Yu. V. Knyazev, D. A. Balaev, A. A. Dubrovskiy, S. V. Semenov, V. L. Kirillov, O. N. Martyanov
{"title":"抑制超小ϵ-Fe2O3纳米颗粒的磁跃迁:核正向散射数据的尺寸效应","authors":"Yu. V. Knyazev, D. A. Balaev, A. A. Dubrovskiy, S. V. Semenov, V. L. Kirillov, O. N. Martyanov","doi":"10.1134/S0021364025606396","DOIUrl":null,"url":null,"abstract":"<p>The features of the magnetic structure of ultrasmall <span>\\(\\epsilon \\)</span>-Fe<sub>2</sub>O<sub>3</sub> nanoparticles have been studied by the nuclear forward scattering technique using synchrotron radiation. The sample consists of isolated <span>\\(\\epsilon \\)</span>-Fe<sub>2</sub>O<sub>3</sub> nanoparticles with an average size of <span>\\(\\langle d\\rangle = 3.8\\)</span> nm immobilized in a SiO<sub>2</sub> xerogel matrix. The time-domain spectra have been measured in the temperature range of 4–300 K in zero external magnetic field and field <span>\\(H = 4\\)</span> T applied in the longitudinal direction. The character of the change in the hyperfine field <i>H</i><sub>hf</sub> as a function of the external magnetic field is the same in the entire temperature range: unlike large <span>\\(\\epsilon \\)</span>-Fe<sub>2</sub>O<sub>3</sub> particles, a monotonic increase in <i>H</i><sub>hf</sub> is observed in the external field. These results indicate that there is no magnetic transition in the temperature range of 80–150 K for ultrasmall (smaller than <span>\\( \\approx \\)</span>9 nm) <span>\\(\\epsilon \\)</span>-Fe<sub>2</sub>O<sub>3</sub> particles, and the magnetic structure is noncollinear in the range of 4–300 K.</p>","PeriodicalId":604,"journal":{"name":"JETP Letters","volume":"121 10","pages":"800 - 805"},"PeriodicalIF":1.3000,"publicationDate":"2025-07-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1134/S0021364025606396.pdf","citationCount":"0","resultStr":"{\"title\":\"Suppression of the Magnetic Transition in Ultrasmall ϵ-Fe2O3 Nanoparticles: the Size Effect from Nuclear Forward Scattering Data\",\"authors\":\"Yu. V. Knyazev, D. A. Balaev, A. A. Dubrovskiy, S. V. Semenov, V. L. Kirillov, O. N. Martyanov\",\"doi\":\"10.1134/S0021364025606396\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The features of the magnetic structure of ultrasmall <span>\\\\(\\\\epsilon \\\\)</span>-Fe<sub>2</sub>O<sub>3</sub> nanoparticles have been studied by the nuclear forward scattering technique using synchrotron radiation. The sample consists of isolated <span>\\\\(\\\\epsilon \\\\)</span>-Fe<sub>2</sub>O<sub>3</sub> nanoparticles with an average size of <span>\\\\(\\\\langle d\\\\rangle = 3.8\\\\)</span> nm immobilized in a SiO<sub>2</sub> xerogel matrix. The time-domain spectra have been measured in the temperature range of 4–300 K in zero external magnetic field and field <span>\\\\(H = 4\\\\)</span> T applied in the longitudinal direction. The character of the change in the hyperfine field <i>H</i><sub>hf</sub> as a function of the external magnetic field is the same in the entire temperature range: unlike large <span>\\\\(\\\\epsilon \\\\)</span>-Fe<sub>2</sub>O<sub>3</sub> particles, a monotonic increase in <i>H</i><sub>hf</sub> is observed in the external field. These results indicate that there is no magnetic transition in the temperature range of 80–150 K for ultrasmall (smaller than <span>\\\\( \\\\approx \\\\)</span>9 nm) <span>\\\\(\\\\epsilon \\\\)</span>-Fe<sub>2</sub>O<sub>3</sub> particles, and the magnetic structure is noncollinear in the range of 4–300 K.</p>\",\"PeriodicalId\":604,\"journal\":{\"name\":\"JETP Letters\",\"volume\":\"121 10\",\"pages\":\"800 - 805\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2025-07-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1134/S0021364025606396.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"JETP Letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S0021364025606396\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"JETP Letters","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S0021364025606396","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Suppression of the Magnetic Transition in Ultrasmall ϵ-Fe2O3 Nanoparticles: the Size Effect from Nuclear Forward Scattering Data
The features of the magnetic structure of ultrasmall \(\epsilon \)-Fe2O3 nanoparticles have been studied by the nuclear forward scattering technique using synchrotron radiation. The sample consists of isolated \(\epsilon \)-Fe2O3 nanoparticles with an average size of \(\langle d\rangle = 3.8\) nm immobilized in a SiO2 xerogel matrix. The time-domain spectra have been measured in the temperature range of 4–300 K in zero external magnetic field and field \(H = 4\) T applied in the longitudinal direction. The character of the change in the hyperfine field Hhf as a function of the external magnetic field is the same in the entire temperature range: unlike large \(\epsilon \)-Fe2O3 particles, a monotonic increase in Hhf is observed in the external field. These results indicate that there is no magnetic transition in the temperature range of 80–150 K for ultrasmall (smaller than \( \approx \)9 nm) \(\epsilon \)-Fe2O3 particles, and the magnetic structure is noncollinear in the range of 4–300 K.
期刊介绍:
All topics of experimental and theoretical physics including gravitation, field theory, elementary particles and nuclei, plasma, nonlinear phenomena, condensed matter, superconductivity, superfluidity, lasers, and surfaces.