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© 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 164
Synthesis and characterization of structural and Magnetic Properties of
ZnO doped SnO2 Nano Composites
1aParveen Rathi, 2Manoj Kumar, 3Rajesh Sharma
1 Research Scholar, ECE Deptt., Om Sterling Global University, Hisar, Haryana (India)
2 Associate professor, ECE Deptt., Om Sterling Global University, Hisar, Haryana (India)
3Assistant professor, Physics Deptt., MNS Govt. College, Bhiwani, Haryana (India)
--------------------------------------------------------------------------***---------------------------------------------------------------------------
Abstract: The magnetic properties of SnO2 ZnO Nano
Composites nanoparticles of metal oxides are studied here.
The subjected nano composites nanoparticles of metal
oxides were synthesized using the chemical route method i.e.
microwave-assisted co-precipitation method. The
synthesized samples were characterized by the methods of
X-ray diffraction, FTIR Spectroscopy, UV-VIS Spectroscopy,
and vibrating sample magnetometer (VSM) for the magnetic
properties of the samples. The results suggest that samples
are of nano size and are magnetic. The hysteresis curves of
the samples results were analyzed and retentivity, coercivity,
and hysteresis loss of the samples were compared. The
comparative study suggests the applications of the samples
as per their properties of magnetic behavior.
Keywords: Magnetic, nano-materials, nano-composites,
Vibrating Sample Magnetometer
1. INTRODUCTION
The nano-composite materials have been the subject of
interest and complete study since long before. The interest
in the heterogeneous systems comprised of nanoparticles
is the thrust area/field because of their present and
prospective utilitarian applications. That these
nanoparticles are fundamentally related to the high
surface-to-volume ratio and the high total inter-facial area
of the embedded nanoparticles. Furthermore, many size-
dependent functional properties can be enriched by
nanoparticles and the hosting materials with interesting
multi-functionalities [1].
Magnetic nanoparticles are the most popular functional
nanofillers [2,3] for the thrust area. The magnetic
properties of the resultant nano-composites are affected
and sometimes are limited by various factors, such as the
degree of dispersion/aggregation of nanoparticles, the
strength ofinter-particle interactions, and the effect of the
surface on the nanoparticle's magnetism [4,5]. Some
aspects are still perplexing, such as the extent to which the
interface between magnetic nanoparticles and the given
enclosure influences their properties [6-12].
Since the fundamental principle of nano-magnetism has
long been established [13-14], a general prophetical
picture of the magnetic properties of a given nano-
composites or a family of nanocomposites are still not
clear. This is due to the number of parameters that are not
known completely and which obstruct the knowledge of
the physical processes at the nanoscale and this will affect
the interpretation of the measured magnetic properties of
the nano-composites [15-16].
2. RESEARCH METHODOLOGY
Experimental Synthesis Techniques: - The
formation of Ni-doped SnO2 was performed by using
microwave-assisted co-precipitation method in which
SnCl2.5H2O and Ni (NO3)2 were dissolved in 100ml of de-
ionized water with appropriate molar concentration. The
resultingsolution was continuously and steadily re-flexing
by using a magnetic stirrer for 1 hour at room temperature
to obtain a clear solution of acidic nature. Then ammonium
solution (NH4OH) was added dropwise with continuous
stirring into the solution so that its pH was maintained at a
value between 8 to 9 which was confirmed using a n
electrode pH meter (pH meter was calibrated byusing
buffer solution). The resultant precipitated solution was
kept for the aging process to stabilize uniform crystal size
for about 24 hours. Now, the precipitate was filtered by
using Whatman qualitative filter paper having pore size
(20-25micro meter). The obtained precipitate was
washed using distilled water and ethanol to release the
impurities such as nitrate and chloride.
The precipitate cake was heated for 4 hours at 100 oC
using a hot plate to remove water content. Now a part of
the resultant sample is grind in agate mortar and pestle
and sampling “as-synthesized sample” and other part was
further calcined at 200.0oC, 400 0oC and 600 0oC
respectively and formed in powder form by using agate
mortar and pestle. The as-synthesized sample, calcined
sample and various calcined samples were kept in an air-
tight container and used for further characterization
techniques.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072
© 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 165
Sample Characterization: Complementary methods
were used to exemplify the structure and phase of heat-
treated samples. XRD of samples were recorded by a
Philips X-ray diffractometer PW/1710; with Ni filter, with
monochromatic Cu Kα radiation of wavelength 1.5418 Å at
50 KV and 40 mA, in the range, 2θ~ 10-80°. The
investigation of the size, shape and particle distribution of
the samples was carried out using a Transmission electron
microscope (Hitachi-H7500) at 100 KV. For this intention,
the dispersion of sample nano-particles was pipettedonto
carbon-coated copper grids. Infrared spectra were
recorded by using Fourier transform infrared
spectrometer (Perkin Elmer 1600) ranging 2500-400 cm-
1, on the pellets obtained by dispersing the samples in
sodium bromide. UV visible spectrum was also recorded
for the nano-particles 12 through a UV visible
spectrometer. Vibrating Sample Magnetometer (V.S.M.)
facilities were availed in CEERI, Pilani (Rajasthan).
Vibrating Sample Magnetometer for Magnetic
measurement, M vs H (±1.5 T) was used for the magnetic
properties characterization for the field strength of ±1.5 T.
The system used is capable of studying the magnetic
properties of nano-composites, thin films, multi-layer and
hetero-structure materials. Further system can measure
and display Hall voltage, resistance, magneto resistance, I-
V characteristics, Hall coefficient, carrier concentration
and mobility of the given samples. The magnetic field
strength ranging in between ±1.5 T with 5 mm variable
magnetic air gap, magnetic field resolution is about 0
001Oe and magnetic field homogeneity is about + 0. 1 %
with over centered 50.8mm diameter circle uniform
working area. Micro Sense Easy VSM software version
9.13Wa is used for the data acquisition and analysis.
3. RESULTS AND DISCUSSION
XRD Analysis: In Powder X-ray diffraction
investigation, the crystalline phase of samples was
calculated at room temperature using Rigaku Mini flex
diffractometer with wavelength of radiation 1.54
Angstrom. In the x ray analysis, two matched Phases were
obtained such as tin oxide which is indexed as A and Zinc
oxide which is indexed as B. the observed xrd pattern
revealed the formation of nano-composites of tin oxide
with Zinc oxide. The experimental and calculated peaks
are well matched which signifies the formation of nano-
composites. The figure
5.1 shows the comparative study of nickle oxide nano-
composites.
4.2Fourier Transform Infrared (FTIR) Study: FTIR
spectra of the SnO2-ZnO. NCS were calcined at different
calcination temperatures 200 0 oC, 400 0 oC and 600 0 oC
for 2 hours, which are shown in Figure 1 Perusal of the
figure shows the IR broad peaks at around 3400 cm-1,
1600 cm-1, 607 cm-1 and 680 cm-1. A broad band
between 3600 cm-1-3330 cm-1 and broad band between
1700 cm-1 -1400 cm-1 have been at tributed to stretching
mode of -OH group, peaks at 607 cm-1 and 680 cm-1 were
attributed to different vibration modes of Sn-O-Sn and Ni-
O. At temperatures 200 oC, 400 oC, and 600 oC peaks
represent the formation of both Sn-O-Sn andNi-O but at
temperatures, 600 oC peaks are highly intense because
of increases in t h e lattice. Thetransmittance increases
with an increase in the calcination temperatures at the
fixed duration of heating 2 hours, It might be due to the
increase of the condensation of the oxygen during the
heating process
4.3Magnetic Properties: -Vibrating Sample
Magnetometer (VSM), the magnetic property of nano-
composites SnO2-ZnO was analyzed using a vibrating
sample magnetometer at roomtemperature. The magnetic
hysteresis loop of the calcined samples is shown in Figure
2 It is clear from the results that the calcined nano-
composites show a soft and ferromagnetic behavior.
It is clear from the magnetic hysteresis loop that the
coercive force decreases with an increase of t
h
e
temperature of ZnO in SnO2 nano-composites and the
retentivity also shows decrement with the increased
temperature. Furthermore, coercive force decreases in
very very small amounts with a
n increase in the
temperature of ZnO in SnO2 nano-composites.
Figure 1 SnO2-ZnO 10% NCS calcined for fixed duration
2 hours at (a) 200 oC (b) 400 oC
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072
© 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 166
(c) 600oC
Figure 2: FTIR Spectra of SnO2-ZnO 10% nano-
particles calcined for fixed duration of 2hours at
calcination temperatures (a) 200oC (b) 400oC (c)
600oC.
Figure 3 Hysteresis Loop of SnO2-ZnO 10% nano-
particles calcined for fixed duration of 2 hours
CONCLUSION: -
The experimental and calculated peaks x-ray diffraction
results are well matched and signify the formation of
nanocomposites. Figure 3 shows the comparative study
ofnickel oxide nano-composites. The FTIR results show
that the transmittance increases with increase in the
calcination temperatures at the fixed duration of heating 2
hours, It might be due to the increase of the condensation
of the oxygen during the heating process. It is clear from
the magnetic hysteresis loop that the coercive force
decreases with the increase of temperature of ZnO inSnO2
nano-composites and the retentivity also shows
decrement with the increased temperature. Furthermore,
coercive force decreases in very very small amount with
increase of temperature ofZnO in SnO2nano-composites.
Acknowledgements
The authors acknowledge their thanks to Principal and
technical staffs of MNS Govt. College, Bhiwani(Haryana) to
provide laboratory facility for synthesis work and the
technical staffs of Central Electronics Engineering
Research Institute, Pilani and Central Instrumentation
Laboratories, Panjab University, Chandigarh for the
characterization of thesamples.
References
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© 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 167
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Synthesis and characterization of structural and Magnetic Properties of ZnO doped SnO2 Nano Composites

  • 1. © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 164 Synthesis and characterization of structural and Magnetic Properties of ZnO doped SnO2 Nano Composites 1aParveen Rathi, 2Manoj Kumar, 3Rajesh Sharma 1 Research Scholar, ECE Deptt., Om Sterling Global University, Hisar, Haryana (India) 2 Associate professor, ECE Deptt., Om Sterling Global University, Hisar, Haryana (India) 3Assistant professor, Physics Deptt., MNS Govt. College, Bhiwani, Haryana (India) --------------------------------------------------------------------------***--------------------------------------------------------------------------- Abstract: The magnetic properties of SnO2 ZnO Nano Composites nanoparticles of metal oxides are studied here. The subjected nano composites nanoparticles of metal oxides were synthesized using the chemical route method i.e. microwave-assisted co-precipitation method. The synthesized samples were characterized by the methods of X-ray diffraction, FTIR Spectroscopy, UV-VIS Spectroscopy, and vibrating sample magnetometer (VSM) for the magnetic properties of the samples. The results suggest that samples are of nano size and are magnetic. The hysteresis curves of the samples results were analyzed and retentivity, coercivity, and hysteresis loss of the samples were compared. The comparative study suggests the applications of the samples as per their properties of magnetic behavior. Keywords: Magnetic, nano-materials, nano-composites, Vibrating Sample Magnetometer 1. INTRODUCTION The nano-composite materials have been the subject of interest and complete study since long before. The interest in the heterogeneous systems comprised of nanoparticles is the thrust area/field because of their present and prospective utilitarian applications. That these nanoparticles are fundamentally related to the high surface-to-volume ratio and the high total inter-facial area of the embedded nanoparticles. Furthermore, many size- dependent functional properties can be enriched by nanoparticles and the hosting materials with interesting multi-functionalities [1]. Magnetic nanoparticles are the most popular functional nanofillers [2,3] for the thrust area. The magnetic properties of the resultant nano-composites are affected and sometimes are limited by various factors, such as the degree of dispersion/aggregation of nanoparticles, the strength ofinter-particle interactions, and the effect of the surface on the nanoparticle's magnetism [4,5]. Some aspects are still perplexing, such as the extent to which the interface between magnetic nanoparticles and the given enclosure influences their properties [6-12]. Since the fundamental principle of nano-magnetism has long been established [13-14], a general prophetical picture of the magnetic properties of a given nano- composites or a family of nanocomposites are still not clear. This is due to the number of parameters that are not known completely and which obstruct the knowledge of the physical processes at the nanoscale and this will affect the interpretation of the measured magnetic properties of the nano-composites [15-16]. 2. RESEARCH METHODOLOGY Experimental Synthesis Techniques: - The formation of Ni-doped SnO2 was performed by using microwave-assisted co-precipitation method in which SnCl2.5H2O and Ni (NO3)2 were dissolved in 100ml of de- ionized water with appropriate molar concentration. The resultingsolution was continuously and steadily re-flexing by using a magnetic stirrer for 1 hour at room temperature to obtain a clear solution of acidic nature. Then ammonium solution (NH4OH) was added dropwise with continuous stirring into the solution so that its pH was maintained at a value between 8 to 9 which was confirmed using a n electrode pH meter (pH meter was calibrated byusing buffer solution). The resultant precipitated solution was kept for the aging process to stabilize uniform crystal size for about 24 hours. Now, the precipitate was filtered by using Whatman qualitative filter paper having pore size (20-25micro meter). The obtained precipitate was washed using distilled water and ethanol to release the impurities such as nitrate and chloride. The precipitate cake was heated for 4 hours at 100 oC using a hot plate to remove water content. Now a part of the resultant sample is grind in agate mortar and pestle and sampling “as-synthesized sample” and other part was further calcined at 200.0oC, 400 0oC and 600 0oC respectively and formed in powder form by using agate mortar and pestle. The as-synthesized sample, calcined sample and various calcined samples were kept in an air- tight container and used for further characterization techniques. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 165 Sample Characterization: Complementary methods were used to exemplify the structure and phase of heat- treated samples. XRD of samples were recorded by a Philips X-ray diffractometer PW/1710; with Ni filter, with monochromatic Cu Kα radiation of wavelength 1.5418 Å at 50 KV and 40 mA, in the range, 2θ~ 10-80°. The investigation of the size, shape and particle distribution of the samples was carried out using a Transmission electron microscope (Hitachi-H7500) at 100 KV. For this intention, the dispersion of sample nano-particles was pipettedonto carbon-coated copper grids. Infrared spectra were recorded by using Fourier transform infrared spectrometer (Perkin Elmer 1600) ranging 2500-400 cm- 1, on the pellets obtained by dispersing the samples in sodium bromide. UV visible spectrum was also recorded for the nano-particles 12 through a UV visible spectrometer. Vibrating Sample Magnetometer (V.S.M.) facilities were availed in CEERI, Pilani (Rajasthan). Vibrating Sample Magnetometer for Magnetic measurement, M vs H (±1.5 T) was used for the magnetic properties characterization for the field strength of ±1.5 T. The system used is capable of studying the magnetic properties of nano-composites, thin films, multi-layer and hetero-structure materials. Further system can measure and display Hall voltage, resistance, magneto resistance, I- V characteristics, Hall coefficient, carrier concentration and mobility of the given samples. The magnetic field strength ranging in between ±1.5 T with 5 mm variable magnetic air gap, magnetic field resolution is about 0 001Oe and magnetic field homogeneity is about + 0. 1 % with over centered 50.8mm diameter circle uniform working area. Micro Sense Easy VSM software version 9.13Wa is used for the data acquisition and analysis. 3. RESULTS AND DISCUSSION XRD Analysis: In Powder X-ray diffraction investigation, the crystalline phase of samples was calculated at room temperature using Rigaku Mini flex diffractometer with wavelength of radiation 1.54 Angstrom. In the x ray analysis, two matched Phases were obtained such as tin oxide which is indexed as A and Zinc oxide which is indexed as B. the observed xrd pattern revealed the formation of nano-composites of tin oxide with Zinc oxide. The experimental and calculated peaks are well matched which signifies the formation of nano- composites. The figure 5.1 shows the comparative study of nickle oxide nano- composites. 4.2Fourier Transform Infrared (FTIR) Study: FTIR spectra of the SnO2-ZnO. NCS were calcined at different calcination temperatures 200 0 oC, 400 0 oC and 600 0 oC for 2 hours, which are shown in Figure 1 Perusal of the figure shows the IR broad peaks at around 3400 cm-1, 1600 cm-1, 607 cm-1 and 680 cm-1. A broad band between 3600 cm-1-3330 cm-1 and broad band between 1700 cm-1 -1400 cm-1 have been at tributed to stretching mode of -OH group, peaks at 607 cm-1 and 680 cm-1 were attributed to different vibration modes of Sn-O-Sn and Ni- O. At temperatures 200 oC, 400 oC, and 600 oC peaks represent the formation of both Sn-O-Sn andNi-O but at temperatures, 600 oC peaks are highly intense because of increases in t h e lattice. Thetransmittance increases with an increase in the calcination temperatures at the fixed duration of heating 2 hours, It might be due to the increase of the condensation of the oxygen during the heating process 4.3Magnetic Properties: -Vibrating Sample Magnetometer (VSM), the magnetic property of nano- composites SnO2-ZnO was analyzed using a vibrating sample magnetometer at roomtemperature. The magnetic hysteresis loop of the calcined samples is shown in Figure 2 It is clear from the results that the calcined nano- composites show a soft and ferromagnetic behavior. It is clear from the magnetic hysteresis loop that the coercive force decreases with an increase of t h e temperature of ZnO in SnO2 nano-composites and the retentivity also shows decrement with the increased temperature. Furthermore, coercive force decreases in very very small amounts with a n increase in the temperature of ZnO in SnO2 nano-composites. Figure 1 SnO2-ZnO 10% NCS calcined for fixed duration 2 hours at (a) 200 oC (b) 400 oC
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 166 (c) 600oC Figure 2: FTIR Spectra of SnO2-ZnO 10% nano- particles calcined for fixed duration of 2hours at calcination temperatures (a) 200oC (b) 400oC (c) 600oC. Figure 3 Hysteresis Loop of SnO2-ZnO 10% nano- particles calcined for fixed duration of 2 hours CONCLUSION: - The experimental and calculated peaks x-ray diffraction results are well matched and signify the formation of nanocomposites. Figure 3 shows the comparative study ofnickel oxide nano-composites. The FTIR results show that the transmittance increases with increase in the calcination temperatures at the fixed duration of heating 2 hours, It might be due to the increase of the condensation of the oxygen during the heating process. It is clear from the magnetic hysteresis loop that the coercive force decreases with the increase of temperature of ZnO inSnO2 nano-composites and the retentivity also shows decrement with the increased temperature. Furthermore, coercive force decreases in very very small amount with increase of temperature ofZnO in SnO2nano-composites. Acknowledgements The authors acknowledge their thanks to Principal and technical staffs of MNS Govt. College, Bhiwani(Haryana) to provide laboratory facility for synthesis work and the technical staffs of Central Electronics Engineering Research Institute, Pilani and Central Instrumentation Laboratories, Panjab University, Chandigarh for the characterization of thesamples. References 1. Chou, T.-W.; Sun, C.-T. Nanocomposites; DEStech Publications: Lancaster, PA, USA, 2012; ISBN 9781605950730. 2. Ajayan, P.M.; Schadler, L.S.; Braun, P.V. Nanocomposite Science and Technology, Wiley- VCH Verlag GmbH & Co. KGaA:Weinheim, Germany, 2003; ISBN 3527303596. 3. Alamri, H. Synthesis of New Magnetic Nanocomposite Materials for Data Storage. Master’s Thesis, University ofWaterloo,Waterloo, ON, Canada, 2012. 4. Koksharov, Y.A. Magnetism of Nanoparticles: Effects of Size, Shape, and Interactions. In Magnetic Nanoparticles; Gubin, S.P., Ed.; Wiley-VCH Verlag GmbH & Co. KGaA: Weinheim, Germany, 2009; pp. 197–254. 5. Allia, P.; Barrera, G.; Tiberto, P.; Nardi, T.; Leterrier, Y.; Sangermano, M. Fe3O4 nanoparticles and nanocomposites with potential application in biomedicine and in communication technologies: Nanoparticle aggregation, interaction, and effective magnetic anisotropy. J. Appl. Phys. 2014, 116. [CrossRef] 6. Manna, P.K.; Yusuf, S.M. Two interface effects: Exchange bias and magnetic proximity. Phys. Rep. 2014, 535, 61–99. [CrossRef] 7. Binns, C.; Domingo, N.; Testa, A.M.; Fiorani, D.; Trohidou, K.N.; Vasilakaki, M.; Blackman, J.A.; Asaduzzaman, A.M.; Baker, S.; Roy, M.; et al. Interface
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 10 Issue: 09 | Sep 2023 www.irjet.net p-ISSN: 2395-0072 © 2023, IRJET | Impact Factor value: 8.226 | ISO 9001:2008 Certified Journal | Page 167 exchange coupling in Co nanoparticles dispersed in a Mn matrix. J. Phys. Condens. Matter 2010, 22. [CrossRef] [PubMed] 8. Coey, J.M.D. Magnetism and Magnetic Materials; Cambridge University Press: Cambridge, UK, 2009; ISBN 9780521816144. 9. Colvin, V.L. The potential environmental impact of engineered nanomaterials. Nat. Biotechnol. 2003, 21, 1166–1170. [CrossRef] [PubMed] 10. Meyer, D.E.; Curran, M.A.; Gonzalez, M.A. An examination of existing data for the industrial manufacture and use of nanocomponents and their role in the life cycle impact of nanoproducts. Environ. Sci. Technol. 2009, 43, 1256–1263. [CrossRef] [PubMed] Appl. Sci. 2019, 9, 212 25 of 28 11. Nardi, T.; Sangermano, M.; Leterrier, Y.; Allia, P.; Tiberto, P.; Månson, J.A.E. UV-cured transparent magnetic polymer nanocomposites. Polymer 2013, 54, 4472–4479. [CrossRef] 12. Allia, P.; Tiberto, P.; Coisson, M.; Chiolerio, A.; Celegato, F.; Vinai, F.; Sangermano, M.; Suber, L.; Marchegiani, G. Evidence for magnetic interactions among magnetite nanoparticles dispersed in photoreticulated PEGDA-600 matrix. J. Nanopart. Res. 2011, 13, 5615–5626. [CrossRef] 13. Sciancalepore, C.; Bondioli, F.; Messori, M. Non- hydrolytic sol–gel synthesis and reactive suspension method: An innovative approach to obtaining magnetite– epoxy nanocomposite materials. J. Sol-Gel Sci. Technol. 2017, 81, 69–83. [CrossRef] 14. Esposito, S.; Dell’Agli, G.; Marocco, A.; Bonelli, B.; Allia, P.; Tiberto, P.; Barrera, G.; Manzoli, M.; Arletti, R.; Pansini, M. Magnetic metal-ceramic nanocomposites obtained from cation-exchanged zeolite by heat treatment in reducing atmosphere. Microporous Mesoporous Mater. 2018, 268, 131–143. [CrossRef] 15. Knobel, M.; Nunes, W.C.; Socolovsky, L.M.; De Biasi, E.; Vargas, J.M.; Denardin, J.C. Superparamagnetism and Other Magnetic Features in Granular Materials: A Review on Ideal and Real Systems. J. Nanosci. Nanotechnol. 2008, 8, 2836–2857. [CrossRef] 16. Gabriele Barrera , Paola Tiberto, Paolo Allia, Barbara Bonelli, Serena Esposito, Antonello Marocco, Michele Pansini and Yves Leterrier. Review Magnetic Properties of Nanocomposites Appl. Sci. 2019, 9, 212.