<p>Magnetoelectric <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq2.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="211" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}-Co{Fe}_{2}{O}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>b</mi> <msub> <mrow> <mi mathvariant="italic">Zr</mi> </mrow> <mrow> <mn>0.52</mn> </mrow> </msub> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>0.48</mn> </mrow> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo>-</mo> <mi>C</mi> <mi>o</mi> <msub> <mrow> <mi mathvariant="italic">Fe</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> composites with different molar fractions (<InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq3.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="330" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}/Co{Fe}_{2}{O}_{4}=3:1, 2:1, 1:1,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>b</mi> <msub> <mrow> <mi mathvariant="italic">Zr</mi> </mrow> <mrow> <mn>0.52</mn> </mrow> </msub> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>0.48</mn> </mrow> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> <mo stretchy="false">/</mo> <mi>C</mi> <mi>o</mi> <msub> <mrow> <mi mathvariant="italic">Fe</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>4</mn> </msub> <mo>=</mo> <mn>3</mn> <mo>:</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>:</mo> <mn>1</mn> <mo>,</mo> <mn>1</mn> <mo>:</mo> <mn>1</mn> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(1:2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>:</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>) were synthesized using citrate-sol–gel route. X-ray diffraction confirmed the presence of perovskite (<InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>b</mi> <msub> <mrow> <mi mathvariant="italic">Zr</mi> </mrow> <mrow> <mn>0.52</mn> </mrow> </msub> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>0.48</mn> </mrow> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>) and spinel (<InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(Co{Fe}_{2}{O}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>o</mi> <msub> <mrow> <mi mathvariant="italic">Fe</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>) structures in the produced composites. Scanning electron microscopy showed a homogeneous mixing of <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>b</mi> <msub> <mrow> <mi mathvariant="italic">Zr</mi> </mrow> <mrow> <mn>0.52</mn> </mrow> </msub> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>0.48</mn> </mrow> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(Co{Fe}_{2}{O}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>o</mi> <msub> <mrow> <mi mathvariant="italic">Fe</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> grains with dense microstructures. The composites' magnetic and ferroelectric hysteresis loops exhibited multiferroic behaviour. Impedance spectroscopy indicated that the composite's overall resistance&#xa0;(<InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\({R}_{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation>) increases up to a <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(1:1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>:</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> molar ratio due to better phase connectivity, which improves magnetoelectric (ME) coupling. When the molar ratio was <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(1:2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>:</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation>, the <InlineEquation ID="IEq12"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq9.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="23" /> </InlineMediaObject> <EquationSource Format="TEX">\({R}_{T}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>R</mi> <mi>T</mi> </msub> </math></EquationSource> </InlineEquation> value dropped, which increased the interface charge carrier leakage and reduced the ME coupling. The composite with an equimolar ratio (<InlineEquation ID="IEq13"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq10.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="31" /> </InlineMediaObject> <EquationSource Format="TEX">\(1:1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>:</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>) achieved the highest ME coefficient (<InlineEquation ID="IEq14"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq14.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\({\alpha }_{ME}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>α</mi> <mrow> <mi mathvariant="italic">ME</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>) value of 10.53&#xa0;mV/cm.Oe. This value is 14 times higher than the equimolar composite produced by mixing the&#xa0;<InlineEquation ID="IEq15"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="122" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>b</mi> <msub> <mrow> <mi mathvariant="italic">Zr</mi> </mrow> <mrow> <mn>0.52</mn> </mrow> </msub> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>0.48</mn> </mrow> </msub> <msub> <mi>O</mi> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq16"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="339_2025_8509_Article_IEq6.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="69" /> </InlineMediaObject> <EquationSource Format="TEX">\(Co{Fe}_{2}{O}_{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>C</mi> <mi>o</mi> <msub> <mrow> <mi mathvariant="italic">Fe</mi> </mrow> <mn>2</mn> </msub> <msub> <mi>O</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> powders due to its dense microstructure, improved connectivity, highest resistance, and reduced leakage current density, making it optimal for ME device applications.</p>

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Enhanced magnetoelectric characteristics of PbZr0.52Ti0.48O3CoFe2O4 composites: impact of molar ratio and phase connectivity

  • S. Ahmed,
  • M. Atif,
  • F. Zafar,
  • W. Khalid,
  • Z. Ali,
  • M. Nadeem

摘要

Magnetoelectric \(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}-Co{Fe}_{2}{O}_{4}\) P b Zr 0.52 Ti 0.48 O 3 - C o Fe 2 O 4 composites with different molar fractions ( \(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}/Co{Fe}_{2}{O}_{4}=3:1, 2:1, 1:1,\) P b Zr 0.52 Ti 0.48 O 3 / C o Fe 2 O 4 = 3 : 1 , 2 : 1 , 1 : 1 , and \(1:2\) 1 : 2 ) were synthesized using citrate-sol–gel route. X-ray diffraction confirmed the presence of perovskite ( \(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\) P b Zr 0.52 Ti 0.48 O 3 ) and spinel ( \(Co{Fe}_{2}{O}_{4}\) C o Fe 2 O 4 ) structures in the produced composites. Scanning electron microscopy showed a homogeneous mixing of \(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\) P b Zr 0.52 Ti 0.48 O 3 and \(Co{Fe}_{2}{O}_{4}\) C o Fe 2 O 4 grains with dense microstructures. The composites' magnetic and ferroelectric hysteresis loops exhibited multiferroic behaviour. Impedance spectroscopy indicated that the composite's overall resistance ( \({R}_{T}\) R T ) increases up to a \(1:1\) 1 : 1 molar ratio due to better phase connectivity, which improves magnetoelectric (ME) coupling. When the molar ratio was \(1:2\) 1 : 2 , the \({R}_{T}\) R T value dropped, which increased the interface charge carrier leakage and reduced the ME coupling. The composite with an equimolar ratio ( \(1:1\) 1 : 1 ) achieved the highest ME coefficient ( \({\alpha }_{ME}\) α ME ) value of 10.53 mV/cm.Oe. This value is 14 times higher than the equimolar composite produced by mixing the  \(Pb{Zr}_{0.52}{Ti}_{0.48}{O}_{3}\) P b Zr 0.52 Ti 0.48 O 3 and \(Co{Fe}_{2}{O}_{4}\) C o Fe 2 O 4 powders due to its dense microstructure, improved connectivity, highest resistance, and reduced leakage current density, making it optimal for ME device applications.