<p>In our previous research, varying Ni concentration in a Mg-doped CuCrO<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_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> matrix enhanced the Seebeck coefficient via carrier–magnon drag, but the overall power factor remained low. In this work, a modified synthesis strategy and precise dopant control enabled the decoupling of thermoelectric parameters, enhancing carrier mobility through Mg<InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-induced potential barriers in Ni<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-doped CuCrO<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_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>. X-ray diffraction (XRD) confirms the incorporation of Mg<InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> and structural modifications, while vibrating sample magnetometry (VSM) reveals Ni<InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation>-driven collinear spin ordering in the frustrated CuCrO<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_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> lattice. Magnetoresistance studies further elucidate the interaction between non-magnetic Mg<InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq4.gif" Format="GIF" Height="11" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{2+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </mmultiscripts> </math></EquationSource> </InlineEquation> and magnetic ordering, shedding light on its impact on transport behavior. This structural and magnetic reconfiguration enhances spin entropy, contributing to an increased Seebeck coefficient (317 <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq11.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="15" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mu\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation>V/K) and electrical conductivity (6779&#xa0;S/m) at 700<InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq12.gif" Format="GIF" Height="7" Rendition="HTML" Resolution="72" Type="Linedraw" Width="9" /> </InlineMediaObject> <EquationSource Format="TEX">\(^\circ\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mo>∘</mo> </mmultiscripts> </math></EquationSource> </InlineEquation>C. The interplay of these effects results in a record-high power factor (0.722 mW/mK<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq13.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 /> <mrow /> <mn>2</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>) among Cu-based delafossites. In addition, thermal conductivity measurements confirm a reduced <InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_15526_Article_IEq14.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>κ</mi> </math></EquationSource> </InlineEquation> of 2.84 W/mK, attributed to increased phonon scattering at Mg-induced interfaces. This study provides direct experimental evidence of interlamellar porosity and spin-driven transport mechanisms, offering new insights into structural tuning for high-performance thermoelectrics.</p>

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Structural and magnetic modifications in Ni–Mg dual-doped CuCrO\(_2\): Insights into carrier filtering and thermoelectric enhancement

  • Jamshina Sanam P.K,
  • Midhun Shah,
  • P.P. Pradyumnan

摘要

In our previous research, varying Ni concentration in a Mg-doped CuCrO \(_2\) 2 matrix enhanced the Seebeck coefficient via carrier–magnon drag, but the overall power factor remained low. In this work, a modified synthesis strategy and precise dopant control enabled the decoupling of thermoelectric parameters, enhancing carrier mobility through Mg \(^{2+}\) 2 + -induced potential barriers in Ni \(^{2+}\) 2 + -doped CuCrO \(_2\) 2 . X-ray diffraction (XRD) confirms the incorporation of Mg \(^{2+}\) 2 + and structural modifications, while vibrating sample magnetometry (VSM) reveals Ni \(^{2+}\) 2 + -driven collinear spin ordering in the frustrated CuCrO \(_2\) 2 lattice. Magnetoresistance studies further elucidate the interaction between non-magnetic Mg \(^{2+}\) 2 + and magnetic ordering, shedding light on its impact on transport behavior. This structural and magnetic reconfiguration enhances spin entropy, contributing to an increased Seebeck coefficient (317 \(\mu\) μ V/K) and electrical conductivity (6779 S/m) at 700 \(^\circ\) C. The interplay of these effects results in a record-high power factor (0.722 mW/mK \(^2\) 2 ) among Cu-based delafossites. In addition, thermal conductivity measurements confirm a reduced \(\kappa\) κ of 2.84 W/mK, attributed to increased phonon scattering at Mg-induced interfaces. This study provides direct experimental evidence of interlamellar porosity and spin-driven transport mechanisms, offering new insights into structural tuning for high-performance thermoelectrics.