N. Venkateshaa,
Shivanand M. Pudakalakattib,
Yasrib Qurishic,
Hanudatta S. Atreyab and
Chandan Srivastava*a
aDepartment of Materials Engineering, Indian Institute of Science, Bangalore, India. E-mail: csrivastava@materials.iisc.ernet.in; Fax: +91-080-2360-0472; Tel: +91-080-22932834
bNMR Research Centre, Indian Institute of Science, Bangalore, India
cDepartment of Molecular Reproduction, Development and Genetics, Indian Institute of Science, Bangalore, India
First published on 9th November 2015
In recent years, magnetic core–shell nanoparticles have received widespread attention due to their unique properties that can be used for various applications. We introduce here a magnetic core–shell nanoparticle system for potential application as a contrast agent in magnetic resonance imaging (MRI). MnFe2O4–Fe3O4 core–shell nanoparticles were synthesized by the wet-chemical synthesis method. Detailed structural and compositional charaterization confirmed the formation of a core–shell microstructure for the nanoparticles. Magnetic charaterization revealed the superparamagnetic nature of the as-synthesized core–shell nanoparticles. Average size and saturation magnetization values obtained for the as-synthesized core–shell nanoparticle were 12.5 nm and 69.34 emu g−1 respectively. The transverse relaxivity value of the water protons obtained in the presence of the core–shell nanoparticles was 184.1 mM−1 s−1. To investigate the effect of the core–shell geometry towards enhancing the relaxivity value, transverse relaxivity values were also obtained in the presence of separately synthesized single phase Fe3O4 and MnFe2O4 nanoparticles. Average size and saturation magnetization values for the as-synthesized Fe3O4 nanoparticles were 12 nm and 65.8 emu g−1 respectively. Average size and saturation magnetization values for the MnFe2O4 nanoparticles were 9 nm and 61.5 emu g−1 respectively. The transverse relaxivity value obtained in the presence of single phase Fe3O4 and MnFe2O4 nanoparticles was 96.6 and 83.2 mM−1 s−1 respectively. All the nanoparticles (core–shell and single phase) were coated with chitosan by a surfactant exchange reaction before determining the relaxivity values. For similar nanoparticle sizes and saturation magnetization values, the highest value of the transverse relaxivity in the case of core–shell nanoparticles clearly illustrated that the difference in the magnetic nature of the core and shell phases in the core–shell nanoparticles creates greater magnetic inhomogeneity in the surrounding medium yielding a high value for proton relaxivity. The MnFe2O4–Fe3O4 core–shell nanoparticles exhibited extremely low toxicity towards the MCF-7 cell line. Taken together, this opens up new avenues for the use of core–shell nanoparticles in MRI.
Recently, magnetic core–shell nanoparticles containing hard and soft magnetic phases have received wide attention due to exchange coupling between the magnetic phases which yields unique properties that can be technologically exploited.8–11 For example, exchange coupling in ferrite–ferrite core–shell nanoparticles has been exploited for localized heating and killing of cancer cells.10 Application of core–shell magnetic nanoparticles as hyperthermia agents is due to a phenomenon known as specific loss power (SLP). SLP is the ability of a system to generate heat when exposed to an electromagnetic field.12,13 Core–shell nanoparticles exhibit significantly higher SLP when compared to the SLP exhibited by single phase nanoparticles. The enhancement in the SLP value is essentially due to the interfacial exchange interaction between magnetic phases in core–shell geometry.10
In this paper, we introduce MnFe2O4–Fe3O4 core–shell nanoparticles system for application as a potential contrast agent material in MRI. MRI is now a widely used imaging technique in medical diagnosis.14 Use of contrast agent materials in MRI is essential for enhancing the probe sensitivity of the MRI technique.15–17 One of the most widely explored materials for use as contrast agent in MRI is magnetic nanoparticles and nanoparticle based systems.15–20 The candidate system chosen for this study is MnFe2O4–Fe3O4 core–shell nanoparticles. It should be noted that apart from widely investigated Fe3O4 nanoparticles for bio-medical imaging, the potential of MnFe2O4 nanoparticles for use as MRI contrast agent has been well established by the researchers.21,22 It has been shown that the MnFe2O4–Fe3O4 core–shell nanoparticles exhibit a very high value of SLP.10 This study exploits the fact that the differences in the magnetocrystalline anisotropy between the two magnetic phases in the core–shell nanoparticle induces relatively greater magnetic inhomogeneties in the vicinity of these core–shell nanoparticles when compared to the extent of inhomogeneity induced by single phase nanoparticles.23,24 Greater magnetic inhomogeneity can induce faster dephasing of the magnetic moments thus significantly reducing the T2 relaxation time and enhancing the transverse relaxivity of the water protons present in the medium surrounding the core–shell nanoparticles. core–shell nanoparticles exhibiting significantly high value of SLP and proton relaxivity can be used both for imaging the cancer cells and destroying it using localized heating.
To synthesize MnFe2O4 nanoparticles, Mn(acac)2 (1 mmol), Fe(acac)3 (2 mmol), 1,2-hexadecanediol (5 mmol), oleic acid (6 mmol), and oleylamine (6 mmol) and diphenyl ether (20 mL) were mixed in a three neck round bottom flask fitted with a magnetic stirrer and a reflux condenser. This reaction mixture was heated to 150 °C and kept at this temperature for 30 min. After 30 min, temperature of the reaction mixture was raised to ∼250 °C and refluxed for 30 min. The nanoparticle synthesis reaction occurred in argon atmosphere. After reflux, the black colored mixture containing precipitated nanoparticles was cooled down to room temperature. 40 mL of ethanol was then added into the nanoparticle dispersion to sediment the nanoparticles which were subsequently isolated by centrifugation.
To synthesize MnFe2O4–Fe3O4 core–shell nanoparticles, 40 mg of MnFe2O4 nanoparticles were dispersed in 20 mL of hexane by sonication. Into this solution, benzyl ether (20 mL), Fe(acac)3 (3 mmol), oleic acid (6 mmol), oleylamine (6 mmol) and 1,2-hexadecanediol (5 mmol) were added. This reaction mixture was then poured into a three neck round bottom flask fitted with a magnetic stirrer and a reflux condenser. The reaction mixture was heated to 100 °C and kept at this temperature for 1 h to evaporate away the hexane. Temperature of the reaction mixture was then raised to 200 °C and was kept at this temperature for 60 min. After this, the temperature of the reaction mixture was raised to 290 °C and was kept at this temperature for 60 min. After 60 min, the reaction mixture containing nanoparticles was allowed to cool down to the room temperature. 40 mL of ethanol was added into the reaction mixture to sediment the nanoparticles which were isolated by centrifugation. The core–shell nanoparticles obtained were then separated by centrifugation (8000 rpm, 10 min).
All NMR experiments were performed at 25 °C on a Bruker Avance-III NMR spectrometer operating at a 1H resonance frequency of 400 MHz. Samples were dissolved in 95% 2H2O and 5% H2O. The transverse relaxation of water (H2O) was measured using CPMG/T2-filter (Carr Purucell Meiboom Gill) NMR experiment.27 The relaxation delay time ‘τ’ was varied between 10 ms to 1 s collecting 12 data points to get the decay curve to extract T2 relaxation time constant. The 16 K complex points were collected with 1.1 s acquisition time and 7000 Hz spectral width. A relaxation delay of 15 s was given between scans.
Preparation of MnFe2O4–Fe3O4 nanoparticle solution: MnFe2O4–Fe3O4 core–shell nanoparticles were prepared in the cell culture media under laminar flow and sterile conditions. Nanoparticles were dispersed uniformly by low speed vortex. The concentrations used for the cytotoxicity assays with MnFe2O4–Fe3O4 core–shell nanoparticles were 100, 50, 25, 12.5 and 6.25 μg mL−1. Throughout this study, microgram per milliliter concentrations have been chosen as the unit of preference as they enable the response to be easily conceptualized in terms of number of particles, surface area and/or number of surface groups.
Average size of the seed and core–shell nanoparticles, obtained from the FWHM of the most intense (311) peak and the Scherrer formula30 was 4.5 and 12 nm respectively. Increase in the average size of the nanoparticles by ∼7 nm is due to the coating of the seed MnFe2O4 nanoparticles by the Fe3O4 phase. TEM bright field image of MnFe2O4 seed nanoparticles is provided in Fig. 2(a). It can be observed that the first step of the synthesis process has produced nearly spherical nanoparticles. SAD pattern obtained from the seed nanoparticles showing the presence of only ferrite phase is also shown in Fig. 2(a). Average size of the nanoparticles obtained from the summation average of sizes of 500 individual nanoparticles was 4.9 ± 0.5 nm. Histogram showing the distribution of seed nanoparticle sizes is provided in Fig. 2(b). TEM bright field image of MnFe2O4–Fe3O4 core–shell nanoparticles is provided in Fig. 2(c). SAD pattern obtained from the nanoparticles showing the presence of only ferrite phase is also shown in Fig. 2(c). Average size of the core–shell nanoparticles obtained from the summation average of sizes of 500 individual nanoparticles was 12.8 ± 1.1 nm. Histogram illustrating the distribution of the core–shell nanoparticle sizes is provided in Fig. 2(d). It can be observed from Fig. 2(c and d) that the synthesis method has produced core–shell nanoparticles with fairly narrow distribution in sizes. Narrow distribution in nanoparticle sizes and presence of negligible number of nanoparticles with sizes ∼5 nm clearly reveals that the reaction conditions adopted in the second step of the synthesis process led to uniform coating of the seed nanoparticles to form uniform core–shell nanoparticles. Core–shell geometry of the nanoparticles produced after the second step of the synthesis process was also confirmed by compositional line profile analysis of individual nanoparticles. A representative compositional line scan analysis result is provided in Fig. 2(e and f). Fig. 2(e) shows the STEM-HAADF image of a representative nanoparticle. The red line on the nanoparticle image is the path along which the compositional data was obtained using an electron probe of ∼1.5 nm size. The compositional profile (distance vs. counts) obtained for the Mn atoms is provided in Fig. 2(f). An abrupt increase in the EDS signal from the Mn elements in the middle of the nanoparticles shows that the core of the representative core–shell nanoparticles contained the MnFe2O4 phase.
Core–shell microstructure was also confirmed from the XPS based analysis of the seed and the core–shell nanoparticles produced respectively in the first and second step of the synthesis process. Fig. 3(a–c) respectively shows the XPS spectra of O1s, Mn2p and Fe2p obtained from the seed and core–shell nanoparticles. Fig. 3(d) shows the complete XPS spectrums. The O1s spectrums (in Fig. 3(c)) obtained from both the samples were deconvoluted into three peaks falling in the binding energy range of 526–533 eV. The peak at ∼528.5 eV corresponds to the lattice oxygen species O2− whereas the two peaks at the higher binding energy values of ∼529.5 and ∼530.5 eV correspond respectively to the hydroxyl and carboxyl group of the oleic acid adsorbed on the surface of nanoparticles.29 In Fig. 3(a), peaks at 641 and 653 eV corresponding respectively to the Mn2p3/2 and Mn2p1/2 of Mn2+ are observed only for the seed nanoparticles.31 The Mn2p spectrum of the core–shell nanoparticles do not show any peak suggesting the absence of MnFe2O4 phase on the surface of the core–shell nanoparticles. The Fe2p spectra (Fig. 3(b)) revealed peaks at ∼710 and ∼723.3 eV with the separation of 13.3 eV indicating the presence of Fe3+. The XPS results thus clearly revealed the formation of MnFe2O4–Fe3O4 core–shell nanoparticles.
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Fig. 3 XPS spectrums showing (a) Mn, (b) Fe (c) O peaks and (d) full XPS spectrum of MnFe2O4 seeds and MnFe2O4–Fe3O4 core–shell nanoparticles. |
Magnetic hysteresis curves obtained from MnFe2O4 seeds and MnFe2O4–Fe3O4 core–shell nanoparticles are shown in Fig. 4(a). Magnetic hysteresis curves were obtained at the room temperature using an applied field that varied in the range of 0–2 Tesla. As observed in Fig. 4(a), the magnetic hysteresis curves from both MnFe2O4 seeds and MnFe2O4–Fe3O4 core–shell nanoparticles reveal negligible coercivity and no magnetic saturation till 2 Tesla applied field. Both these attributes indicate that the as-synthesized seed and core–shell nanoparticles were superparamagnetic in nature. Saturation magnetization value obtained for the seed and the core–shell nanoparticles respectively was 69.34 and 50.75 emu g−1. Superparamagnetic nature was also confirmed from the occurrence of peak in the form of a broad hump in the ZFC curves for both the nanoparticles. ZFC curves are shown in Fig. 4(b). MnFe2O4 seed nanoparticles exhibit a clear hump in the ZFC curve. Whereas, the core–shell nanoparticles exhibit a broad peak at higher temperature. The shift of the ZFC curve peak was due to the increase in the nanoparticle size. The broadness of the ZFC curve for the case when the distribution between the particle sizes is narrow (as in the present case for core–shell nanoparticles) essentially illustrates interaction between magnetic spins at the MnFe2O4 and Fe3O4 interface.32
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Fig. 4 (a) M–H curves obtained from MnFe2O4 seeds and MnFe2O4–Fe3O4 core–shell nanoparticles and (b) zero field cooled (ZFC) curves obtained from seeds and core–shell nanoparticles. |
Transverse relaxivity of water protons in the presence of chitosan-coated MnFe2O4–Fe3O4 core–shell nanoparticles at different concentrations were measured using the NMR spin-echo method.33 The exponentially decaying curves obtained for all the samples at different concentrations of iron were used to calculate the transverse relaxivity (T2) values. The decay plots used for calculating the T2 of water protons in the presence of chitosan coated core shell nanoparticles are provided in Fig. 5(a). The data points were fitted according to the eqn (1)33
MXY(t) = MXY(0)e−t/T2 | (1) |
To illustrate the effect of exchange coupling towards enhancing the relaxivity value as observed in the present case of MnFe2O4–Fe3O4 core–shell nanoparticles, ∼9 nm sized MnFe2O4 nanoparticles and ∼12 nm sized Fe3O4 nanoparticles were also synthesized. Procedures used for the synthesis of single phase MnFe2O4 and Fe3O4 nanoparticles used for the comparative study are provided respectively in Section 2.2 and 2.3.
XRD profile, TEM bright field image and M–H curve obtained from the as-synthesized MnFe2O4 nanoparticles are shown in Fig. 6. The XRD profile in Fig. 6(a) reveals diffraction peaks corresponding only to the ferrite phase indicating that the synthesis process produced MnFe2O4 phase nanoparticles. Size of the nanoparticles obtained from the FWHM of the (311) peak and the Scherrer formula was 9 nm. TEM bright field image and SAD pattern obtained from as-synthesized nanoparticles is shown in Fig. 6(b). TEM bright field image reveals the formation of faceted nanoparticles. The SAD pattern shows diffraction rings corresponding to the MnFe2O4 phase. The size distribution histogram obtained from the as-synthesized nanoparticles is provided in Fig. 6(c). It can be seen that the nanoparticles are fairly uniform in size. Magnetic hysteresis curve obtained from MnFe2O4 nanoparticles using an applied magnetic field in the range of 0–2 Tesla are shown in Fig. 6(d). The magnetic hysteresis curve shows negligible coercivity and no magnetic saturation. Both these attributes illustrates the superparamagnetic nature of the as-synthesized MnFe2O4 nanoparticles. Saturation magnetization value obtained from the magnetic hysteresis curve was 61.5 emu g−1.
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Fig. 6 (a) XRD profile, (b) TEM bright field image and SAD pattern. (c) Size distribution histogram and (d) M vs. H curve obtained from 9 nm MnFe2O4 nanoparticles. |
XRD profile, TEM bright field image and M–H curve obtained for Fe3O4 nanoparticles are shown in Fig. 7. XRD curve obtained from the as-synthesized nanoparticles is shown in Fig. 7(a). The XRD profile shows diffraction peaks corresponding only to the Fe3O4 phase indicating that the synthesis process has produced Fe3O4 phase nanoparticles. Average size of the nanoparticles obtained from the FWHM of the (311) peak and the Scherrer formula was 12 nm. TEM bright field image and SAD pattern obtained from as-synthesized nanoparticles is shown in Fig. 7(b). TEM bright field image reveals the formation of faceted nanoparticles. The SAD pattern shows diffraction rings corresponding to the Fe3O4 phase. Size distribution histogram obtained from the as-synthesized Fe3O4 nanoparticles is provided in Fig. 7(c). It can be seen that the nanoparticle are fairly uniform in size. Magnetic hysteresis curve obtained from Fe3O4 nanoparticles using an applied magnetic field in the range of 0–2 tesla are shown in Fig. 7(d). The magnetic hysteresis curve shows negligible coercivity and no magnetic saturation. Both these attributes illustrate the superparamagnetic nature of the as-synthesized Fe3O4 nanoparticles. Saturation magnetization value obtained from the magnetic hysteresis curve was 65.8 emu g−1.
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Fig. 7 (a) XRD profile, (b) TEM bright field image and SAD pattern (c) size distribution histogram and (d) M vs. H curve obtained from 12 nm Fe3O4 nanoparticles. |
Transverse relaxivity of water protons in the presence of chitosan-coated 9 nm MnFe2O4 and 12 nm Fe3O4 were determined by the same method which was used for determining the relaxivity of water protons in the presence of MnFe2O4–Fe3O4 core–shell nanoparticles. 1/T2 vs. Fe concentration was plotted and r2 (transverse relaxivity) was obtained by determining the slope of the line fitted to the data points. The plots used for the calculation of r2 values are shown in Fig. 8.
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Fig. 8 1/T2 vs. Fe concentration curves of water protons in the presence of chitosan coated (a) 9 nm MnFe2O4 and (b) 12 nm Fe3O4 nanoparticles. |
Table 1 summarizes the values for the average size, saturation magnetization and transverse relaxivity obtained from the Fe3O4 nanoparticles, MnFe2O4 and MnFe2O4–Fe3O4 core–shell nanoparticles. It can be observed from Table 1 that the highest value of the transverse relaxivity is obtained for the core–shell nanoparticles eventhough the saturation magnetization values and nanoparticle sizes are similar for the three cases. The highest value of transverse relaxivity in the case of core–shell nanoparticles illustrates that these nanoparticles created largest magnetic inhomogeneity in the water medium surrounding them. The origin of the greater magnetic inhomogeneity was the difference in the magnetic nature of the MnFe2O4 and Fe3O4 phases in the core–shell nanoparticles.
Sample | Average size (nm) | Saturation magnetization (emu g−1) | Transverse relaxivity (mM−1 s−1) |
---|---|---|---|
MnFe2O4 | 9 | 61.5 | 83.2 |
Fe3O4 | 12 | 65.8 | 96.6 |
MnFe2O4–Fe3O4core–shell | 12.5 | 69.34 | 184.1 |
To investigate the cytotoxicity of the MnFe2O4–Fe3O4 core–shell nanoparticles, MTT assay was performed using MCF-7 (human breast cancer cells). Iron concentration of the chitosan coated nanoparticle dispersion was determined by AAS (Atomic Absorption Spectroscopy). The iron concentration of chitosan coated nanoparticles was determined by AAS. The standard solutions of 1, 2, 3, 4 and 5 ppm were prepared by using ferrous ammonium sulphate to obtain the calibration curve. 1 mL of nanoparticle dispersion, taken from the stock solution, containing chitosan coated core–shell nanoparticles were dissolved in 4 mL of concentrated H2SO4 contained in a 25 mL volumetric flask. Distill water was then added into the volumetric flask to fill it to 25 mL capacity. The absorbance value obtained for this solution was then used to determine the iron concentration in the stock solution using the calibration curve. Required volumes of the particle dispersion from the stock solution were then used for the MTT assay. Results from the cytotoxicity experiment shown in Fig. 9 clearly reveal that the core shell nanoparticles with different concentrations (100, 50, 25, 12.5 and 6.25 μg mL−1) are bio-compatible towards the MCF-7 cell line.
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Fig. 9 MTT assay of chitosan coated MnFe2O4–Fe3O4 core shell nanoparticles. Incubation time was 24 hours. |
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