Spectral, electrical, magnetic and radiation shielding studies of Mg-doped Ni–Cu–Zn nanoferrites

Nanoferrites of Ni 0.1 Cu 0.2 Mg x Zn (0.7− x ) Fe 2 O 4 ( x  = 0.0, 0.15, 0.25, 0.35, 0.45, 0.55 and 0.70 wt%) system fabricated using flash auto combustion technique. All investigated samples annealed for 2 h at 600 °C. XRD, FTIR and TEM were utilized to evaluate the structural characterization of...

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Veröffentlicht in:Journal of materials science. Materials in electronics 2020-11, Vol.31 (22), p.20210-20222
Hauptverfasser: Henaish, A. M. A., Mostafa, M., Salem, B. I., Zakaly, Hesham M. H., Issa, Shams A. M., Weinstein, I. A., Hemeda, O. M.
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container_issue 22
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container_title Journal of materials science. Materials in electronics
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creator Henaish, A. M. A.
Mostafa, M.
Salem, B. I.
Zakaly, Hesham M. H.
Issa, Shams A. M.
Weinstein, I. A.
Hemeda, O. M.
description Nanoferrites of Ni 0.1 Cu 0.2 Mg x Zn (0.7− x ) Fe 2 O 4 ( x  = 0.0, 0.15, 0.25, 0.35, 0.45, 0.55 and 0.70 wt%) system fabricated using flash auto combustion technique. All investigated samples annealed for 2 h at 600 °C. XRD, FTIR and TEM were utilized to evaluate the structural characterization of as-prepared samples. The electrical DC resistivity of the investigated samples is evaluated as a function of frequency and temperature. The initial magnetic permeability ( μ i ) is dependent on the temperature and was measured at constant frequency 1 kHz and 10 kHz of the sinusoidal wave. A single-phase of spinel structure was formed and with increasing Mg content the peak (311) of 100% intensity decreases, which demonstrates the presence of Mg, which slows down the growth of the crystal as X-ray result. The FTIR spectra of the prepared ferrite samples are distinguished by the presence of two strong absorption bands ( ν 1  = 554 cm −1 ) and ( ν 2  = 449 cm −1 ). The morphological observation is determined by the transmission electron microscopy (TEM) and shows that the particles size ranged between 26 and 39 nm. It can notice shifted Curie temperature ( T c ) to a higher temperature by increasing Mg content. Mass attenuation coefficient ( μ m ), mean free path ( λ ), half value layer ( X 1/2 ), tenth value layer ( X 1/10 ) and effective atomic numbers ( Z eff ) for the studied samples, have been simulated using FLUKA (2020.0beta.2), while energy change from 15 × 10 –3 to 15 3+  keV with increasing Mg concentration, both μm and Zeff decrease. The largest value of μm and Zeff when x  = 0% while sample x  = 0.35% has a minimum value of λ , X 1/10 and X 1/2 .
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A single-phase of spinel structure was formed and with increasing Mg content the peak (311) of 100% intensity decreases, which demonstrates the presence of Mg, which slows down the growth of the crystal as X-ray result. The FTIR spectra of the prepared ferrite samples are distinguished by the presence of two strong absorption bands ( ν 1  = 554 cm −1 ) and ( ν 2  = 449 cm −1 ). The morphological observation is determined by the transmission electron microscopy (TEM) and shows that the particles size ranged between 26 and 39 nm. It can notice shifted Curie temperature ( T c ) to a higher temperature by increasing Mg content. Mass attenuation coefficient ( μ m ), mean free path ( λ ), half value layer ( X 1/2 ), tenth value layer ( X 1/10 ) and effective atomic numbers ( Z eff ) for the studied samples, have been simulated using FLUKA (2020.0beta.2), while energy change from 15 × 10 –3 to 15 3+  keV with increasing Mg concentration, both μm and Zeff decrease. 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The initial magnetic permeability ( μ i ) is dependent on the temperature and was measured at constant frequency 1 kHz and 10 kHz of the sinusoidal wave. A single-phase of spinel structure was formed and with increasing Mg content the peak (311) of 100% intensity decreases, which demonstrates the presence of Mg, which slows down the growth of the crystal as X-ray result. The FTIR spectra of the prepared ferrite samples are distinguished by the presence of two strong absorption bands ( ν 1  = 554 cm −1 ) and ( ν 2  = 449 cm −1 ). The morphological observation is determined by the transmission electron microscopy (TEM) and shows that the particles size ranged between 26 and 39 nm. It can notice shifted Curie temperature ( T c ) to a higher temperature by increasing Mg content. 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Materials in electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Henaish, A. M. A.</au><au>Mostafa, M.</au><au>Salem, B. I.</au><au>Zakaly, Hesham M. H.</au><au>Issa, Shams A. M.</au><au>Weinstein, I. A.</au><au>Hemeda, O. M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spectral, electrical, magnetic and radiation shielding studies of Mg-doped Ni–Cu–Zn nanoferrites</atitle><jtitle>Journal of materials science. Materials in electronics</jtitle><stitle>J Mater Sci: Mater Electron</stitle><date>2020-11-01</date><risdate>2020</risdate><volume>31</volume><issue>22</issue><spage>20210</spage><epage>20222</epage><pages>20210-20222</pages><issn>0957-4522</issn><eissn>1573-482X</eissn><abstract>Nanoferrites of Ni 0.1 Cu 0.2 Mg x Zn (0.7− x ) Fe 2 O 4 ( x  = 0.0, 0.15, 0.25, 0.35, 0.45, 0.55 and 0.70 wt%) system fabricated using flash auto combustion technique. All investigated samples annealed for 2 h at 600 °C. XRD, FTIR and TEM were utilized to evaluate the structural characterization of as-prepared samples. The electrical DC resistivity of the investigated samples is evaluated as a function of frequency and temperature. The initial magnetic permeability ( μ i ) is dependent on the temperature and was measured at constant frequency 1 kHz and 10 kHz of the sinusoidal wave. A single-phase of spinel structure was formed and with increasing Mg content the peak (311) of 100% intensity decreases, which demonstrates the presence of Mg, which slows down the growth of the crystal as X-ray result. The FTIR spectra of the prepared ferrite samples are distinguished by the presence of two strong absorption bands ( ν 1  = 554 cm −1 ) and ( ν 2  = 449 cm −1 ). The morphological observation is determined by the transmission electron microscopy (TEM) and shows that the particles size ranged between 26 and 39 nm. It can notice shifted Curie temperature ( T c ) to a higher temperature by increasing Mg content. Mass attenuation coefficient ( μ m ), mean free path ( λ ), half value layer ( X 1/2 ), tenth value layer ( X 1/10 ) and effective atomic numbers ( Z eff ) for the studied samples, have been simulated using FLUKA (2020.0beta.2), while energy change from 15 × 10 –3 to 15 3+  keV with increasing Mg concentration, both μm and Zeff decrease. The largest value of μm and Zeff when x  = 0% while sample x  = 0.35% has a minimum value of λ , X 1/10 and X 1/2 .</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10854-020-04541-x</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0002-9166-7497</orcidid></addata></record>
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subjects Absorption spectra
Atoms & subatomic particles
Attenuation coefficients
Characterization and Evaluation of Materials
Chemistry and Materials Science
Copper
Crystal growth
Curie temperature
Evaluation
Ferrites
Investigations
Magnesium
Magnetic fields
Magnetic permeability
Magnetic shielding
Materials Science
Morphology
Nanoparticles
Nickel
Optical and Electronic Materials
Permeability
Radiation
Radiation shielding
Sensors
Simulation
Sine waves
Structural analysis
Temperature dependence
Transmission electron microscopy
Zinc
title Spectral, electrical, magnetic and radiation shielding studies of Mg-doped Ni–Cu–Zn nanoferrites
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