Magnetic circular dichroism of f-f electron transitions in Ho3+ and Nd3+ ions in antiferromagnetic crystal Ho0.75Nd0.25Fe3(BO3)4 in the region of spin-reorientation transition
{"title":"Magnetic circular dichroism of f-f electron transitions in Ho3+ and Nd3+ ions in antiferromagnetic crystal Ho0.75Nd0.25Fe3(BO3)4 in the region of spin-reorientation transition","authors":"A.V. Malakhovskii, V.V. Sokolov, A.L. Sukhachev, I.A. Gudim","doi":"10.1016/j.jmmm.2024.172613","DOIUrl":null,"url":null,"abstract":"<div><div>Absorption and magnetic circular dichroism (MCD) spectra have been studied in the region of <sup>5</sup><em>I</em><sub>8</sub> → <sup>5</sup><em>F</em><sub>2</sub>, <sup>5</sup><em>S</em><sub>2</sub>, <sup>5</sup><em>F</em><sub>3</sub>, and <sup>5</sup><em>F</em><sub>5</sub> absorption bands of the Ho<sup>3+</sup> ion and in the region of <sup>4</sup><em>I</em><sub>9/2</sub>→<sup>4</sup><em>G</em><sub>7/2</sub>, <sup>2</sup><em>K</em><sub>13/2</sub>, <sup>4</sup><em>S</em><sub>3/2</sub>, <sup>4</sup><em>F</em><sub>7/2</sub>, <sup>4</sup><em>F</em><sub>5/2</sub> and <sup>2</sup><em>H</em><sub>9/2</sub> absorption bands of the Nd<sup>3+</sup> ion in an antiferromagnetic trigonal crystal Ho<sub>0.75</sub>Nd<sub>0.25</sub>Fe<sub>3</sub>(BO<sub>3</sub>)<sub>4</sub> in the temperature range from 5 to 90 K. A qualitative change in the shape of the MCD spectra of Ho<sup>3+</sup> ion was revealed during the spin-reorientation transition at <em>T</em><sub>R</sub> = 6.9 К. Below <em>T<sub>R</sub></em>, in the easy-axis state of the crystal, the MCD spectrum has a shape typical for paramagnets, i.e., it consists of diamagnetic and paramagnetic parts. Just above <em>T</em><sub>R</sub>, in the easy-plane state of the crystal, MCD of Ho<sup>3+</sup> ion has a spectrum similar to the absorption spectrum, which is typical for the paramagnetic part of the MCD. It was shown, that in the easy-plane state the exchange field of iron, being perpendicular to the external field directed along the <em>C</em><sub>3</sub> axis, quenches the usual paramagnetic and diamagnetic MCD in Ho<sup>3+</sup> ion, but creates a condition for the appearance of a large paramagnetic MCD of mixing (<em>B</em>-term). With temperature increasing, the MCD spectrum of Ho<sup>3+</sup> ion gradually turns into a spectrum typical for paramagnets with the predominance of the sign-changing diamagnetic part, because the influence of the exchange field decreases. The shape of the MCD spectra of Nd<sup>3+</sup> ions are typical for paramagnets but does not change during the reorientation transition in the rest of the crystal. This means that the magnetic moment of the Nd<sup>3+</sup> ion does not make a reorientation transition simultaneously with the Fe<sup>3+</sup> and Ho<sup>3+</sup> ions of the rest of the crystal. This phenomenon is accounted for by a strong local magnetic anisotropy of the Nd<sup>3+</sup> ion and by a weak exchange interaction Fe-Nd, which is not enough for rotation of the Nd<sup>3+</sup> ion moment synchronously with that of the Fe<sup>3+</sup> ion. The magneto-optical properties of neodymium are controlled by the easy-axis anisotropy of neodymium.</div></div>","PeriodicalId":366,"journal":{"name":"Journal of Magnetism and Magnetic Materials","volume":"611 ","pages":"Article 172613"},"PeriodicalIF":2.5000,"publicationDate":"2024-10-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnetism and Magnetic Materials","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0304885324009041","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Absorption and magnetic circular dichroism (MCD) spectra have been studied in the region of 5I8 → 5F2, 5S2, 5F3, and 5F5 absorption bands of the Ho3+ ion and in the region of 4I9/2→4G7/2, 2K13/2, 4S3/2, 4F7/2, 4F5/2 and 2H9/2 absorption bands of the Nd3+ ion in an antiferromagnetic trigonal crystal Ho0.75Nd0.25Fe3(BO3)4 in the temperature range from 5 to 90 K. A qualitative change in the shape of the MCD spectra of Ho3+ ion was revealed during the spin-reorientation transition at TR = 6.9 К. Below TR, in the easy-axis state of the crystal, the MCD spectrum has a shape typical for paramagnets, i.e., it consists of diamagnetic and paramagnetic parts. Just above TR, in the easy-plane state of the crystal, MCD of Ho3+ ion has a spectrum similar to the absorption spectrum, which is typical for the paramagnetic part of the MCD. It was shown, that in the easy-plane state the exchange field of iron, being perpendicular to the external field directed along the C3 axis, quenches the usual paramagnetic and diamagnetic MCD in Ho3+ ion, but creates a condition for the appearance of a large paramagnetic MCD of mixing (B-term). With temperature increasing, the MCD spectrum of Ho3+ ion gradually turns into a spectrum typical for paramagnets with the predominance of the sign-changing diamagnetic part, because the influence of the exchange field decreases. The shape of the MCD spectra of Nd3+ ions are typical for paramagnets but does not change during the reorientation transition in the rest of the crystal. This means that the magnetic moment of the Nd3+ ion does not make a reorientation transition simultaneously with the Fe3+ and Ho3+ ions of the rest of the crystal. This phenomenon is accounted for by a strong local magnetic anisotropy of the Nd3+ ion and by a weak exchange interaction Fe-Nd, which is not enough for rotation of the Nd3+ ion moment synchronously with that of the Fe3+ ion. The magneto-optical properties of neodymium are controlled by the easy-axis anisotropy of neodymium.
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