Deciphering temperature-driven magnetic transformations and canting mechanism in the Y<sub>3</sub>Fe<sub>5-<i>x</i> </sub>Cd<i> <sub>x</sub> </i>O<sub>12</sub> compound: a coupled molecular field and phenomenological analysis

Their excellent electric and magnetic properties make the yttrium iron garnet (YIG)-based materials suitable for a wide variety of technological applications, such as microwave and magneto-optical devices. So, theoretical and experimental investigations are of great importance to understand and modify their properties. In this study, the Y<sub>3</sub>Fe<sub>5-<i>x</i></sub>Cd<i><sub>x</sub></i>O<sub>12</sub>compounds were synthesized via the sol-gel method for Cd doping levels of<i>x</i>= 0.00, 0.01, 0.03, 0.05, and 0.07. X-ray diffraction analysis revealed that the single YIG phase is maintained at 100% for<i>x</i>= 0.00 and 0.01, while minor secondary CdO phases are detected at higher doping levels, 0.13% for<i>x</i>= 0.03%, 1.17% for<i>x</i>= 0.05, and 4.42% for<i>x</i>= 0.07. Concurrently, the lattice parameter increased from 12.3808 Å (<i>x</i>= 0.00) to 12.4012 Å (<i>x</i>= 0.07), and the unit cell volume expanded from 1897.8 Å<sup>3</sup>to 1907.4 Å<sup>3</sup>, reflecting the incorporation of some Cd<sup>2+</sup>ions in place of Fe<sup>3+</sup>. Magnetic measurements performed between 100 K and 300 K indicated a systematic decrease in saturation magnetization (<i>M</i><sub>s</sub>) with increasing temperature. The experimental<i>M</i><sub>s</sub>values, determined by fitting the high-field data (800-10 000 Oe) with the law of approach to saturation, were quantitatively reproduced using a coupled theoretical model that integrates Dionne's modifications to the molecular field coefficients with a phenomenological analysis of cation distribution. The relevance of coupling the models lies in the dependence of the molecular field coefficients on cation distribution, which is critical for accurately calculating the saturation magnetization and understanding the underlying physical mechanisms. Remarkably, considering magnetic moment canting resulted in a maximum relative deviation of only 7.50% from experimental values, compared to discrepancies as high as 38.7% when assuming a collinear arrangement of magnetic moments. The preferential occupancy of Cd<sup>2+</sup>in octahedral sites, with an occupation probability seven orders of magnitude greater than in tetrahedral sites, further underlines its role in modulating the net magnetic moment.

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Journal
Journal of Physics Condensed Matter
Published
2025-07-24
DOI
https://doi.org/10.1088/1361-648x/adf3a2
Primary Topic
Advanced Condensed Matter Physics
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article
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Deciphering temperature-driven magnetic transformations and canting mechanism in the Y3Fe5-x Cd x O12 compound: a coupled molecular field and phenomenological analysis

E. Padrón‐Hernández, R. Peña‐Garcia, A. Franco, Y. Guerra et al.
Journal of Physics Condensed Matter
Advanced Condensed Matter Physics
article

Deciphering temperature-driven magnetic transformations and canting mechanism in the Y3Fe5-x Cd x O12 compound: a coupled molecular field and phenomenological analysis

E. Padrón‐Hernández, R. Peña‐Garcia, A. Franco, Y. Guerra, J. Matilla-Arias, F. Guerrero
article en

Abstract

Their excellent electric and magnetic properties make the yttrium iron garnet (YIG)-based materials suitable for a wide variety of technological applications, such as microwave and magneto-optical devices. So, theoretical and experimental investigations are of great importance to understand and modify their properties. In this study, the Y<sub>3</sub>Fe<sub>5-<i>x</i></sub>Cd<i><sub>x</sub></i>O<sub>12</sub>compounds were synthesized via the sol-gel method for Cd doping levels of<i>x</i>= 0.00, 0.01, 0.03, 0.05, and 0.07. X-ray diffraction analysis revealed that the single YIG phase is maintained at 100% for<i>x</i>= 0.00 and 0.01, while minor secondary CdO phases are detected at higher doping levels, 0.13% for<i>x</i>= 0.03%, 1.17% for<i>x</i>= 0.05, and 4.42% for<i>x</i>= 0.07. Concurrently, the lattice parameter increased from 12.3808 Å (<i>x</i>= 0.00) to 12.4012 Å (<i>x</i>= 0.07), and the unit cell volume expanded from 1897.8 Å<sup>3</sup>to 1907.4 Å<sup>3</sup>, reflecting the incorporation of some Cd<sup>2+</sup>ions in place of Fe<sup>3+</sup>. Magnetic measurements performed between 100 K and 300 K indicated a systematic decrease in saturation magnetization (<i>M</i><sub>s</sub>) with increasing temperature. The experimental<i>M</i><sub>s</sub>values, determined by fitting the high-field data (800-10 000 Oe) with the law of approach to saturation, were quantitatively reproduced using a coupled theoretical model that integrates Dionne's modifications to the molecular field coefficients with a phenomenological analysis of cation distribution. The relevance of coupling the models lies in the dependence of the molecular field coefficients on cation distribution, which is critical for accurately calculating the saturation magnetization and understanding the underlying physical mechanisms. Remarkably, considering magnetic moment canting resulted in a maximum relative deviation of only 7.50% from experimental values, compared to discrepancies as high as 38.7% when assuming a collinear arrangement of magnetic moments. The preferential occupancy of Cd<sup>2+</sup>in octahedral sites, with an occupation probability seven orders of magnitude greater than in tetrahedral sites, further underlines its role in modulating the net magnetic moment.

Journal of Physics Condensed MatterVol. 37(31)
Universidade Federal de Pernambuco (BR), University of Granma (CU), Universidade Federal do Amazonas (BR), Universidade Federal Rural de Pernambuco (BR), Universidade Federal de Goiás (BR), Universidade Federal de Alagoas (BR)
Openalex Percentile: Top 89%
Advanced Condensed Matter Physics
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