Magnetic properties of Sr0.95Nd0.05Fe12-xScxO19 hexaferrite nanoparticles

Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters increasing continuously with x was proved by X-ray diffraction. Scanning electron microscope control of the microstructure shows a decrease...

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Published inJournal of alloys and compounds Vol. 852; p. 156969
Main Authors Hilczer, Andrzej, Pasińska, Katarzyna
Format Journal Article
LanguageEnglish
Published Lausanne Elsevier B.V 25.01.2021
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Abstract Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters increasing continuously with x was proved by X-ray diffraction. Scanning electron microscope control of the microstructure shows a decrease in particle size with increasing x from 1000 to ∼250 nm. Saturated hysteresis loops were obtained in field of 5 T and magnetization switching via curling mode was observed for crystallites with sizes from 1000 to ∼600 nm. For smaller particles magnetization was switched via coherent reorientation. The effect of doping on magnetic properties was apparent in samples containing more than one Sc3+ ion substituting Fe3+ pro one unit cell (x ≥ 0.60). The saturation magnetization was found to increase on cooling from 300 K and for samples with x ≥ 0.60 exhibits local maximum at Tcone temperatures considerably lower in comparison with those of bulk counterparts. The appearance of conical magnetic order is reflected in temperature dependences of extrinsic magnetic properties, coercivity and remanence, which decrease also on doping. Temperature variation of magnetization in zero field cooling/field cooling modes shows that Tcone is shifted downwards with increasing field. [Display omitted] •Sr0.95Nd0.05Fe12-xScxO19 nanocrystallites 50–100 nm thick, 250–1000 nm in diameter.•Size effect distinguished in magnetization switching curling and coherent modes.•Changes in magnetic properties apparent from concentrations >1 Sc/unit cell.•Conical magnetization appears at T ∼100 K lower than in bulk counterparts.
AbstractList Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters increasing continuously with x was proved by X-ray diffraction. Scanning electron microscope control of the microstructure shows a decrease in particle size with increasing x from 1000 to ∼250 nm. Saturated hysteresis loops were obtained in field of 5 T and magnetization switching via curling mode was observed for crystallites with sizes from 1000 to ∼600 nm. For smaller particles magnetization was switched via coherent reorientation. The effect of doping on magnetic properties was apparent in samples containing more than one Sc3+ ion substituting Fe3+ pro one unit cell (x ≥ 0.60). The saturation magnetization was found to increase on cooling from 300 K and for samples with x ≥ 0.60 exhibits local maximum at Tcone temperatures considerably lower in comparison with those of bulk counterparts. The appearance of conical magnetic order is reflected in temperature dependences of extrinsic magnetic properties, coercivity and remanence, which decrease also on doping. Temperature variation of magnetization in zero field cooling/field cooling modes shows that Tcone is shifted downwards with increasing field.
Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters increasing continuously with x was proved by X-ray diffraction. Scanning electron microscope control of the microstructure shows a decrease in particle size with increasing x from 1000 to ∼250 nm. Saturated hysteresis loops were obtained in field of 5 T and magnetization switching via curling mode was observed for crystallites with sizes from 1000 to ∼600 nm. For smaller particles magnetization was switched via coherent reorientation. The effect of doping on magnetic properties was apparent in samples containing more than one Sc3+ ion substituting Fe3+ pro one unit cell (x ≥ 0.60). The saturation magnetization was found to increase on cooling from 300 K and for samples with x ≥ 0.60 exhibits local maximum at Tcone temperatures considerably lower in comparison with those of bulk counterparts. The appearance of conical magnetic order is reflected in temperature dependences of extrinsic magnetic properties, coercivity and remanence, which decrease also on doping. Temperature variation of magnetization in zero field cooling/field cooling modes shows that Tcone is shifted downwards with increasing field. [Display omitted] •Sr0.95Nd0.05Fe12-xScxO19 nanocrystallites 50–100 nm thick, 250–1000 nm in diameter.•Size effect distinguished in magnetization switching curling and coherent modes.•Changes in magnetic properties apparent from concentrations >1 Sc/unit cell.•Conical magnetization appears at T ∼100 K lower than in bulk counterparts.
ArticleNumber 156969
Author Pasińska, Katarzyna
Hilczer, Andrzej
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  givenname: Katarzyna
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  organization: Institute of Low Temperature and Structure Research, Polish Academy of Sciences, Okólna 2, 50-422, Wrocław, Poland
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Keywords Magnetic measurements
Hexaferrite
Citric sol-gel method
Size effect
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Snippet Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters...
Sr0.95Nd0.05Fe12-xScxO19 (0 ≤ x ≤ 1.56) nanocrystallites, 50–100 nm thick, were obtained by citric sol-gel method. Single P63/mmc phase with lattice parameters...
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SubjectTerms Citric sol-gel method
Coercivity
Cooling
Crystallites
Doping
Hexaferrite
Hysteresis loops
Lattice parameters
Lattice vibration
Magnetic measurements
Magnetic properties
Magnetic saturation
Magnetism
Magnetization
Nanoparticles
Remanence
Size effect
Sol-gel processes
Unit cell
Title Magnetic properties of Sr0.95Nd0.05Fe12-xScxO19 hexaferrite nanoparticles
URI https://dx.doi.org/10.1016/j.jallcom.2020.156969
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