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Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel
Cd(x)Ni(0.5−x)Cu(0.2)Zn(0.3)Fe(2)O(4) (0 ≤ x ≤ 0.50) ferrite with a spinel structure was prepared using the sol–gel self-propagation method. The effects of Cd(2+) doping on the structure, morphology, dielectric, and magnetic properties of Ni–Cu–Zn ferrite were examined using XRD, SEM, EDX, FTIR, MPM...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10459885/ https://www.ncbi.nlm.nih.gov/pubmed/37630362 http://dx.doi.org/10.3390/molecules28166110 |
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author | Yang, Hu Yang, Xingxing Lin, Jinpei Yang, Fang He, Yun Lin, Qing |
author_facet | Yang, Hu Yang, Xingxing Lin, Jinpei Yang, Fang He, Yun Lin, Qing |
author_sort | Yang, Hu |
collection | PubMed |
description | Cd(x)Ni(0.5−x)Cu(0.2)Zn(0.3)Fe(2)O(4) (0 ≤ x ≤ 0.50) ferrite with a spinel structure was prepared using the sol–gel self-propagation method. The effects of Cd(2+) doping on the structure, morphology, dielectric, and magnetic properties of Ni–Cu–Zn ferrite were examined using XRD, SEM, EDX, FTIR, MPMS, and dielectric tests. The cubic spinel structure was verified by XRD and FTIR analyses. The crystallite size and particle size information of the samples were obtained with XRD and SEM analysis. The sample particle size belonged to a class of nanoscale materials with a particle size range of 1–100 nm. The minor difference between the grain size and particle size indicated that the sample nanoparticles were composed of numerous microcrystals. The EDX spectra indicated that the samples contained all stoichiometric elements. MPMS was used to measure the hysteresis lines of the samples. According to the hysteresis line, the saturation magnetization intensity (M(s)), coercivity (H(c)), and magnetic moment (μ(B)) of the sample increased and then decreased with the increase in cadmium concentration. The magnetization strength (M(s)) is between 4–67 emu/g, and the coercivity (H(c)) is between 9–46 Oe. The curves of the real part of the dielectric constant (ε′), the imaginary part of the dielectric constant (ε″), and the loss factor (tanδ) with frequency were measured in the frequency range 100 Hz–100 kHz by means of an impedance analyzer. The complex modulus spectrum was analyzed to understand the dynamics of the conduction process. |
format | Online Article Text |
id | pubmed-10459885 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-104598852023-08-27 Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel Yang, Hu Yang, Xingxing Lin, Jinpei Yang, Fang He, Yun Lin, Qing Molecules Article Cd(x)Ni(0.5−x)Cu(0.2)Zn(0.3)Fe(2)O(4) (0 ≤ x ≤ 0.50) ferrite with a spinel structure was prepared using the sol–gel self-propagation method. The effects of Cd(2+) doping on the structure, morphology, dielectric, and magnetic properties of Ni–Cu–Zn ferrite were examined using XRD, SEM, EDX, FTIR, MPMS, and dielectric tests. The cubic spinel structure was verified by XRD and FTIR analyses. The crystallite size and particle size information of the samples were obtained with XRD and SEM analysis. The sample particle size belonged to a class of nanoscale materials with a particle size range of 1–100 nm. The minor difference between the grain size and particle size indicated that the sample nanoparticles were composed of numerous microcrystals. The EDX spectra indicated that the samples contained all stoichiometric elements. MPMS was used to measure the hysteresis lines of the samples. According to the hysteresis line, the saturation magnetization intensity (M(s)), coercivity (H(c)), and magnetic moment (μ(B)) of the sample increased and then decreased with the increase in cadmium concentration. The magnetization strength (M(s)) is between 4–67 emu/g, and the coercivity (H(c)) is between 9–46 Oe. The curves of the real part of the dielectric constant (ε′), the imaginary part of the dielectric constant (ε″), and the loss factor (tanδ) with frequency were measured in the frequency range 100 Hz–100 kHz by means of an impedance analyzer. The complex modulus spectrum was analyzed to understand the dynamics of the conduction process. MDPI 2023-08-17 /pmc/articles/PMC10459885/ /pubmed/37630362 http://dx.doi.org/10.3390/molecules28166110 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Yang, Hu Yang, Xingxing Lin, Jinpei Yang, Fang He, Yun Lin, Qing Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title | Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title_full | Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title_fullStr | Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title_full_unstemmed | Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title_short | Effect of Cd(2+) Substitution on Structural–Magnetic and Dielectric Properties of Ni–Cu–Zn Spinel Ferrite Nanomaterials by Sol–Gel |
title_sort | effect of cd(2+) substitution on structural–magnetic and dielectric properties of ni–cu–zn spinel ferrite nanomaterials by sol–gel |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10459885/ https://www.ncbi.nlm.nih.gov/pubmed/37630362 http://dx.doi.org/10.3390/molecules28166110 |
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