ABSTRACT
Objective:
To evaluate the potential of magnetic hyperthermia using aminosilane-coated superparamagnetic iron oxide nanoparticles in glioblastoma tumor model.
Methods:
The aminosilane-coated superparamagnetic iron oxide nanoparticles were analyzed as to their stability in aqueous medium and their heating potential through specific absorption rate, when submitted to magnetic hyperthermia with different frequencies and intensities of alternating magnetic field. In magnetic hyperthermia in vitro assays, the C6 cells cultured and transduced with luciferase were analyzed by bioluminescence in the absence/presence of alternating magnetic field, and also with and without aminosilane-coated superparamagnetic iron oxide nanoparticles. In the in vivo study, the measurement of bioluminescence was performed 21 days after glioblastoma induction with C6 cells in rats. After 24 hours, the aminosilane-coated superparamagnetic iron oxide nanoparticles were implanted in animals, and magnetic hyperthermia was performed for 40 minutes, using the best conditions of frequency and intensity of alternating magnetic field tested in the in vitro study (the highest specific absorption rate value) and verified the difference of bioluminescence before and after magnetic hyperthermia.
Results:
The aminosilane-coated superparamagnetic iron oxide nanoparticles were stable, and their heating capacity increased along with higher frequency and intensity of alternating magnetic field. The magnetic hyperthermia application with 874kHz and 200 Gauss of alternating magnetic field determined the best value of specific absorption rate (194.917W/g). When these magnetic hyperthermia parameters were used in in vitro and in vivo analysis, resulted in cell death of 52.0% and 32.8%, respectively, detected by bioluminescence.
Conclusion:
The magnetic hyperthermia was promissing for the therapeutical process of glioblastoma tumors in animal model, using aminosilane-coated superparamagnetic iron oxide nanoparticles, which presented high specific absorption rate.
Keywords: Glioblastoma/therapy; Magnetic, hyperthermia; Nanoparticles; Magnetite nanoparticles; Cell tracking/methods; Aminosilane; Tumoral model; Rats
RESUMO
Objetivo:
Avaliar o potencial da técnica de magneto-hipertermia utilizando nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana em modelo de tumores de glioblastoma.
Métodos:
As nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana foram avaliadas quanto à sua estabilidade em meio aquoso e a seu potencial de aquecimento pela taxa de absorção específica, quando submetidas à magneto-hipertermia, com diferentes frequências e intensidades de campo magnético alternado. Nos ensaios de magneto-hipertermia in vitro, as células C6 cultivadas e transduzidas com luciferase foram avaliadas por bioluminescência na presença/ausência do campo magnético alternado, como também com e sem nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana. No estudo in vivo, a medida de bioluminescência foi adquirida no 21º dia após indução do glioblastoma com células C6 nos ratos. Após 24 horas, as nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana foram implantadas no animal, tendo sido realizada a magneto-hipertermia por 40 minutos, nas melhores condições de frequência e intensidade de campo magnético alternado testado no estudo in vitro (maior valor da taxa de absorção específica); foi verificada a diferença do bioluminescência antes e após a magneto-hipertermia.
Resultados:
As nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana se mostraram estáveis, e sua capacidade de aquecimento aumentou com o incremento da frequência e da intensidade de campo magnético alternado. A aplicação da magneto-hipertermia, com 874kHz e 200 Gauss do campo magnético alternado, determinou o melhor valor da taxa de absorção específica (194,917W/g). Quando utilizados, estes parâmetros de magneto-hipertermia in vitro resultaram em morte celular de 52,0% e in vivo de 32,8% por bioluminescência.
Conclusão:
A técnica de magneto-hipertermia foi promissora para o processo terapêutico de tumores de glioblastoma no modelo animal utilizando as nanopartículas superparamagnéticas de óxido de ferro recobertas com aminosilana recobertas com aminosilana, que apresentaram alta taxa de absorção específica.
Descritores: Glioblastoma/terapia; Magneto, hipertermia; Nanopartículas; Nanopartículas de magnetita; Aminosilana; Modelo tumoral; Ratos
INTRODUCTION
Glioblastoma (GBM) accounts for 47.7% of all malignant brain tumors, and only 5.6% of patients affected survive up to 5 years after diagnosis, as per the statistical report of the Central Brain Tumor Registry of the United States (CBTRUS),( 1 ) with a prognosis that is still guarded. Glioblastoma represents one of the most devastating diseases of the central nervous system due to its extremely aggressive behavior, and no satisfactory responses to the varied therapeutic modalities so far.( 2 )
Preclinical studies in GBM tumors allowed understanding and evaluation of the different strategies for the therapeutic process.( 3 , 4 ) Among the preclinical models of tumor induction,( 5 ) those that use C6 cells show advantages due to histological aspects and their similarities with findings in humans. These include nuclear polymorphism, high rates of mitosis, tumor necrosis foci, intratumor hemorrhage, invasion of the parenchyma, and neoangiogenesis.( 5 , 6 )
Since currently there is no effective treatment for GBM, alternative therapeutic mechanisms have been developed,( 7 ) among which, magnetic hyperthermia (MHT). Its relevance results from significant antitumor effects in models of GBM,( 8 , 9 ) as well as in other types of tumors.( 10 , 11 ) In the MHT technique, when directed towards the tumor and exposed to an alternating magnetic field (AMF) with appropriate intensity frequencies, the magnetic nanoparticles are heated until reaching a therapeutic temperature of 42-45°C,( 12 ) capable of affecting the tumor mass without hindering the surrounding normal tissue.( 9 )
Superparamagnetic iron oxide nanoparticles (SPIONs) have a great potential for application in the MHT, based on their magnetic properties of energy transformation, generating heat.( 9 ) Preclinical studies showed the efficacy of several biocompatible sizes and coatings of SPIONs,( 13 ) although in many of these studies the efficacy of MHT was evaluated in models of GBM tumors induced in the flanks of the animals instead of intracerebral induction.( 13 ) Applications, both of the inductive cells of the tumor as well as the SPIONs through stereotaxis, are the most adequate options for the representation of the GBM model submitted to an MHT treatment. They mimic what really happens, and due to the need to place a large quantity of SPIONs located in the tumor to increase the heating potential of thermotherapy.( 14 )
There are some aspects that still need to be assessed relative to efficacy of MHT therapy, such as the physical and chemical properties of the nanoparticles, coatings, size, type of magnetic nanoparticle, AMF parameters (frequency and intensity of oscillating field), concentration of nanoparticles, time of application of MHT, as well as few studies using models of intracerebral glioblastoma.( 8 , 13 ) One of the magnetic nanoparticles that presents with a great potential is SPIONs coated with aminosilane (SPIONsAmin), as they present with a greater value of saturation magnetization (790.93 A/m) and influences the heating capacity, in comparison with SPIONs coated with other materials, for instance, carboxymethyl-dextran (227.13 A/m).( 15 ) Using SPIONsAmin in assays with MHT, Jordan et al.,( 9 ) showed that SPIONs enabled the formation of more stable deposits of nanoparticles around the entire tumor, relative to SPIONs coated with dextran. Additionally, these SPIONsAmin were evaluated and used for clinical applications in patients with tumors,( 16 ) and did not harm cortical neurons in animal model studies.( 17 )
In this sense, the present study seeks to elucidate, in vitro and in vivo, the properties of SPIONs coated with aminosilane associated with different parameters of MHT in the therapeutic efficiency of GBM in preclinical models. Therefore, we evaluated the characteristics of the appropriate AMF for MHT applied in the treatment of GBM tumors, due to the efficiency in heating of the SPIONsAmin, resulting from the intensity of the magnetic field and the frequency of oscillation, as well as the assessment of the efficacy of MHT therapy in vitro and in vivo, by means of the bioluminescence (BLM) technique.
OBJECTIVE
To evaluate the potential of the magnetic hyperthermia using nanoparticles of iron oxide coated with aminosilane in models of glioblastoma tumors.
METHODS
Experimental design
This study was developed in three stages. In the first stage, tests were performed of stability of the hydrodynamic size of the SPIONsAmin (Figure 1A), as well as of the transformation potential of magnetic into thermal energy in the SPIONsAmin, using different frequencies and intensities of magnetic field, obtaining, from the heating curves, the specific absorption rate (SAR) (Figure 1B). In the second stage, in vitro tests were performed to verify the viability of C6 cells with and without the application of MHT, in the presence and absence of SPIONsAmin (Figure 1C). In the third stage, in vivo MHT assays were conducted, initiating with a tumor induction of intracerebral GBM in rats, by means of the application of 106 C6 cells through stereotaxis (Figure 1D), followed by the tumor evaluation by BLM, pre- and post-application of MHT (Figure 1E), which used the parameters established in the first and second stages.
Magnetic nanoparticles
SPIONsAmin with a magnetite nucleus (Fe3O4) (Chemicell, Berlin, Germany), with a density of ∼1.25g/cm3, coupled with the functional amine (NH2) group, and HD 100nm and zeta potential +20mV.
Size distribution of aminosilane-coated superparamagnetic iron oxide nanoparticles
To evaluate the polydispersion of the HD and stability of SPIONsAmin, the dynamic light scattering (DLS) technique was used, with the Zetasizer Nano S (Malvern, UK) system. The assessment was made at the concentration of 100mgFe/mL, and data were collected at 25°C, for a 60-second equilibrium period, with recordings every 30 minutes for 24 hours.
Heating potential of the aminosilane-coated superparamagnetic iron oxide nanoparticles in the magnetic hyperthermia system
To determine the heating potential of SPIONsamin with the MHT technique, an AMF system model DM100 (nB nanoScale Biomagnetics) was used, combining four frequencies (309, 557, 715, and 874kHz), and five intensities of magnetic field (100, 125, 150, 175, and 200 Gauss) to obtain the heating curves.
We used 100μL of SPIONsAmin at the concentration of 5mg/mL dispersed in an aqueous medium, allocated in a thermally isolated recipient. The temperature of the SPIONsAmin was monitored through an optical fiber system (Luxtron 3204), initiating all the analyses at 19°C.
The heating curves obtained were used to calculate the values of SAR in W/g for each frequency and magnetic field applied, according to equation 1:
(Equation 1) |
where Hwater is the specific heat of the water, ΔT/δt is the initial inclination of the temperature in °C/s, and CFe is the concentration of iron in g/mL.
In vitro study
C6 cell culture
The C6 cell line was cultivated in RPMI medium (GIBCO® Invitrogen Corporation, CA, USA), supplemented with 10% bovine fetal serum (BFS) (GIBCO® Invitrogen Corporation, CA, USA), and incubated at 37°C (5% of CO2) until reaching a confluence of 70%, when it then was trypsinized to be used in the proposed trials.
The C6 cells were transduced with a luciferase lentiviral vector as per a previously established protocol,( 1 8) resulting in the acquisition of cells transfected with luciferase for the evaluation of treatment with the BLM technique.
Evaluation of magnetic hyperthermia in vitro
Samples containing 106 C6 cells suspended in 200µL of RPMI 10% BFS were evaluated in triplicate under four conditions: C6 cells (Control Group), C6 cells marked with SPIONsAmin, C6 cells submitted to MHT, and C6 cells marked with SPIONsAmin submitted to MHT. Marking of the C6 with SPIONsAmin was performed with 600mg Fe/mL for 18 hours. In the samples submitted to MHT, we used the parameters of 200 Gauss and 874kHz for a period of 40 minutes. Efficiency of the MHT technique (cell viability) was evaluated with BLM, in which 100µL of luciferin were added to each sample, along with the posterior acquisition of images employing the IVIS Lumina III (XenogenCorp, USA) equipment.
Study in vivo
Animals
Ten male Wistar rats at 2 months of age (weighing 290 to 350g) were used. The animals were acclimated at the Surgical Experimentation and Training Center (CETEC) of the Instituto de Ensino e Pesquisa Albert Einstein (CEUA 3126-17). This vivarium is accredited by the Association for Assessment and Accreditation of Laboratory Animal Care International (AAALAC). The animals were kept in individual boxes lined with autoclaved sawdust, with water and balanced feed ad libitum, following a light-dark cycle of 12 hours (7 am to 7 pm), with a temperature of 21°C (±2°C), as per international specifications.
Glioblastoma tumor induction with C6 cells
The animals were anesthetized with ketamine (90mg/kg)and xylazine (12mg/kg). Implantation of C6 cells (106/10µL of culture medium) was done by stereotaxis according to the established protocol.( 6 ) The point of implantation of cells in the right frontal cortex was determined and marked on the bone surface following orientations of Swansen's stereotaxical atlas:( 19 ) anteroposterior = 2.0mm; latero-lateral = 2.0mm; depth = 2.5mm.
Magnetic hyperthermia process assay in the animal model
The in vivo MHT assays were performed 21 days after tumor induction. This application of tumor staging is based on previous studies of the group.( 20 , 21 )
Before being submitted to the MHT process, the control tumor evaluation was performed on the 21st day with the BLM technique, using IVIS equipment in which the animals were maintained with inhaled anesthesia of isofluorane (2% saturation) with a flow of 2.5L/min of oxygen. The BLM signal was acquired after 5 minutes of administration of 100μL luciferin solution (1mM in PBS).
On the 22nd day after tumor induction, 50µg of iron were applied contained in 10µL of the colloidal suspension of SPIONsAmin, divided into four equidistant points, 3mm from the central region of the tumor mass using stereotaxis equipment. After 20 minutes of the SPIONsAmin application, the animals were positioned inside the coil of the MHT equipment and submitted to the planned heating, composed of two parts. During the first part, the frequency of 874kHz and a field of 200 Gauss were used until reaching 42°C; during the second part, the frequency was maintained and the intensity of the field was modulated to maintain the temperature at 42°C, totaling up a period de 40 minutes of MHT. Mapping of the intratumor temperature was measured with an optical fiber (Luxtron 3204) with temperature probes (diameter of 0.55mm).
After MHT application, the animals were reassessed by means of BLM, and thus was determined the difference of the signal between the images before and after therapy in photons/second.
RESULTS
Dynamic light scattering
The measurements of stability performed with the DLS technique on the SPIONsAmin dispersed in water are shown in figure 2. The curves of figure 2A indicate that the SPIONsAmin are polydispersed in the hydrodynamic size, in which the peak of maximal intensity corresponding to the mean HD was 110±5nm, with no significant difference between the measurements (p>0.05) acquired in 24 hours. Therefore, we can consider SPIONsAmin stable during the period analyzed, as shown in figure 2B.
Heating capacity of the aminosilane-coated superparamagnetic iron oxide nanoparticles
The heating curves of the SPIONsAmin obtained when submitted to AMF are shown in figure 3. The evaluation of heating shows that for samples submitted to AMD intensities varying from 100 to 200 Gauss for fixed frequencies, the heating temperature is incremented with the increase of the magnetic field (Figure 3A-D), as well as with the elevation of frequencies. Heating time also decreases with the use of elevated frequencies and AMF (Figure 3D). Aminosilane-coated superparamagnetic iron oxide nanoparticles dispersed in an aqueous medium under the action of an ADF of 200 Gauss and 874kHz, provided greater heating relative to other parameters, and the temperature reached 50°C in less than 50 seconds (Figure 3D).
Specific absorption rate calculation
The analysis of SAR (Figure 4) was carried out based on the heating curves previously obtained (Figure 3). It was noted that the exposure of SPIONsAmin at 874kHz and 200 Gauss afforded a higher SAR (194.917W/g) among all the analyses (Figure 4). Table 1 shows the values of SAR in each analysis applied, and SAR depended on the intensity of the AMF and the frequency. The value of SAR measured at 200 Gauss within the frequency range of 309 to 874kHz is incremented by 28.5 to 194.7W/g, and is significant (p<0.001) relative to the frequencies analyzed, as well as in the fields analyzed (p<0.001), since in the case of SAR measured as 874kHz in the magnetic field of 100-200 Gauss there is an increment of 57.2 to 194.7W/g. Therefore, the values of SAR increased insofar as the established parameters of frequency and intensity of the magnetic field also raise; the results presented of the interaction between both the parameters are significant (p<0.001).
Table 1. Specific absorption rate values calculated for aminosilane-coated superparamagnetic iron oxide nanoparticles, under the effect of alternating magnetic fields of 100, 125, 150, 175, and 200 Gauss for 309, 557, 715, and 874kHz.
Frequency of AMF(kHz) | Intensity of AMF (Gauss) | SAR (W/g) |
---|---|---|
309 | 100 | 12.2±2.4 |
125 | 16.2±2.2 | |
150 | 23.0±3.4 | |
175 | 24.4±3.9 | |
200 | 28.5±3.5 | |
557 | 100 | 19.2±4.1 |
125 | 29.2±6.8 | |
150 | 32.5±6.4 | |
175 | 36.3±6.4 | |
200 | 50.4±5.0 | |
715 | 100 | 46.2±4.1 |
125 | 49.4±6.2 | |
150 | 90.6±7.9 | |
175 | 96.0±9.9 | |
200 | 120.4±7.7 | |
874 | 100 | 57.2±4.5 |
125 | 77.4±6.1 | |
150 | 115.1±8.5 | |
175 | 172.6±9.8 | |
200 | 194.7±10.8 |
By the variance analysis (ANOVA), a significant difference was verified among the fields and frequencies, and in the interaction between fields and frequencies with p<0.001. The data were previously tested as to distribution. AMF: alternating magnetic field; SAR: specific absorption rate.
Evaluation in vitro of magnetic hyperthermia
The C6 cells of the control group, when observed by the BLM image, presented with an intensity of 2.33x108 photons/s (Figure 5I), with no significant difference (p>0.05) as to the intensity of BLM of the C6 cells submitted to MHT (200 Gauss and 874kHz) in the absence of SPIONsAmin (2.37x108 photons/s) (Figure 5II) as to the intensity of BLM of the C6 cells in the presence only of SPIONsAmin (2.32x108 photons/s) (Figure 5III). These results indicate that neither AMF nor SPIONsAmin by themselves interfere in the viability of C6 cells. However, in C6 cells that received MHT applications in the presence of SPIONsAmin, a 52% reduction was noted in cellular viability when compared to the controls (1.14x108 photons/s) (Figure 5-IV).
Evaluation of magnetic hyperthermia in the animal model by bioluminescence
On the 21st day after tumor induction, the baseline evaluation of the tumor by BLM without the application of luciferin showed that the BLM equipment alone is not capable of biasing the analysis result (Figure 5A). After application of luciferin and before the application of the AMF, the tumor signal recorded by BLM was 3.45x109 photons/s (Figure 5B). After 24 hours, MHT was applied (200 Gauss and 874kHz) for 40 minutes, with an observed signal decay to 2.32x109 photons/s (Figure 5C). After application of MHT using the best conditions of AMF intensity and frequency previously tested in vitro, the decrease in tumor mass relative to the controls was 32.8% (Figure 5D).
DISCUSSION
The use of nanotechnological resources applied to therapeutic techniques for aggressive tumors, such as the GBM, has represented an important role in preclinical studies, especially the use of magnetic nanoparticles for diagnostic and therapeutic purposes.( 22 )Superparamagnetic iron oxide nanoparticles have different physical and chemical characteristics with different biological interactions,( 23 ) such as the HD, in which the conservation of the size over time avoids the formation of clusters, making the SPIONs stabler,( 24 ) and consequently, more effective in the MHT technique.( 25 ) This is an important characteristic, albeit poorly explored relative to the description of stability of SPIONs. In the present study, the kinetics of the aggregation process of the SPIONsAmin monitored for 24 hours by DLS, showed that there was no formation of clusters, maintaining the HD and its distribution polydispersed, a characteristic of the magnetic nanoparticles.( 26 )
After guaranteeing the stability of the SPIONsAmin, the heating potential measured by SAR was evaluated with the objective of planning the therapeutic temperature. In the process of characterization of the heating curves obtained by the variations of amplitude and frequency of AMF, a forced hysteresis is evident in the SPIONsAmin, which contributes to the complex magnetization in heating, as well as the electromagnetic and thermal processes that influence heating.( 27 ) Heating of the aqueous dispersion of SPIONsAmin when submitted to MHT essays, occurs due to a spatial arrangement of the SPIONsAmin, which under the action of the magnetic field, produces changes in the interparticulate dipole-dipole interactions and in the Brownian movement.( 28 ) A review study showed that magnetite nanoparticles with similar properties applied in preclinical studies, showed SAR values in the range of 96 to 286W/g.( 13 ) In clinical applications, SAR values are within the range of 0.12 to 2,452W/g, depending on the characteristics of the nanoparticles, as well as of the experimental parameters.( 25 , 29 , 30 ) Thus, the values of SAR found in our study were consistent with literature, in which the highest value of SAR was 194.917W/g for the colloidal suspension of the SPIONsAmin submitted to AMF of 874kHz and 200 Gauss, proving adequate for the in vivo application of the MHT therapy.
Before the application of MHT in vivo, it was noted, through the BLM images in the in vitro sample, that AMF did not influence the viability of the C6 cells in the absence of SPIONsAmin, or the viability of the cells in the presence of SPIONsAMIN in AMF. The BLM technique, due to its sensitivity, is used in the evaluation of tumor growth and of possible metastases,( 31 ) and has a good correlation with other imaging techniques, such as magnetic resonance and histology( 27 , 31 ) in monitoring of tumor growth.
The efficiency of MHT of the SPIONsAmin administered locally in the tumor mass can be influenced by several factors, such as the dispersion of SPIONsAmin throughout the tissues surrounding the administration site, which affects the heating produced by the SPIONsAmin in the presence of AMF. Additionally, heating can be influenced by physiological aspects that are implicit in the calculation of heat transfer (Pennes equation), such as local metabolism, blood perfusion rates, coefficient of heat transfer in the tissues involved, specific mass of the blood, among others.( 32 , 33 ) In our study, we obtained 32.5% efficiency with a single application of MHT, using the lowest mass value of SPIONsAmin (50µg Fe) in comparison with other studies that applied in the range of 0.5 to 3mg Fe in glioma tumors induced in the flank or subcutaneous regions.( 13 ) Use of high concentrations of iron nanoparticles can cause toxicity to neighboring tissues, as well as affect other organs associated in the biodistribution and elimination of nanoparticles through the liver, kidneys, and spleen.( 34 )
As a limitation of the study, we can point out that the efficiency of MHT through the evaluation of cell viability was not tested with a shorter AMF application time, or in its effect over time.
Preclinical studies of MHT showed promising results when combined with another treatment, such as radiation therapy or chemotherapy.( 35 ) Nonetheless, there are challenges to be overcome in order to increase the efficiency of MHT for clinical application. The increase in efficiency of MHT therapy depends of the prior determination of AMF parameters, which produce the adequate value of nanomaterial SAR, as well as the appropriate evaluation of in vitro and in vivo with molecular imaging techniques, such as BLM. Finally, we can affirm that SPIONsAmin have the potential for MHT therapy in the treatment of GBM tumors.
CONCLUSION
The present study evaluated the potential of magnetic hyperthermia using the aminosilane-coated superparamagnetic iron oxide nanoparticles for the treatment of glioblastoma in the animal model. The value of the specific absorption rate characterized for aminosilane-coated superparamagnetic iron oxide nanoparticles submitted to the action of an alternating magnetic field, indicates a good capacity for heating in order to reach the temperature. The bioluminescence technique showed, after application of magnetic hyperthermia therapy, a reduction in cell viability by 32.8% in the in vitro study and of 52% in the in vivo study. Therefore, application of magnetic hyperthermia proved to be promising for the therapeutic process of glioblastoma tumors using aminosilane-coated superparamagnetic iron oxide nanoparticles, which demonstrates favorable magnetic characteristics for the process of magnetic hyperthermia. Nevertheless, a careful assessment of other parameters involved, such as magnetic properties, polydispersion of superparamagnetic iron oxide nanoparticles, morphology, dose applied of superparamagnetic iron oxide nanoparticles, site of administration, periodic applications of the treatment, among others is necessary.
ACKNOWLEDGMENTS
To Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) and Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES); to the team of the Surgical Experimentation and Training Center and Experimentation Research Center of Instituto Israelita de Ensino e Pesquisa Albert Einstein.
REFERENCES
- 1.Ostrom QT, Gittleman H, Truitt G, Boscia A, Kruchko C, Barnholtz-Sloan JS. CBTRUS Statistical Report: Primary Brain and Other Central Nervous System Tumors Diagnosed in the United States in 2011-2015. Neuro-oncol. 2018;20(suppl_4):iv1–iv86. doi: 10.1093/neuonc/noy131. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 2.Davis ME. Glioblastoma: overview of disease and treatment. Clin J Oncol Nurs. 2016;20(5 Suppl):S2–S8. doi: 10.1188/16.CJON.S1.2-8. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 3.Chen L, Zhang Y, Yang J, Hagan JP, Li M. Vertebrate animal models of glioma: understanding the mechanisms and developing new therapies. Biochim Biophys Acta. 2013;1836(1):158–165. doi: 10.1016/j.bbcan.2013.04.003. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 4.Bai RY, Staedtke V, Riggins GJ. Molecular targeting of glioblastoma: drug discovery and therapies. Trends Mol Med. 2011;17(6):301–312. doi: 10.1016/j.molmed.2011.01.011. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 5.Barth RF, Kaur B. Rat brain tumor models in experimental neuro-oncology: the C6, 9L, T9, RG2, F98, BT4C, RT-2 and CNS-1 gliomas. J Neurooncol. 2009;94(3):299–312. doi: 10.1007/s11060-009-9875-7. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 6.da Silva AC, Cabral FR, Mamani JB, Malheiros JM, Polli RS, Tannus A, et al. Tumor growth analysis by magnetic resonance imaging of the C6 glioblastoma model with prospects for the assessment of magnetohyperthermia therapy. einstein (São Paulo) 2012;10(1):11–15. doi: 10.1590/s1679-45082012000100004. [DOI] [PubMed] [Google Scholar]
- 7.Shergalis A, Bankhead A, 3rd, Luesakul U, Muangsin N, Neamati N. Current challenges and opportunities in treating glioblastoma. Pharmacol Rev. 2018;70(3):412–445. doi: 10.1124/pr.117.014944. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 8.Mahmoudi K, Bouras A, Bozec D, Ivkov R, Hadjipanayis C. Magnetic hyperthermia therapy for the treatment of glioblastoma: a review of the therapy's history, efficacy and application in humans. Int J Hyperthermia. 2018;34(8):1316–1328. doi: 10.1080/02656736.2018.1430867. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 9.Jordan A, Scholz R, Maier-Hauff K, van Landeghem FK, Waldoefner N, Teichgraeber U, et al. The effect of thermotherapy using magnetic nanoparticles on rat malignant glioma. J Neurooncol. 2006;78(1):7–14. doi: 10.1007/s11060-005-9059-z. [DOI] [PubMed] [Google Scholar]
- 10.Jordan A, Scholz R, Wust P, Fähling H, Krause J, Wlodarczyk W, et al. Effects of magnetic fluid hyperthermia (MFH) on C3H mammary carcinoma in vivo. Int J Hyperthermia. 1997;13(6):587–605. doi: 10.3109/02656739709023559. [DOI] [PubMed] [Google Scholar]
- 11.Johannsen M, Jordan A, Scholz R, Koch M, Lein M, Deger S, et al. Evaluation of magnetic fluid hyperthermia in a standard rat model of prostate cancer. J Endourol. 2004;18(5):495–500. doi: 10.1089/0892779041271715. [DOI] [PubMed] [Google Scholar]
- 12.Shaterabadi Z, Nabiyouni G, Soleymani M. Physics responsible for heating efficiency and self-controlled temperature rise of magnetic nanoparticles in magnetic hyperthermia therapy. Prog Biophys Mol Biol. 2018;133:9–19. doi: 10.1016/j.pbiomolbio.2017.10.001. Review. [DOI] [PubMed] [Google Scholar]
- 13.Silva AC, Oliveira TR, Mamani JB, Malheiros SM, Malavolta L, Pavon LF, et al. Application of hyperthermia induced by superparamagnetic iron oxide nanoparticles in glioma treatment. Int J Nanomedicine. 2011;6:591–603. doi: 10.2147/IJN.S14737. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 14.Maier-Hauff K, Ulrich F, Nestler D, Niehoff H, Wust P, Thiesen B, et al. Efficacy and safety of intratumoral thermotherapy using magnetic iron-oxide nanoparticles combined with external beam radiotherapy on patients with recurrent glioblastoma multiforme. J Neurooncol. 2011;103(2):317–324. doi: 10.1007/s11060-010-0389-0. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 15.Yuan Y, Tasciuc DA. Comparison between experimental and predicted specific absorption rate of functionalized iron oxide nanoparticle suspensions. J Magn Magn Mater. 2011;323(20):2463–2469. [Google Scholar]
- 16.Maier-Hauff K, Rothe R, Scholz R, Gneveckow U, Wust P, Thiesen B, et al. Intracranial thermotherapy using magnetic nanoparticles combined with external beam radiotherapy: results of a feasibility study on patients with glioblastoma multiforme. J Neurooncol. 2007;81(1):53–60. doi: 10.1007/s11060-006-9195-0. [DOI] [PubMed] [Google Scholar]
- 17.Rivet CJ, Yuan Y, Gilbert RJ, Borca-Tasciuc DA. Effect of magnetic nanoparticle heating on cortical neuron viability. Int J Hyperthermia. 2014;30(2):79–85. doi: 10.3109/02656736.2013.873825. [DOI] [PubMed] [Google Scholar]
- 18.Fantacini DM, Picanço-Castro V. Production of recombinant factor VIII in human cell lines. Methods Mol Biol. 2018;1674:63–74. doi: 10.1007/978-1-4939-7312-5_5. [DOI] [PubMed] [Google Scholar]
- 19.Swanson L. Brain maps: structure of the rat brain. 3rd ed. Philadelphia: Elsevier; 1992. [Google Scholar]
- 20.Mamani JB, Malheiros JM, Cardoso EF, Tannús A, Silveira PH, Gamarra LF. In vivo magnetic resonance imaging tracking of C6 glioma cells labeled with superparamagnetic iron oxide nanoparticles. einstein (São Paulo) 2012;10(2):164–170. doi: 10.1590/s1679-45082012000200009. [DOI] [PubMed] [Google Scholar]
- 21.Souza TK, Nucci MP, Mamani JB, da Silva HR, Fantacini DM, de Souza LE, et al. Image and motor behavior for monitoring tumor growth in C6 glioma model. PLoS One. 2018;13(7):e0201453. doi: 10.1371/journal.pone.0201453. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 22.Fernandez-Fernandez A, Manchanda R, McGoron AJ. Theranostic applications of nanomaterials in cancer: drug delivery, image-guided therapy, and multifunctional platforms. Appl Biochem Biotechnol. 2011;165(7-8):1628–1651. doi: 10.1007/s12010-011-9383-z. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 23.Treuel L, Eslahian KA, Docter D, Lang T, Zellner R, Nienhaus K, et al. Physicochemical characterization of nanoparticles and their behavior in the biological environment. Phys Chem Chem Phys. 2014;16(29):15053–15067. doi: 10.1039/c4cp00058g. [DOI] [PubMed] [Google Scholar]
- 24.Moore TL, Rodriguez-Lorenzo L, Hirsch V, Balog S, Urban D, Jud C, et al. Nanoparticle colloidal stability in cell culture media and impact on cellular interactions. Chem Soc Rev. 2015;44(17):6287–6305. doi: 10.1039/c4cs00487f. [DOI] [PubMed] [Google Scholar]
- 25.Abenojar EC, Wickramasinghe S, Bas-Concepcion J, Samia AC. Structural effects on the magnetic hyperthermia properties of iron oxide nanoparticles. Progress in Natural Science: Materials International. 2016;26(5):440–448. [Google Scholar]
- 26.Lim J, Yeap SP, Che HX, Low SC. Characterization of magnetic nanoparticle by dynamic light scattering. Nanoscale Res Lett. 2013;8(1):381–381. doi: 10.1186/1556-276X-8-381. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 27.Soetaert F, Kandala SK, Bakuzis A, Ivkov R. Experimental estimation and analysis of variance of the measured loss power of magnetic nanoparticles. Sci Rep. 2017;7(1):6661–6661. doi: 10.1038/s41598-017-07088-w. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 28.Branquinho LC, Carrião MS, Costa AS, Zufelato N, Sousa MH, Miotto R, et al. Effect of magnetic dipolar interactions on nanoparticle heating efficiency: implications for cancer hyperthermia. Sci Rep. 2013;3(1):2887–2887. doi: 10.1038/srep02887. Erratum in: Sci Resp. 2014;4:3637. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 29.Jeon S, Hurley KR, Bischof JC, Haynes CL, Hogan CJ. Quantifying intra- and extracellular aggregation of iron oxide nanoparticles and its influence on specific absorption rate. Nanoscale. 2016;8(35):16053–16064. doi: 10.1039/c6nr04042j. [DOI] [PubMed] [Google Scholar]
- 30.Orsinia NJ, Babić-Stojića B, Spasojevića V, Calatayud MP, Cvjetićanin N, Goya GF. Magnetic and power absorption measurements on iron oxide nanoparticles synthesized by thermal decomposition of Fe(acac)3. J Magn Magn Mater. 2018;449:286–296. [Google Scholar]
- 31.Adiseshaiah PP, Patel NL, Ileva LV, Kalen JD, Haines DC, McNeil SE. Longitudinal imaging of cancer cell metastases in two preclinical models: a correlation of noninvasive imaging to histopathology. Int J Mol Imaging. 2014;2014:102702–102702. doi: 10.1155/2014/102702. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 32.Attar MM, Haghpanahi M, Amanpour S, Mohaqeq M. Analysis of bioheat transfer equation for hyperthermia cancer treatment. J Mech Sci Technol. 2014;28(2):763–771. [Google Scholar]
- 33.Giordano MA, Gutierrez G, Rinaldi C. Fundamental solutions to the bioheat equation and their application to magnetic fluid hyperthermia. Int J Hyperthermia. 2010;26(5):475–484. doi: 10.3109/02656731003749643. [DOI] [PubMed] [Google Scholar]
- 34.Patil US, Adireddy S, Jaiswal A, Mandava S, Lee BR, Chrisey DB. In Vitro/In Vivo Toxicity Evaluation and Quantification of Iron Oxide Nanoparticles. Int J Mol Sci. 2015;16(10):24417–24450. doi: 10.3390/ijms161024417. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 35.Chang D, Lim M, Goos JA, Qiao R, Ng YY, Mansfeld FM, et al. Biologically Targeted Magnetic Hyperthermia: potential and Limitations. Front Pharmacol. 2018;9:831–831. doi: 10.3389/fphar.2018.00831. Review. [DOI] [PMC free article] [PubMed] [Google Scholar]