<p>Oxygen vacancies (OVs) provide a powerful route for tuning the performance of oxide photocatalysts; however, a quantitative understanding of how vacancy concentration governs the structure–property landscape of <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Bi</mtext> <mn>2</mn> </msub> <msub> <mtext>WO</mtext> <mn>6</mn> </msub> </mrow> </math></EquationSource> </InlineEquation>. remains incomplete. In this work, first-principles density functional theory calculations were used to systematically investigate pristine and oxygen-vacancy-containing orthorhombic <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Bi</mtext> <mn>2</mn> </msub> <msub> <mtext>WO</mtext> <mn>6</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\left( {{\text{Pca2}}_{1} } \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mfenced close=")" open="("> <msub> <mtext>Pca2</mtext> <mn>1</mn> </msub> </mfenced> </math></EquationSource> </InlineEquation>. Vacancy configurations were generated by removing oxygen atoms from inequivalent lattice sites. Formation-energy analysis identified O2 and O3 as the most favorable vacancy sites, and a series of models with OV concentrations of approximately 4.2–25%, corresponding to 1–6 oxygen vacancies in the 36-atom <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({\text{Bi}}_{{8}} {\text{W}}_{4} {\text{O}}_{24}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Bi</mtext> <mn>8</mn> </msub> <msub> <mtext>W</mtext> <mn>4</mn> </msub> <msub> <mtext>O</mtext> <mn>24</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> periodic cell, was constructed. Progressive vacancy introduction induced pronounced local coordination changes around Bi and non-monotonic lattice responses. In the selected 4-OV arrangement, the strong expansion of the <i>b</i> parameter and unit-cell volume was attributed to a configuration-dependent finite-cell effect arising from the ordered vacancy geometry, rather than to an intrinsic concentration threshold. Electronically, OVs introduced donor states near the conduction-band minimum, shifted the Fermi level into the conduction band, induced <i>n</i>-type character, and reduced the band gap from 2.326&#xa0;eV in pristine <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>Bi</mtext> <mn>2</mn> </msub> <msub> <mtext>WO</mtext> <mn>6</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> to 0.9&#xa0;eV for the three-vacancy model, with further narrowing at higher vacancy concentrations. Density-of-states and electron-density-difference analyses revealed Bi-6<i>p</i>-dominated defect states, vacancy-centered F-center-like electron localization, and progressive charge accumulation on Bi atoms. Optically, vacancy engineering produced a red-shifted absorption edge, emergent absorption features in the 1–4&#xa0;eV range, enhanced low-energy dielectric responses, and an increased static dielectric constant.</p>

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Effect of Oxygen-Vacancy Concentration on the Structural, Electronic, and Optical Properties of Bi2WO6 Photocatalyst: A DFT Study

  • Doan Thi Hien,
  • Pham Van Hai,
  • Luc Huy Hoang,
  • Tran Phan Thuy Linh

摘要

Oxygen vacancies (OVs) provide a powerful route for tuning the performance of oxide photocatalysts; however, a quantitative understanding of how vacancy concentration governs the structure–property landscape of \({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\) Bi 2 WO 6 . remains incomplete. In this work, first-principles density functional theory calculations were used to systematically investigate pristine and oxygen-vacancy-containing orthorhombic \({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\) Bi 2 WO 6 \(\left( {{\text{Pca2}}_{1} } \right)\) Pca2 1 . Vacancy configurations were generated by removing oxygen atoms from inequivalent lattice sites. Formation-energy analysis identified O2 and O3 as the most favorable vacancy sites, and a series of models with OV concentrations of approximately 4.2–25%, corresponding to 1–6 oxygen vacancies in the 36-atom \({\text{Bi}}_{{8}} {\text{W}}_{4} {\text{O}}_{24}\) Bi 8 W 4 O 24 periodic cell, was constructed. Progressive vacancy introduction induced pronounced local coordination changes around Bi and non-monotonic lattice responses. In the selected 4-OV arrangement, the strong expansion of the b parameter and unit-cell volume was attributed to a configuration-dependent finite-cell effect arising from the ordered vacancy geometry, rather than to an intrinsic concentration threshold. Electronically, OVs introduced donor states near the conduction-band minimum, shifted the Fermi level into the conduction band, induced n-type character, and reduced the band gap from 2.326 eV in pristine \({\text{Bi}}_{{2}} {\text{WO}}_{{6}}\) Bi 2 WO 6 to 0.9 eV for the three-vacancy model, with further narrowing at higher vacancy concentrations. Density-of-states and electron-density-difference analyses revealed Bi-6p-dominated defect states, vacancy-centered F-center-like electron localization, and progressive charge accumulation on Bi atoms. Optically, vacancy engineering produced a red-shifted absorption edge, emergent absorption features in the 1–4 eV range, enhanced low-energy dielectric responses, and an increased static dielectric constant.