<p>Co<sub>0.5</sub>Zn<sub>0.5</sub>Er<sub>x</sub>Fe<sub>2−x</sub>O<sub>4</sub> <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((x=0.00-0.10)\)</EquationSource> </InlineEquation>&#xa0;nanoferrites were synthesized by a sol–gel auto-combustion route to examine the effect of Er³⁺ on structural, microstructural, vibrational, thermal, and magnetic characteristics. X-ray diffraction with Rietveld refinement confirmed a single-phase cubic spinel (Fd–3&#xa0;m) with a near-linear Vegard-type increase in lattice parameter from 8.3954 Å <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\((x=0.00)\)</EquationSource> </InlineEquation>&#xa0;to 8.4118 Å <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\((x=0.08)\)</EquationSource> </InlineEquation>&#xa0;and a slight relaxation at <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(x=0.10\)</EquationSource> </InlineEquation>, consistent with B-site Er³⁺ substitution under a constrained Bertaut distribution. Williamson–Hall analysis showed a reduction of coherent domain size from 38.3&#xa0;nm to 16.6&#xa0;nm across the series. Thermal analysis gave a total mass loss of <b>~</b> 11.24% with a dominant crystallization exotherm at <b>~</b> 318&#xa0;°C (low end of the typical 300–450&#xa0;°C range), and negligible mass change beyond <b>~</b> 450&#xa0;°C, indicating thermal stability. FTIR spectra exhibited the characteristic M–O bands near <b>~</b> 530&#xa0;cm⁻<sup>1</sup> (A-site) and <b>~</b> 420&#xa0;cm⁻<sup>1</sup> (B-site), both blue-shifting with <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(x\)</EquationSource> </InlineEquation>; the corresponding force constants increase modestly, supporting octahedral-sublattice perturbation. FESEM revealed irregular, plate-like agglomerates, while TEM/HRTEM showed clear spinel lattice fringes (with <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({D}_{\text{W}\text{H}}\le\:{D}_{\text{T}\text{E}\text{M}}\)</EquationSource> </InlineEquation>, as expected). VSM confirmed soft ferrimagnetic behavior at 300&#xa0;K with very low coercivity (<b>~</b> 1.5–2.0 Oe) and a decrease in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({M}_{s}\)</EquationSource> </InlineEquation>&#xa0;from 28.4 to 21.2 emu·g⁻<sup>1</sup> due to B-site moment dilution and enhanced surface spin canting. These results establish phase-pure Co–Zn–Er spinels with soft-magnetic behavior, indicating potential for high-frequency uses; however, application-specific validation requires frequency-dependent dielectric/permeability and RF-loss measurements.</p>

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Tailoring Structural and Magnetic Properties of Co–Zn Ferrite Nanoparticles via Erbium Substitution

  • Priti A. Ingle,
  • S. B. Kadam,
  • Rameshwar B. Borade,
  • Ketan P. Gattu,
  • V. D. Mote,
  • R. H. Kadam,
  • S. S. More

摘要

Co0.5Zn0.5ErxFe2−xO4 \((x=0.00-0.10)\)  nanoferrites were synthesized by a sol–gel auto-combustion route to examine the effect of Er³⁺ on structural, microstructural, vibrational, thermal, and magnetic characteristics. X-ray diffraction with Rietveld refinement confirmed a single-phase cubic spinel (Fd–3 m) with a near-linear Vegard-type increase in lattice parameter from 8.3954 Å \((x=0.00)\)  to 8.4118 Å \((x=0.08)\)  and a slight relaxation at \(x=0.10\) , consistent with B-site Er³⁺ substitution under a constrained Bertaut distribution. Williamson–Hall analysis showed a reduction of coherent domain size from 38.3 nm to 16.6 nm across the series. Thermal analysis gave a total mass loss of ~ 11.24% with a dominant crystallization exotherm at ~ 318 °C (low end of the typical 300–450 °C range), and negligible mass change beyond ~ 450 °C, indicating thermal stability. FTIR spectra exhibited the characteristic M–O bands near ~ 530 cm⁻1 (A-site) and ~ 420 cm⁻1 (B-site), both blue-shifting with \(x\) ; the corresponding force constants increase modestly, supporting octahedral-sublattice perturbation. FESEM revealed irregular, plate-like agglomerates, while TEM/HRTEM showed clear spinel lattice fringes (with \({D}_{\text{W}\text{H}}\le\:{D}_{\text{T}\text{E}\text{M}}\) , as expected). VSM confirmed soft ferrimagnetic behavior at 300 K with very low coercivity (~ 1.5–2.0 Oe) and a decrease in \({M}_{s}\)  from 28.4 to 21.2 emu·g⁻1 due to B-site moment dilution and enhanced surface spin canting. These results establish phase-pure Co–Zn–Er spinels with soft-magnetic behavior, indicating potential for high-frequency uses; however, application-specific validation requires frequency-dependent dielectric/permeability and RF-loss measurements.