<p>This study explores the effects of partially substituting <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(Ca^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <msup> <mi>a</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(Sr^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <msup> <mi>r</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> on the structural, magnetic, and magnet-transport properties of the mixed valence perovskite manganites La<sub>0.7</sub>Ca<sub>0.18–<i> x</i></sub>Sr<sub><i>x</i></sub>Ba<sub>0.12</sub>Mn<sub>0.95</sub>Sn<sub>0.05</sub>O<sub>3</sub> (0≤<i>x</i>≤0.04), synthesized using the solid-state reaction (SSR) method. The substitution of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(Ca^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <msup> <mi>a</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> by the larger <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(Sr^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <msup> <mi>r</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> cation is expected to generate internal chemical pressure within the perovskite lattice, leading to modifications in the <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(Mn - O - Mn\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mi>n</mi> <mo>-</mo> <mi>O</mi> <mo>-</mo> <mi>M</mi> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation> bond geometry and consequently affecting the double-exchange interactions responsible for the magnetoresistance effect. X-ray diffraction analysis indicates that all samples adopt an orthorhombic crystalline structure with Pbnm space group. The substitution of <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(Ca^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <msup> <mi>a</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> with larger <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(Sr^{2 + }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>S</mi> <msup> <mi>r</mi> <mrow> <mn>2</mn> <mo>+</mo> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> cation increases the average A-site ionic radius <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(r_{{\text{A}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>r</mi> <mtext>A</mtext> </msub> </math></EquationSource> </InlineEquation>, resulting in an increase of the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(Mn - O - Mn\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mi>n</mi> <mo>-</mo> <mi>O</mi> <mo>-</mo> <mi>M</mi> <mi>n</mi> </mrow> </math></EquationSource> </InlineEquation> bond angle and a decrease in the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(Mn - O\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>M</mi> <mi>n</mi> <mo>-</mo> <mi>O</mi> </mrow> </math></EquationSource> </InlineEquation> bond distance. These structural adjustments enhance the electron bandwidth <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(W\)</EquationSource> <EquationSource Format="MATHML"><math> <mi>W</mi> </math></EquationSource> </InlineEquation> and strengthen the ferromagnetic double-exchange <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\left( {DE} \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <mrow> <mi mathvariant="italic">DE</mi> </mrow> </mfenced> </math></EquationSource> </InlineEquation> interaction. Consequently, the Curie temperature (<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(T_{{\text{C}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mtext>C</mtext> </msub> </math></EquationSource> </InlineEquation>) increases from 148.7 to 233.3 K, and the metal-insulator transition (<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(T_{{{\text{MI}}}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>T</mi> <mtext>MI</mtext> </msub> </math></EquationSource> </InlineEquation>) shifts toward higher temperatures. Temperature-dependent ac susceptibility at various frequencies indicates the presence of magnetic relaxation associated with domain wall motion and dynamic magnetic responses within the ferromagnetic ordered state. The hysteresis loops exhibit ferromagnetic behavior at 1.8 K and paramagnetic state at 300 K. Furthermore, a systematic decrease in magnetoresistance <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\left( {MR} \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <mrow> <mi mathvariant="italic">MR</mi> </mrow> </mfenced> </math></EquationSource> </InlineEquation> from 38 to 20.3% is observed with increasing <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(Sr\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Sr</mi> </mrow> </math></EquationSource> </InlineEquation> content. These findings demonstrate that minor <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(Sr\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Sr</mi> </mrow> </math></EquationSource> </InlineEquation>-doping at the <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(Ca\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="italic">Ca</mi> </mrow> </math></EquationSource> </InlineEquation>-site is an effective tool for tuning the competition between lattice distortion and magnetic interactions, directly influencing the electronic and magneto-transport performance of these manganites.</p>

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Effect of Sr doping on the magnetic, electrical and magneto-transport properties of La0.7Ca0.18−xSrxBa0.12Mn0.95Sn0.05O3 (0 ≤ x ≤ 0.04) perovskite manganites

  • Ibtihal Belal,
  • Faiza Meriche,
  • Nabil Mahamdioua,
  • Jose Alonso Alonso,
  • Jose Luis Martinez,
  • Cabir Terzioglu,
  • Allaoua Boukerika

摘要

This study explores the effects of partially substituting \(Ca^{2 + }\) C a 2 + with \(Sr^{2 + }\) S r 2 + on the structural, magnetic, and magnet-transport properties of the mixed valence perovskite manganites La0.7Ca0.18– xSrxBa0.12Mn0.95Sn0.05O3 (0≤x≤0.04), synthesized using the solid-state reaction (SSR) method. The substitution of \(Ca^{2 + }\) C a 2 + by the larger \(Sr^{2 + }\) S r 2 + cation is expected to generate internal chemical pressure within the perovskite lattice, leading to modifications in the \(Mn - O - Mn\) M n - O - M n bond geometry and consequently affecting the double-exchange interactions responsible for the magnetoresistance effect. X-ray diffraction analysis indicates that all samples adopt an orthorhombic crystalline structure with Pbnm space group. The substitution of \(Ca^{2 + }\) C a 2 + with larger \(Sr^{2 + }\) S r 2 + cation increases the average A-site ionic radius \(r_{{\text{A}}}\) r A , resulting in an increase of the \(Mn - O - Mn\) M n - O - M n bond angle and a decrease in the \(Mn - O\) M n - O bond distance. These structural adjustments enhance the electron bandwidth \(W\) W and strengthen the ferromagnetic double-exchange \(\left( {DE} \right)\) DE interaction. Consequently, the Curie temperature ( \(T_{{\text{C}}}\) T C ) increases from 148.7 to 233.3 K, and the metal-insulator transition ( \(T_{{{\text{MI}}}}\) T MI ) shifts toward higher temperatures. Temperature-dependent ac susceptibility at various frequencies indicates the presence of magnetic relaxation associated with domain wall motion and dynamic magnetic responses within the ferromagnetic ordered state. The hysteresis loops exhibit ferromagnetic behavior at 1.8 K and paramagnetic state at 300 K. Furthermore, a systematic decrease in magnetoresistance \(\left( {MR} \right)\) MR from 38 to 20.3% is observed with increasing \(Sr\) Sr content. These findings demonstrate that minor \(Sr\) Sr -doping at the \(Ca\) Ca -site is an effective tool for tuning the competition between lattice distortion and magnetic interactions, directly influencing the electronic and magneto-transport performance of these manganites.