<p>The features of the magnetic structure of ultrasmall <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <!--JETPLet2560639Knyazev-m1--> </InlineEquation>-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 <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <!--JETPLet2560639Knyazev-m2--> </InlineEquation>-Fe<sub>2</sub>O<sub>3</sub> nanoparticles with an average size of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="67" /> </InlineMediaObject> <EquationSource Format="TEX">\(\langle d\rangle = 3.8\)</EquationSource> <!--JETPLet2560639Knyazev-m3--> </InlineEquation> 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 <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="47" /> </InlineMediaObject> <EquationSource Format="TEX">\(H = 4\)</EquationSource> <!--JETPLet2560639Knyazev-m4--> </InlineEquation> 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 <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <!--JETPLet2560639Knyazev-m5--> </InlineEquation>-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 <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq6.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\( \approx \)</EquationSource> <!--JETPLet2560639Knyazev-m6--> </InlineEquation>9 nm) <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11448_2025_4230_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="10" /> </InlineMediaObject> <EquationSource Format="TEX">\(\epsilon \)</EquationSource> <!--JETPLet2560639Knyazev-m7--> </InlineEquation>-Fe<sub>2</sub>O<sub>3</sub> particles, and the magnetic structure is noncollinear in the range of 4–300 K.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Suppression of the Magnetic Transition in Ultrasmall ϵ-Fe2O3 Nanoparticles: the Size Effect from Nuclear Forward Scattering Data

  • Yu. V. Knyazev,
  • D. A. Balaev,
  • A. A. Dubrovskiy,
  • S. V. Semenov,
  • V. L. Kirillov,
  • O. N. Martyanov

摘要

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.