<p>In the present work, the effect of Zn substitutionon the structural, electrical, and magnetic properties of Zn-substituted double-layered manganite with La<sub>2.01</sub>Sr<sub>0.99</sub>Mn<sub>2-x</sub>Zn<sub>x</sub>O<sub>7</sub> <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\((x=0 and 0.2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>=</mo> <mn>0</mn> <mi>a</mi> <mi>n</mi> <mi>d</mi> <mn>0.2</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> formula has been investigated. Both compounds were synthesized using the solid-state reaction method. The X-ray diffraction analysis, based on the diffractograms refinement, reveals that both samples crystallize in a tetragonal structure with an I4/mmm space group with a notable increase in the cell parameters and a decrease in crystallite size upon substitution. A decrease in the grain sizes is observed through the analysis of scanning electron microscope images. The electrical resistivity investigation, using the four-probe technique, indicates that both compounds exhibit metal–insulator transition T<sub>MI</sub>, which shifted to lower temperatures with 10% Zn substitution, accompanied by a considerable increase in resistivity. The resistivity fitting curves revealed that the electrical conduction is governed by a combination of the residual, weak localization, and electron–electron interactions at<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(T&lt; {T}_{MI}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>&lt;</mo> <msub> <mi>T</mi> <mrow> <mi mathvariant="italic">MI</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, whereas at<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(T&gt;{T}_{MI}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>&gt;</mo> <msub> <mi>T</mi> <mrow> <mi mathvariant="italic">MI</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, it is governed by two models: adiabatic small polaron hopping (ASPH) above <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({\theta }_{D}/2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>θ</mi> <mi>D</mi> </msub> <mo stretchy="false">/</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and 3D-Mott’s variable range hopping (VRH) below it. A slight improvement in the obtained magnetoresistance was observed in the substituted sample at<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(T&lt;59 K\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>T</mi> <mo>&lt;</mo> <mn>59</mn> <mi>K</mi> </mrow> </math></EquationSource> </InlineEquation>. Density of state, mean hopping distance <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({R}_{h},\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>R</mi> <mi>h</mi> </msub> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and mean hopping energy <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({E}_{h}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>E</mi> <mi>h</mi> </msub> </math></EquationSource> </InlineEquation> were determined and discussed. The magnetic investigation revealed a decrease in the Curie temperature with substitution from 335 to 212&#xa0;K, and the appearance of the Griffiths phase. Magnetization measurements as a function of magnetic field revealed the presence of the ferromagnetic state at 5&#xa0;K for both samples. At room temperature, the parent sample remains in ferromagnetic state, while the substituted one changes to a paramagnetic state. The present findings demonstrate that Zn doping modifies double exchange and the metal–insulator transition, enhancing magnetoresistance and providing insights for low-temperature magnetic sensor applications and layered manganite physics.</p>

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Influence of B-site substitution on the correlated structural–electrical–magnetic properties in the double-layered manganite La2.01Sr0.99Mn2-xZnxO7 (x = 0 and 0.2)

  • Akrem Bellouti,
  • Nabil Mahamdioua,
  • Sevgi Polat Altintas,
  • Nevin Soylu Koc,
  • Fatih Denbri,
  • Faiza Meriche,
  • Jose A. Alonso,
  • Jose L. Martinez

摘要

In the present work, the effect of Zn substitutionon the structural, electrical, and magnetic properties of Zn-substituted double-layered manganite with La2.01Sr0.99Mn2-xZnxO7 \((x=0 and 0.2)\) ( x = 0 a n d 0.2 ) formula has been investigated. Both compounds were synthesized using the solid-state reaction method. The X-ray diffraction analysis, based on the diffractograms refinement, reveals that both samples crystallize in a tetragonal structure with an I4/mmm space group with a notable increase in the cell parameters and a decrease in crystallite size upon substitution. A decrease in the grain sizes is observed through the analysis of scanning electron microscope images. The electrical resistivity investigation, using the four-probe technique, indicates that both compounds exhibit metal–insulator transition TMI, which shifted to lower temperatures with 10% Zn substitution, accompanied by a considerable increase in resistivity. The resistivity fitting curves revealed that the electrical conduction is governed by a combination of the residual, weak localization, and electron–electron interactions at \(T< {T}_{MI}\) T < T MI , whereas at \(T>{T}_{MI}\) T > T MI , it is governed by two models: adiabatic small polaron hopping (ASPH) above \({\theta }_{D}/2\) θ D / 2 and 3D-Mott’s variable range hopping (VRH) below it. A slight improvement in the obtained magnetoresistance was observed in the substituted sample at \(T<59 K\) T < 59 K . Density of state, mean hopping distance \({R}_{h},\) R h , and mean hopping energy \({E}_{h}\) E h were determined and discussed. The magnetic investigation revealed a decrease in the Curie temperature with substitution from 335 to 212 K, and the appearance of the Griffiths phase. Magnetization measurements as a function of magnetic field revealed the presence of the ferromagnetic state at 5 K for both samples. At room temperature, the parent sample remains in ferromagnetic state, while the substituted one changes to a paramagnetic state. The present findings demonstrate that Zn doping modifies double exchange and the metal–insulator transition, enhancing magnetoresistance and providing insights for low-temperature magnetic sensor applications and layered manganite physics.