Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites

Research output: Contribution to journalArticleResearchpeer review

Authors

  • Feriel Zdiri
  • José María Alonso
  • Taoufik Mnasri
  • Patricia de la Presa
  • Irene Morales
  • José Luis Martínez
  • Rached Ben Younes
  • Pilar Marin

External Research Organisations

  • University of Gafsa
  • Complutense University of Madrid (UCM)
  • Spanish National Research Council (CSIC)
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Details

Original languageEnglish
Article number1573
Pages (from-to)21
JournalMATERIALS
Volume16
Issue number4
Early online date13 Feb 2023
Publication statusPublished - Feb 2023
Externally publishedYes

Abstract

We have investigated the structural, magnetic, and electrical transport properties of Pr 0.7 Sr 0.3 Mn (1−x)Co x O 3 nanopowders (x = 0, 0.05, 0.10 and 0.15). The Pechini Sol-gel method was used to synthesize these nanopowders. X-ray diffraction at room temperature shows that all the nano powders have an orthorhombic structure of Pnma space group crystallography. The average crystallite size of samples x = 0, 0.05, 0.10, and 0.15 are 33.78 nm, 29 nm, 33.61 nm, and 24.27 nm, respectively. Semi-quantitative chemical analysis by energy dispersive spectroscopy (EDS) confirms the expected stoichiometry of the sample. Magnetic measurements indicate that all samples show a ferromagnetic (FM) to paramagnetic (PM) transition with increasing temperature. The Curie temperature T C gradually decreases (300 K, 270 K, 250 K, and 235 K for x = 0, 0.05, 0.10, and 0.15, respectively) with increasing Co concentrations. The M-H curves for all compounds reveal the PM behavior at 300 K, while the FM behavior characterizes the magnetic hysteresis at low temperature (5 K). The electrical resistivity measurements show that all compounds exhibit metallic behavior at low temperature (T < T (Formula presented.)) well fitted by the relation (Formula presented.) = (Formula presented.) 0 + (Formula presented.) 2T 2 + (Formula presented.) 4.5T 4.5 and semiconductor behavior above Tρ (T > T (Formula presented.)), for which the electronic transport can be explained by the variable range hopping model and the adiabatic small polaron hopping model. All samples have significant magnetoresistance (MR) values, even at room temperature. This presented research provides an innovative and practical approach to develop materials in several technological areas, such as ultra-high density magnetic recording and magneto resistive sensors.

Keywords

    magnetization, magnetoresistance (MR), Mn-perovskite, resistivity and electrical conduction, X-ray diffraction

ASJC Scopus subject areas

Cite this

Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites. / Zdiri, Feriel; Alonso, José María; Mnasri, Taoufik et al.
In: MATERIALS, Vol. 16, No. 4, 1573, 02.2023, p. 21.

Research output: Contribution to journalArticleResearchpeer review

Zdiri, F., Alonso, J. M., Mnasri, T., Presa, P. D. L., Morales, I., Martínez, J. L., Younes, R. B., & Marin, P. (2023). Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites. MATERIALS, 16(4), 21. Article 1573. https://doi.org/10.3390/ma16041573
Zdiri F, Alonso JM, Mnasri T, Presa PDL, Morales I, Martínez JL et al. Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites. MATERIALS. 2023 Feb;16(4):21. 1573. Epub 2023 Feb 13. doi: 10.3390/ma16041573
Zdiri, Feriel ; Alonso, José María ; Mnasri, Taoufik et al. / Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites. In: MATERIALS. 2023 ; Vol. 16, No. 4. pp. 21.
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abstract = "We have investigated the structural, magnetic, and electrical transport properties of Pr 0.7 Sr 0.3 Mn (1−x)Co x O 3 nanopowders (x = 0, 0.05, 0.10 and 0.15). The Pechini Sol-gel method was used to synthesize these nanopowders. X-ray diffraction at room temperature shows that all the nano powders have an orthorhombic structure of Pnma space group crystallography. The average crystallite size of samples x = 0, 0.05, 0.10, and 0.15 are 33.78 nm, 29 nm, 33.61 nm, and 24.27 nm, respectively. Semi-quantitative chemical analysis by energy dispersive spectroscopy (EDS) confirms the expected stoichiometry of the sample. Magnetic measurements indicate that all samples show a ferromagnetic (FM) to paramagnetic (PM) transition with increasing temperature. The Curie temperature T C gradually decreases (300 K, 270 K, 250 K, and 235 K for x = 0, 0.05, 0.10, and 0.15, respectively) with increasing Co concentrations. The M-H curves for all compounds reveal the PM behavior at 300 K, while the FM behavior characterizes the magnetic hysteresis at low temperature (5 K). The electrical resistivity measurements show that all compounds exhibit metallic behavior at low temperature (T < T (Formula presented.)) well fitted by the relation (Formula presented.) = (Formula presented.) 0 + (Formula presented.) 2T 2 + (Formula presented.) 4.5T 4.5 and semiconductor behavior above Tρ (T > T (Formula presented.)), for which the electronic transport can be explained by the variable range hopping model and the adiabatic small polaron hopping model. All samples have significant magnetoresistance (MR) values, even at room temperature. This presented research provides an innovative and practical approach to develop materials in several technological areas, such as ultra-high density magnetic recording and magneto resistive sensors.",
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T1 - Effects of Partial Manganese Substitution by Cobalt on the Physical Properties of Pr0.7Sr0.3Mn(1−x)CoxO3 (0 ≤ x ≤ 0.15) Manganites

AU - Zdiri, Feriel

AU - Alonso, José María

AU - Mnasri, Taoufik

AU - Presa, Patricia de la

AU - Morales, Irene

AU - Martínez, José Luis

AU - Younes, Rached Ben

AU - Marin, Pilar

N1 - Publisher Copyright: © 2023 by the authors.

PY - 2023/2

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N2 - We have investigated the structural, magnetic, and electrical transport properties of Pr 0.7 Sr 0.3 Mn (1−x)Co x O 3 nanopowders (x = 0, 0.05, 0.10 and 0.15). The Pechini Sol-gel method was used to synthesize these nanopowders. X-ray diffraction at room temperature shows that all the nano powders have an orthorhombic structure of Pnma space group crystallography. The average crystallite size of samples x = 0, 0.05, 0.10, and 0.15 are 33.78 nm, 29 nm, 33.61 nm, and 24.27 nm, respectively. Semi-quantitative chemical analysis by energy dispersive spectroscopy (EDS) confirms the expected stoichiometry of the sample. Magnetic measurements indicate that all samples show a ferromagnetic (FM) to paramagnetic (PM) transition with increasing temperature. The Curie temperature T C gradually decreases (300 K, 270 K, 250 K, and 235 K for x = 0, 0.05, 0.10, and 0.15, respectively) with increasing Co concentrations. The M-H curves for all compounds reveal the PM behavior at 300 K, while the FM behavior characterizes the magnetic hysteresis at low temperature (5 K). The electrical resistivity measurements show that all compounds exhibit metallic behavior at low temperature (T < T (Formula presented.)) well fitted by the relation (Formula presented.) = (Formula presented.) 0 + (Formula presented.) 2T 2 + (Formula presented.) 4.5T 4.5 and semiconductor behavior above Tρ (T > T (Formula presented.)), for which the electronic transport can be explained by the variable range hopping model and the adiabatic small polaron hopping model. All samples have significant magnetoresistance (MR) values, even at room temperature. This presented research provides an innovative and practical approach to develop materials in several technological areas, such as ultra-high density magnetic recording and magneto resistive sensors.

AB - We have investigated the structural, magnetic, and electrical transport properties of Pr 0.7 Sr 0.3 Mn (1−x)Co x O 3 nanopowders (x = 0, 0.05, 0.10 and 0.15). The Pechini Sol-gel method was used to synthesize these nanopowders. X-ray diffraction at room temperature shows that all the nano powders have an orthorhombic structure of Pnma space group crystallography. The average crystallite size of samples x = 0, 0.05, 0.10, and 0.15 are 33.78 nm, 29 nm, 33.61 nm, and 24.27 nm, respectively. Semi-quantitative chemical analysis by energy dispersive spectroscopy (EDS) confirms the expected stoichiometry of the sample. Magnetic measurements indicate that all samples show a ferromagnetic (FM) to paramagnetic (PM) transition with increasing temperature. The Curie temperature T C gradually decreases (300 K, 270 K, 250 K, and 235 K for x = 0, 0.05, 0.10, and 0.15, respectively) with increasing Co concentrations. The M-H curves for all compounds reveal the PM behavior at 300 K, while the FM behavior characterizes the magnetic hysteresis at low temperature (5 K). The electrical resistivity measurements show that all compounds exhibit metallic behavior at low temperature (T < T (Formula presented.)) well fitted by the relation (Formula presented.) = (Formula presented.) 0 + (Formula presented.) 2T 2 + (Formula presented.) 4.5T 4.5 and semiconductor behavior above Tρ (T > T (Formula presented.)), for which the electronic transport can be explained by the variable range hopping model and the adiabatic small polaron hopping model. All samples have significant magnetoresistance (MR) values, even at room temperature. This presented research provides an innovative and practical approach to develop materials in several technological areas, such as ultra-high density magnetic recording and magneto resistive sensors.

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