<p>Although double halide perovskites have garnered significant attention as environmentally benign and structurally versatile alternatives to lead-based counterparts, the optoelectronic behavior of the <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\hbox {Rb}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>Rb</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\hbox {YAuX}_6\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>YAuX</mtext> <mn>6</mn> </msub> </math></EquationSource> </InlineEquation> (<i>X</i> = F, Cl, Br, I) remain underexplored. Given the favorable bandgaps 1.47&#xa0;eV, 2.04&#xa0;eV, 1.63&#xa0;eV, and 1.13 eV (GGA) and 1.19&#xa0;eV, 1.85&#xa0;eV, 1.48&#xa0;eV, and 0.94 eV (GGA+SOC) and stability often associated with gold-based perovskites, and the significant impact of spin-orbit coupling (SOC) owing to the presence of heavy elements including gold, theoretical calculations were performed using density functional theory on the double halide perovskite compound <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\hbox {Rb}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>Rb</mtext> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\hbox {YAuX}_6\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mtext>YAuX</mtext> <mn>6</mn> </msub> </math></EquationSource> </InlineEquation> (<i>X</i> = F, Cl, Br, I). We have found that the computed bandgaps and the most active optical absorption are within the Vis–UV range with an absorption coefficient <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> &gt; <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\hbox {10}^5\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>10</mtext> <mn>5</mn> </msup> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\hbox {cm}^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>cm</mtext> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, suggesting that these materials are highly promising for the development of efficient and stable light-harvesting materials for next-generation solar energy technologies.</p>

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A DFT Study on the Structural, Electronic, Optical, and Mechanical Properties of Lead-Free Perovskites \(\hbox {Rb}_2\) \(\hbox {YAuX}_6\) (X = F, Cl, Br, I) for Solar Cell Applications

  • Angela Chinggelkim,
  • R. Zosiamliana,
  • Laltha Kimi,
  • Lalhum Hima,
  • Bernard Lalroliana,
  • Lalrinthara Pachuau,
  • Shivraj Gurung,
  • Lalhriat Zuala

摘要

Although double halide perovskites have garnered significant attention as environmentally benign and structurally versatile alternatives to lead-based counterparts, the optoelectronic behavior of the \(\hbox {Rb}_2\) Rb 2 \(\hbox {YAuX}_6\) YAuX 6 (X = F, Cl, Br, I) remain underexplored. Given the favorable bandgaps 1.47 eV, 2.04 eV, 1.63 eV, and 1.13 eV (GGA) and 1.19 eV, 1.85 eV, 1.48 eV, and 0.94 eV (GGA+SOC) and stability often associated with gold-based perovskites, and the significant impact of spin-orbit coupling (SOC) owing to the presence of heavy elements including gold, theoretical calculations were performed using density functional theory on the double halide perovskite compound \(\hbox {Rb}_2\) Rb 2 \(\hbox {YAuX}_6\) YAuX 6 (X = F, Cl, Br, I). We have found that the computed bandgaps and the most active optical absorption are within the Vis–UV range with an absorption coefficient \(\alpha \) α > \(\hbox {10}^5\) 10 5 \(\hbox {cm}^{-1}\) cm - 1 , suggesting that these materials are highly promising for the development of efficient and stable light-harvesting materials for next-generation solar energy technologies.