<p>This study investigates the potential of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeX}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeX</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> (<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\text {X}=\text {S}, \text {Se}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mtext>X</mtext> <mo>=</mo> <mtext>S</mtext> <mo>,</mo> <mtext>Se</mtext> </mrow> </math></EquationSource> </InlineEquation>) chalcogenides as attractive photo-ferroelectric materials for visible-light energy conversion. Using first-principles density functional theory (DFT) calculations, we reveal that these compounds exhibit a robust ferroelectricity-driven bulk photovoltaic effect (BPVE), eliminating the need for external electric fields—an inherent limitation in conventional ferroelectric oxides. The <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeX}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeX</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> materials possess bandgaps ranging from 0.97 to <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(1.90\text { eV}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1.90</mn> <mspace width="0.333333em" /> <mtext>eV</mtext> </mrow> </math></EquationSource> </InlineEquation>, aligning well with the visible spectrum and supporting effective light harvesting. <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeS}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeS</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> displays higher spontaneous polarization than <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeSe}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeSe</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>, facilitating efficient charge separation, while their non-centrosymmetric crystal symmetry enables strong shift current generation via the Berry connection mechanism. Notably, orthorhombic <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeSe}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeSe</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> exhibits a peak shift current conductivity of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(131~\mu \text {A/V}^{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>131</mn> <mspace width="3.33333pt" /> <mi>μ</mi> <msup> <mtext>A/V</mtext> <mn>2</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> within the visible range, comparable to the best known BPVE materials. These results highlight the remarkable interplay between the electronic, optical, and ferroelectric properties in <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\text {Ag}_2\text {GeX}_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Ag</mtext> <mn>2</mn> </msub> <msub> <mtext>GeX</mtext> <mn>3</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> compounds, positioning them as viable candidates for next-generation solar energy applications. Their ability to surpass traditional efficiency limits via the intrinsic BPVE mechanism offers a compelling pathway toward high-performance, sustainable photovoltaic technologies.</p>

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First-principles exploration of Ag2GeX3(X=S,Se) chalcogenides as photo-ferroelectric materials for visible-light energy conversion

  • Naouel Chelil,
  • Mohammed Sahnoun

摘要

This study investigates the potential of \(\text {Ag}_2\text {GeX}_3\) Ag 2 GeX 3 ( \(\text {X}=\text {S}, \text {Se}\) X = S , Se ) chalcogenides as attractive photo-ferroelectric materials for visible-light energy conversion. Using first-principles density functional theory (DFT) calculations, we reveal that these compounds exhibit a robust ferroelectricity-driven bulk photovoltaic effect (BPVE), eliminating the need for external electric fields—an inherent limitation in conventional ferroelectric oxides. The \(\text {Ag}_2\text {GeX}_3\) Ag 2 GeX 3 materials possess bandgaps ranging from 0.97 to \(1.90\text { eV}\) 1.90 eV , aligning well with the visible spectrum and supporting effective light harvesting. \(\text {Ag}_2\text {GeS}_3\) Ag 2 GeS 3 displays higher spontaneous polarization than \(\text {Ag}_2\text {GeSe}_3\) Ag 2 GeSe 3 , facilitating efficient charge separation, while their non-centrosymmetric crystal symmetry enables strong shift current generation via the Berry connection mechanism. Notably, orthorhombic \(\text {Ag}_2\text {GeSe}_3\) Ag 2 GeSe 3 exhibits a peak shift current conductivity of \(131~\mu \text {A/V}^{2}\) 131 μ A/V 2 within the visible range, comparable to the best known BPVE materials. These results highlight the remarkable interplay between the electronic, optical, and ferroelectric properties in \(\text {Ag}_2\text {GeX}_3\) Ag 2 GeX 3 compounds, positioning them as viable candidates for next-generation solar energy applications. Their ability to surpass traditional efficiency limits via the intrinsic BPVE mechanism offers a compelling pathway toward high-performance, sustainable photovoltaic technologies.