<p>Hole-doped manganites <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="203" /> </InlineMediaObject> <EquationSource Format="TEX">\({\text{La}}_{\left(0.6-x\right)}{\text{Ca}}_{x}{\text{Sm}}_{0.1}{\text{Ba}}_{0.3}{\text{MnO}}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>La</mtext> <mfenced close=")" open="("> <mn>0.6</mn> <mo>-</mo> <mi>x</mi> </mfenced> </msub> <msub> <mtext>Ca</mtext> <mi>x</mi> </msub> <msub> <mtext>Sm</mtext> <mrow> <mn>0.1</mn> </mrow> </msub> <msub> <mtext>Ba</mtext> <mrow> <mn>0.3</mn> </mrow> </msub> <msub> <mtext>MnO</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (with <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq3.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(x=0.0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>=</mo> <mn>0.0</mn> </mrow> </math></EquationSource> </InlineEquation> and 0.1) were synthesized using a solid-state reaction method. The structural, microstructural, electrical transport, magnetotransport, and temperature coefficient of resistance (TCR) properties were thoroughly investigated. X-ray diffraction (XRD) analysis revealed that both compounds crystallized in an orthorhombic structure with the Imma space group, with no secondary phases detected. The Ca-doped sample exhibited significantly smaller and more homogeneous grains compared to the undoped sample. Resistivity measurements showed a metal–insulator transition around <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(221 K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>221</mn> <mi>K</mi> </mrow> </math></EquationSource> </InlineEquation>, with the transition temperature shifting to lower values upon Ca-doping. Magnetoresistance (MR) values at low temperatures were substantial, reaching 23.37% for the undoped sample and <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(23.7\%\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>23.7</mn> <mo>%</mo> </mrow> </math></EquationSource> </InlineEquation> for the Ca-doped sample at <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(290 K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>290</mn> <mi>K</mi> </mrow> </math></EquationSource> </InlineEquation>. The temperature dependence of resistivity exhibited both intrinsic and extrinsic contributions to magnetoresistance (MR), with a peak MR of 23.7% for the Ca-doped sample and <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="51" /> </InlineMediaObject> <EquationSource Format="TEX">\(23.37\%\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>23.37</mn> <mo>%</mo> </mrow> </math></EquationSource> </InlineEquation> for the undoped one at low temperatures. The TCR curve showed a peak of <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="10854_2025_14707_Article_IEq8.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(1.78 \%{K}^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1.78</mn> <mo>%</mo> <msup> <mrow> <mi>K</mi> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> at room temperature, indicating significant temperature-dependent resistance changes. Low-temperature resistivity was described with a combination of residual resistivity, weak localization, and electron–electron interactions, whereas the high-temperature behavior is well described by adiabatic small polaron hopping. These results bring out the complexity in the interrelation between structural changes and magnetotransport properties and emphasize the role of Ca-doping in tuning electrical and magnetoresistive properties in manganite perovskite.</p>

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Magnetoresistive and electrical response characteristics of hole-doped polycrystalline simple perovskite manganites La0.6−xCaxSm0.1Ba0.3MnO3 (x = 0.0 and 0.1)

  • Sadek Boufligha,
  • Nabil Mahamdioua,
  • Sevgi Polat Altintas,
  • Nevin Soylu Koc

摘要

Hole-doped manganites \({\text{La}}_{\left(0.6-x\right)}{\text{Ca}}_{x}{\text{Sm}}_{0.1}{\text{Ba}}_{0.3}{\text{MnO}}_{3}\) La 0.6 - x Ca x Sm 0.1 Ba 0.3 MnO 3 (with \(x=0.0\) x = 0.0 and 0.1) were synthesized using a solid-state reaction method. The structural, microstructural, electrical transport, magnetotransport, and temperature coefficient of resistance (TCR) properties were thoroughly investigated. X-ray diffraction (XRD) analysis revealed that both compounds crystallized in an orthorhombic structure with the Imma space group, with no secondary phases detected. The Ca-doped sample exhibited significantly smaller and more homogeneous grains compared to the undoped sample. Resistivity measurements showed a metal–insulator transition around \(221 K\) 221 K , with the transition temperature shifting to lower values upon Ca-doping. Magnetoresistance (MR) values at low temperatures were substantial, reaching 23.37% for the undoped sample and \(23.7\%\) 23.7 % for the Ca-doped sample at \(290 K\) 290 K . The temperature dependence of resistivity exhibited both intrinsic and extrinsic contributions to magnetoresistance (MR), with a peak MR of 23.7% for the Ca-doped sample and \(23.37\%\) 23.37 % for the undoped one at low temperatures. The TCR curve showed a peak of \(1.78 \%{K}^{-1}\) 1.78 % K - 1 at room temperature, indicating significant temperature-dependent resistance changes. Low-temperature resistivity was described with a combination of residual resistivity, weak localization, and electron–electron interactions, whereas the high-temperature behavior is well described by adiabatic small polaron hopping. These results bring out the complexity in the interrelation between structural changes and magnetotransport properties and emphasize the role of Ca-doping in tuning electrical and magnetoresistive properties in manganite perovskite.