<p>In the present study, we observe how conductivity and magnetism in multiferroic spinels can be modulated through doping. Due to antiferromagnetic interaction between both cobalt-chromium and chromium-chromium ions in CoCr<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, the system has a frustrated magnetic structure. However, when the system is doped by iron then due to the dominant Fe-Co antiferromagnetic exchange interactions, the magnetic frustration in the system is overcome and the system becomes a collinear ferrimagnet. Our main focus in the present communication however is to understand how the spinel CoCr<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> becomes a half-metal as we dope it with iron and replace the Cr ions with Fe ions to gradually convert it into the inverse spinel CoFe<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq1.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>O<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10948_2025_7026_Article_IEq2.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="8" /> </InlineMediaObject> <EquationSource Format="TEX">\(_4\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>4</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>. The system is found to become half-metallic primarily due to the effect of cobalt ions in disordered state at the octahedral sites upon iron doping. This half-metallic nature makes the system suitable for spintronic based applications. The disorder-induced broadening of the otherwise narrow 3d bands of the cobalt species is identified as the primary cause of half-metallicity.</p>

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Promoting Half-metallicity in Spinels Through Doping

  • Shreemoyee Ganguly

摘要

In the present study, we observe how conductivity and magnetism in multiferroic spinels can be modulated through doping. Due to antiferromagnetic interaction between both cobalt-chromium and chromium-chromium ions in CoCr \(_2\) 2 O \(_4\) 4 , the system has a frustrated magnetic structure. However, when the system is doped by iron then due to the dominant Fe-Co antiferromagnetic exchange interactions, the magnetic frustration in the system is overcome and the system becomes a collinear ferrimagnet. Our main focus in the present communication however is to understand how the spinel CoCr \(_2\) 2 O \(_4\) 4 becomes a half-metal as we dope it with iron and replace the Cr ions with Fe ions to gradually convert it into the inverse spinel CoFe \(_2\) 2 O \(_4\) 4 . The system is found to become half-metallic primarily due to the effect of cobalt ions in disordered state at the octahedral sites upon iron doping. This half-metallic nature makes the system suitable for spintronic based applications. The disorder-induced broadening of the otherwise narrow 3d bands of the cobalt species is identified as the primary cause of half-metallicity.