<p>Crystal phases <i>Pbcm</i> (monoclinic), <i>Cmcm</i> (orthorhombic), <i>P4/mbm</i> (tetragonal) and <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43207_2025_519_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pm\overline{3 }m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>m</mi> <mover> <mn>3</mn> <mo>¯</mo> </mover> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation>(cubic) of the perovskite AgNbO<sub>3</sub>; <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43207_2025_519_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pm\overline{3 }m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>m</mi> <mover> <mn>3</mn> <mo>¯</mo> </mover> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation> (cubic) of AgNb<sub>0.5</sub>Ta<sub>0.5</sub>O<sub>3</sub>; and <i>R3c</i> (rhombohedral), <i>P2/m</i> (monoclinic), <i>Cmcm</i> (orthorhombic), <i>P4/mbm</i> (tetragonal) and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43207_2025_519_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pm\overline{3 }m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>m</mi> <mover> <mn>3</mn> <mo>¯</mo> </mover> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation> (cubic) of AgTaO<sub>3</sub> have been studied using DFT. To investigate stable crystal phases, cohesive energies and formation enthalpy are calculated demonstrating that <i>P4/mbm</i>, <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="43207_2025_519_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(Pm\overline{3 }m\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>m</mi> <mover> <mn>3</mn> <mo>¯</mo> </mover> <mi>m</mi> </mrow> </math></EquationSource> </InlineEquation> and <i>P2/m</i> are the stable phases of AgNbO<sub>3</sub>, AgNb<sub>0.5</sub>Ta<sub>0.5</sub>O<sub>3</sub> and AgTaO<sub>3</sub> respectively. The electronic properties are examined through the mBJ exchange potential in their stable structural phases reveal that allAgNb<sub>1-x</sub>Ta<sub>x</sub>O<sub>3</sub> (<i>x</i> = 0, 0.5 and 1) perovskites are direct band gap semiconductors with energy gaps of 1.686, 1.973 and 2.1&#xa0;eV respectively. Previous studies reported an indirect band gap of 2.97&#xa0;eV for AgTaO<sub>3</sub>. These systems are semiconductors with ideal band gaps, leading to a wide array of applications including dielectric and photocatalytic devices. The optoelectronic properties of these compounds suggest that they are promising candidates for optical devices such as LEDs, photodiodes, quantum wells and solar cells in the visible region of the electromagnetic spectrum. </p>

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Structural phase transition and optoelectronic properties of lead-free AgNb1-xTaxO3 (x = 0, 0.5 and 1) perovskite systems

  • Mian Abdul Wahab,
  • Hidayat Ullah Khan,
  • Iftikhar Ahmad,
  • Amir Ullah,
  • Zahid Ali

摘要

Crystal phases Pbcm (monoclinic), Cmcm (orthorhombic), P4/mbm (tetragonal) and \(Pm\overline{3 }m\) P m 3 ¯ m (cubic) of the perovskite AgNbO3; \(Pm\overline{3 }m\) P m 3 ¯ m (cubic) of AgNb0.5Ta0.5O3; and R3c (rhombohedral), P2/m (monoclinic), Cmcm (orthorhombic), P4/mbm (tetragonal) and \(Pm\overline{3 }m\) P m 3 ¯ m (cubic) of AgTaO3 have been studied using DFT. To investigate stable crystal phases, cohesive energies and formation enthalpy are calculated demonstrating that P4/mbm, \(Pm\overline{3 }m\) P m 3 ¯ m and P2/m are the stable phases of AgNbO3, AgNb0.5Ta0.5O3 and AgTaO3 respectively. The electronic properties are examined through the mBJ exchange potential in their stable structural phases reveal that allAgNb1-xTaxO3 (x = 0, 0.5 and 1) perovskites are direct band gap semiconductors with energy gaps of 1.686, 1.973 and 2.1 eV respectively. Previous studies reported an indirect band gap of 2.97 eV for AgTaO3. These systems are semiconductors with ideal band gaps, leading to a wide array of applications including dielectric and photocatalytic devices. The optoelectronic properties of these compounds suggest that they are promising candidates for optical devices such as LEDs, photodiodes, quantum wells and solar cells in the visible region of the electromagnetic spectrum.