6H2O–alcohol solution (0.0193 mmol/L) were transferred to the flask. Subsequently, 200 mL sodium borohydride–alcohol solution (0.0657 mmol/L) was gradually added after 30 minutes of magnetic stirring with argon flow. The mixture was heated to 40°C and stirred with argon flow for 1 hour. The black product was precipitated out by centrifugation (10,000 rpm for 6 minutes), and then dried in a vacuum for 48 hours at 40°C, after which, FePt NPs were obtained.
Dry FePt NPs (10 mg) were dissolved in ethyl alcohol by sonication. Cys (~100 mg) was added into this solution and dissolved by sonication at 30°C. This mixture was sonicated for 6 hours at 40°C. The unconnected ligand in solution was then washed away by ethyl alcohol. Finally, the surface-coated FePt NPs were collected, and stored in a bottle filled with N2.
FePt NPs characterization
The formation and the phase structures of the samples were identified by powder XRD on a Bruker D8/Advance-X ray Diffractometer (Bruker Corporation, Billerica, MA, USA), using Cu Kα radiation (λ=1.5406 Å). The morphology, the phase structure, and the degree of dispersion of the samples were observed on an EM2010FEF-Ω transmission electron microscope (JEOL, Tokyo, Japan). FTIR spectra were recorded and the ligand attachment was verified by the Nicolet 5700 FTIR Spectrometer. The magnetic properties of the samples were measured by PPMS (Quantum Design, Inc., San Diego, CA, USA). The measurements between −10,000 and 10,000 Oe at 300 K were chosen.
Cell culture and treatment
The Vero cell line and HeLa cell line (both purchased from the Type Culture Collection of the Chinese Academy of Sciences, Shanghai, People’s Republic of China) were both maintained in Minimum Essential Medium (Thermo Fisher Scientific, Waltham, MA, USA) which contained 10% fetal bovine serum (Thermo Fisher Scientific, Waltham, MA, USA), 100 units penicillin mL−1, and 100 μg streptomycin mL−1 (Beyotime Biotechnology, Shanghai, People’s Republic of China) in a 37°C incubator (Thermo Fisher Scientific Waltham, MA, USA) with 5% CO2.
Cytotoxicity assay on Vero cells
Vero cells were seeded in 96-well plates for 24 hours, with 1.2×104 cells in each well. A series of FePt–Cys NPs were dispersed in the cells, with final concentrations of 12.5, 25, 125, and 250 μg/mL for an additional day. Survival fraction was measured by the MTT assay. After all the cells were treated, 20 μL MTT (20 mg/L) were placed into each well for 4 hours at 37°C. Finally, 150 μL dimethyl sulfoxide (DMSO) was added to each well, and the 96-well plates were shaken for 10 minutes. A microplate reader (Thermo Fisher Scientific Waltham, MA, USA) was used to determine the absorbance values at 590 nm.
Combined FePt treatment and external beam radiation dose response on HeLa cells
The HeLa cell line was cultured in 96-well plates, with 2.5×103 cells in each well. After 24 hours, a series of FePt–Cys NPs were added into each well, with final concentrations of 0, 25, 50, and 100 μg/mL. Two hours later, the groups of HeLa cells were irradiated with 0, 2, 4, 6, 8, and 10 Gy 6 MV photon beams, respectively, using the Varian Clinac® iX Linear Accelerator (Varian Medical Systems, Palo Alto, CA, USA) at the Zhongnan Hospital of Wuhan University, Wuhan, Hubei, People’s Republic of China. Following incubation of the cells at 37°C for 72 hours, an MTT assay was used to measure the cell viability. The two experiment groups were then prepared for measurement of their interactive effect by injecting 0, 12.5, 25, and 50 μg/mL FePt–Cys NPs before and after 2 Gy X-ray beam irradiation. After the cells were incubated for 72 hours, the MTT assay was used to collect the data. All data were expressed as mean ± standard deviation, and a two-way analysis of variance (ANOVA) and a Student’s t-test.
HeLa cells were incubated with 25 μg/mL FePt–Cys NPs for 24 hours. After the medium had been removed, 2.5% glutaraldehyde and 1% osmic acid were added to fix the cells. Subsequently, the dehydration of cells was performed by the serial addition of ethanol (30%, 50%, 60%, 70%, 80%, and 90% concentrations), and the embedding of cells was achieved using EPON812. The cells were then polymerized in an oven at 60°C for 24 hours. The cells were sliced (~100 nm thick) using a diamond knife on a Leica ultramicrotome (Leica Microsystems, Wertzlar, Germany), and placed onto a copper grid. Images were captured by TEM.
MRI and CT imaging in vitro
A column of centrifuge tubes which contained 0.01–100 mmol/L FePt NPs and a phosphate buffer saline (PBS) control was used for MRI and CT contrast imaging. T2-weighted three-dimensional spin echo sequences for in vitro MRI (MAGNETOM Trio Tim 3.0T, Siemens, Munich, Bavaria, Germany) were performed at the Hospital of Wuhan University, Wuhan, Hubei, People’s Republic of China, and used the following parameters: a repetition time of 550 milliseconds, an echo time of 15 milliseconds, a flip angle of 15°, a slice thickness of 1.5 mm, and a matrix of 256×196 pixels. The CT imaging (Sensation Cardiac 64x, Siemens, Munich, Bavaria, Germany) parameters were as follows: slice thickness, 3 mm; 120 kvp, 80 mA; filed, 512×512; gantry rotation time, 0.3 second; table speed, 30 mm/rotation.
Characterization of FePt NPs
Figure 1A shows the XRD patterns of the FePt NPs. Compared to the powder diffraction file standard card, all four characteristic peaks of the chemically-disordered, face-centered cubic structure of FePt were clearly identified in the curve, which had planes of (111), (200), (220), and (311), respectively.27,28 No other characteristic peak of iron oxide or pure Pt was found in the powder XRD. Interestingly, as the values calculated from broader XRD by the Debye–Scherrer formula usually suggests smaller sizes, the XRD scan was in line with the size of FePt NPs calculated from the TEM images.35 The TEM images of FePt NPs are shown in Figure 1B. The average size of FePt NPs was 3.11±0.53 nm. This size was calculated by averaging the sizes of 100 NPs; size distribution is shown in Figure 1C. The FePt NPs appeared to have globose-shaped nuclei (ultimately determined to be cuboctahedral when visualized with high-resolution TEM).25 The TEM images showed no agglomeration, which suggests the excellent monodispersity of FePt NPs because of two reasons: 1) a low reaction temperature (40°C), and 2) the negatively-charged surface resulting in the interparticle repulsive force.35 Figure 1D shows that the saturated mass magnetization of FePt NPs was 1.13 emu/g, coupled with the absence of coercive force, which indicated that the FePt NPs exhibited superparamagnetic behavior at 300 K.36 The ligand exchange was confirmed by FTIR measurements in the range of 400– 4,000 cm−1 with 2 cm−1 resolution at room temperature. The recorded spectrums of bare FePt NPs, Cys, and Cys-capped FePt NPs are shown in Figure 1E. The absorption peak of ~3,425 cm−1 was assigned to the N–H stretching vibration. The vibration of the C–H bond corresponded to the absorption peak at ~3,025 cm−1. The S–H bond vibration absorption peak at ~2540 cm−1 disappeared on the spectrum of FePt-Cys, and at the fingerprint region (1300–900 cm−1) the FePt-Cys spectrum shows many different from the other two; this suggests that the Cys molecules were connected to the surface of FePt NPs by the coordinate bond between S and Pt atoms, which have high affinity for each other.37
Cytotoxicity assay on Vero cells
The in vitro cytotoxicity of Cys-capped FePt NPs was evaluated in the Vero cell line using the MTT assay with a series of different concentrations. The cell viability after incubation for 24 hours is shown in Figure 2. The original data of concentrations 12.5, 25, and 125 μg/mL FePt–Cys NPs did not show a significant difference when compared to the control group of the Vero cells, and this is reflected in the cell viability (almost 100%) illustrated in Figure 2. When the concentration of FePt NPs was raised to 250 μg/mL, the Vero cells showed only a ~14% loss of cell viability. These results indicate that FePt NPs have no significant cytotoxicity on Vero cells in vitro at concentrations below 250 μg/mL.
Figure 2 Cell viability of Vero cells treated with FePt NPs.
Combined FePt therapy and external beam radiation dose response on HeLa cells
In order to assess the ability of FePt–Cys NPs with or without X-ray beams on cell inhibition of HeLa cells, HeLa cells were cultured with FePt–Cys NPs irradiated by serial doses of X-ray beams. As shown by the data displayed in Figure 3, the survival rates of HeLa cells were significantly suppressed by FePt–Cys NPs without irradiation, in a concentration-dependent manner, in the range of 25–100 μg/mL. For example, the cell viability of the group treated with 25 μg/mL FePt–Cys NPs and irradiated by 2 Gy X-ray beams showed no significant difference to that of the group treated with 100 μg/mL FePt–Cys NPs only; this was slightly lower than that of the groups irradiated by 8 Gy or 10 Gy X-Ray beams. Therefore, the results suggest that FePt–Cys NPs can not only inhibit the growth of HeLa cells in a concentration-dependent manner, but also show a combination effect with X-rays to suppress the proliferation of HeLa cells more remarkably. By comparison, HeLa cells seemed to be more sensitive to the NPs than Vero cells.
Figure 3 The growth inhibition of HeLa cells treated with FePt NPs combined with X-ray beams.
To further confirm the existence of the potential interaction effects between FePt–Cys NPs and X-ray, FePt–Cys NPs were injected into the wells cultured with HeLa cells pre or postirradiation, and all the experiment groups were irradiated by the 2 Gy X-ray beam. As shown in Figure 4, cell viabilities of the group that only received irradiation remained consistent. Once NPs were injected at 2 hours pre- or postirradiation, cell viabilities showed ~5%, ~9%, and ~10% differences between the two kinds of group at 12.5, 25, and 50 μg/mL concentrations of the FePt–Cys NPs, respectively. Therefore, all the cellular results demonstrate that FePt–Cys NPs not only remarkably inhibited the cell proliferation of HeLa cells, but also had combination effects with X-ray beams to suppress the proliferation of HeLa cells.
Figure 4 The growth inhibition of HeLa cells treated with FePt NPs before and after 2 Gy X-ray irradiation.
The cellular uptake of FePt NPs by HeLa cells was captured by TEM. As shown in Figure 5, the vesicles containing black FePt NPs were observed, proving the direct cellular internalization of the FePt NPs. The left side of Figure 5A shows that HeLa cells, the initial phase, and during the formation of the vesicles absorbed the black FePt NPs. The release and diffusion of the vesicle-wrapped FePt NPs into the cytoplasm are shown in the right side of Figure 5A. As can be seen at the bottom of Figure 5C, the FePt NPs were penetrating the membrane of cellular nuclei. The right sides of Figure 5A and D shows that the pathway of NPs is a kind of endocytosis called macropinocytosis.
MRI and CT image in vitro
The in vitro T2-weighted MRI images of various FePt concentrations were captured by a 3T MR imager, and the calculated intensity of each tube compared to that of the PBS tube was normalized, as shown in Figure 6. The 100 mM FePt tube presented the most effective negative MR contrast enhancement, with a signal intensity decrease of ~40%. Overall, as shown by the MRI, FePt NPs demonstrated an excellent inverse contrast in vitro in a concentration-dependent manner. The in vitro CT imaging was examined at various FePt concentrations, and the positive contrast effects of the NPs were certified by these results. The calculated CT value of each tube was pointed and plotted, and shown in Figure 6B, with the CT value of PBS set to 0. In accordance with the results of the MRI, the 100 mM FePt tube exerted the most effective positive CT contrast enhancement. Overall, the FePt NPs displayed contrast enhancement in the CT in vitro in a concentration-dependent manner.
To date, it has been reported that FePt alloy NPs significantly inhibit the growth of tumor cells (such as U87, H4, HeLa, A2780, A431, Sk-Br3, and HEK-293) by acting as yolk in a yolk-shell nanocrystal, coated with phospholipid or other chemical compounds.35,38–41 Furthermore, in the area of medical imaging, FePt NPs are considered to have great potential in MRI and MRI/CT dual-model imaging as a regenerative medicine.31,33 However, we confirm that there is still a paucity of research on FePt NPs in the radiotherapy field, in which the NPs may hold potential. The current study reports the synthesis of 3.11±0.53 nm monodispersed FePt NPs by a chemical reduction method, and the coating of these NPs with Cys. The potential applications of NPs in chemoradiotherapy and medical imaging contrast enhancement were studied in HeLa cells exposed to a 6 MV photon beam, and by MRI/CT imaging system in vitro, respectively. The results proved that FePt NPs inhibited the growth of HeLa cells in a concentration-dependent manner, and when the NPs and X-ray beams were combined, the growth inhibition of HeLa cells varied remarkably compared to that treated by NPs or X-rays alone. The results further confirmed the existence of the potential interactive effect between FePt NPs and X-ray beams, and demonstrated the positive and negative imaging contrast enhancement of CT and MRI by FePt NPs. Compared to cisplatin, a kind of traditional anticancer platinum complex, FePt NPs could damage HeLa cells alternatively between HeLa and Vero cells, due to the acid-based environment intracellular. Therefore, collectively, these results could be the definitive backup to endorse FePt NPs as potential novel nanoprobes for the integration of diagnosis and chemoradiotherapy on HeLa cells. The results displayed in Figures 2 and 3 indicate that the FePt NPs show significant cytotoxicity on HeLa cells, while not significantly suppressing the proliferation of Vero cells at a concentration below 250 μg/mL. Previously, Xu et al38 suggested that FePt NPs showed the controlled release in a low pH solution, while there was little degradation of FePt NPs in a solution of pH 7.4. Gao et al29 indicated that, in HeLa cells, the FePt cores of FePt@CoS2 were oxidized and degraded in secondary lysosome with a low-pH environment. Therefore, the current study speculates that the low pH environment may promote the degradation of FePt NPs, triggering the release of ions to damage tumor cells, either directly or indirectly, while few free ions are released in normal cells. To achieve a more effective specific suppression, further studies of engineering the surface of FePt NPs are needed, and are currently in progress. As shown in Figures 3 and 4, FePt NPs inhibited the growth of HeLa in a concentration-dependent manner without irradiation, and the suppression ratios remarkably increased when FePt NPs were combined with irradiation. These results suggested that the NPs not only acted as a chemosensitization agent, but also performed as a radiosensitizer under the environment of irradiation. What was of most interest in the current study was that the low concentration of FePt NPs combined with low-dose X-ray exposure suppressed the proliferation of HeLa cells more significantly than the separate high-dose X-ray beaming on HeLa cells (Figure 3). In other words, the utilization of FePt NPs in chemoradiotherapy may sensitize tumor cells on the one hand, and reduce the required radiation dose on the other. Meanwhile, the FePt NPs showed little cytotoxicity on Vero cells at low concentration. Therefore, the results suggested that FePt NPs may potentially increase the therapeutic gain factor through radiosensitizing, chemosensitization, and reducing the dose absorbed by normal cells. According to the above discussion, the as-synthesized FePt NPs may play a role in the chemoradiotherapy in vitro model as simple but efficient nanoprobes. Their mechanism of cellular action manifested itself in several ways.10,42,43 First, as the FePt NPs were superparamagnetic and water-soluble after surface capping with Cys, the signal intensity of MRI/CT images were negatively/positively enhanced in a concentration-dependent manner (Figure 6). This phenomenon may help to improve the accuracy of tumor location, especially helpful for the location of isolated tumor cells, which have already infiltrated normal tissues and may be the important cause of tumor recurrence. Second, the results showed that FePt NPs suppressed the proliferation of HeLa cells in a concentration-dependent manner as a chemotherapy agent. In order to investigate the damage mechanism caused by FePt NPs, the cellular uptake of FePt NPs was observed by TEM (Figure 5). The NPs surrounding tumor cells were endocytosed by the vesicles, demonstrating a nonspecific endocytic process called macropinocytosis.44,45 Macropinocytosis involves the internalization of large areas of the plasma membrane together with large amounts of fluid. After invagination of membrane plasma and then suspension within small vesicles, these pinocytosis vesicles containing FePt NPs subsequently fuse with lysosomes. Then the chemically stable FePt NPs partially degrade (hydrolyze) into highly active Pt2+, Fe2+, and Fe3+ ions in acid environments (pH ≈4.8, mainly in lysosome). The released Pt2+ ions from primary or secondary lysosomes may then enter into the nuclei and mitochondria, coordinate with 5′-GG-3′ bases of DNA, prevent DNA from replicating properly, and lead to the apoptosis of tumor cells.46,47 Alternatively, the released Fe2+ and Fe3+ ions may trigger an excess of highly reactive oxygen species (ROS) levels as Fenton-like catalysts. The ROS, such as the hydroxyl radical (•OH) and carboxyl radical (•OOH), are powerful agents for damaging various matter in cells, leading to cell death.27,38 Therefore, FePt NPs may have potential to act as chemotherapy agents to kill tumor cells. As demonstrated in the current study, FePt NPs combined with X-ray beams suppressed the proliferation of HeLa cells more efficiently as a radiosensitizer (Figure 4). The mechanism of this phenomenon may be attributed to the partial pressure increase of oxygen which, when accompanied by the excess generation of ROS, led to the increase of HeLa cells’ radiosensitivity at the moment of irradiation.48 Because of the excellent X-ray mass absorption coefficient of the Pt atom,49 the original divergence and homogeneous nature of the X-ray beam could be focused on HeLa cells, aiming to concentrate energy to damage HeLa cells precisely. Here, FePt NPs played a part as radiosensitizers in the progress of a tumor radiotherapy model. Moreover, it would not be farfetched to surmise that normal tissues and organs surrounding tumor cells would absorb less energy from FePt NP-mediated radiotherapy treatment. Indeed, this factor increases the therapeutic gain of FePt NPs. In addition, the increased precision of this method may further promote the degradation of FePt NPs, a hypothesis which is currently being explored. In a nutshell, the current study has proposed that the intelligent application of FePt alloy NPs may improve cancer therapy and imaging effects and, as a multifunctional nanoprobe, decrease the occurrence of complications in the integration of tumor diagnosis and therapy. This idea could satisfy the ultimate goal of personalized chemoradiotherapy. Future work will focus upon the FePt surface engineering of targeted molecules, as well as further exploration of the interactive effect of FePt NPs and X-rays upon the damage of tumor cells, while simultaneously protecting normal cells.
The current study reports the synthesis of superparamagnetic, monodispersed FePt NPs with ligand exchange mediated by Cys. Cytotoxicity was assessed in Vero cells, and the potential utilization of the FePt NPs for integration of chemotherapy and radiotherapy was evaluated in HeLa cells in vitro. Finally, the prospective application of FePt NPs as dual-model contrast agents for MRI/CT molecular imaging was measured via MRI and CT scans in vitro. The results suggested that FePt NPs inhibited the growth of HeLa cells in a concentration-dependent manner while avoiding the effects of significant toxicity to Vero cells at concentrations below 250 μg/mL. The proliferation of HeLa cells was remarkably suppressed by FePt NPs with serial doses of X-ray beams, which showed a greater efficacy than the same concentrations of individual FePt NPs do. The combined effect of FePt NPs and X-ray beam was verified in HeLa cells. Altogether, these results indicated that FePt NPs are a promising nanoprobe for the integration of diagnosis and chemoradiotherapy for tumor treatment.
This study was financially supported by the Natural Science Foundation of China (No 10875092 and 31271511), and the Natural Science Foundation of Hubei Province of China (No 2012KB04449). The authors are grateful to the Department of Radio- and Chemo-therapy, Zhongnan Hospital of Wuhan University, Wuhan, People’s Republic of China, and Elekta Instrument (Shanghai) Ltd. for their assistance with the project.
The authors report no conflicts of interest in this work.
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