<p>The structural, optoelectronic, and magnetic properties of LiXO<sub>2</sub> (<i>X</i> = Co, Ni) delafossite compounds are evaluated using first-principles based <i>DFT</i> calculations to investigate their potential applications in optoelectronic and spintronic devices. Based on calculated ground state energies, LiNiO<sub>2</sub> is a more stable compound, compared to LiCoO<sub>2</sub>. The indirect energy band gap for LiCoO<sub>2</sub> and LiNiO<sub>2</sub> are 4.95 and 5.02&#xa0;eV, respectively, in spin (↑) direction. However, in spin (↓) direction, the values of energy band gaps are 2.05 and 1.82&#xa0;eV for LiCoO<sub>2</sub> and LiNiO<sub>2</sub>, respectively. The total magnetic moment <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\({m}_{tot}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>m</mi> <mrow> <mi mathvariant="italic">tot</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> values for LiCoO<sub>2</sub> are higher, compared to LiNiO<sub>2</sub>. Unfilled d-orbitals (Co <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq2.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(-{3d}^{7}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <msup> <mrow> <mn>3</mn> <mi>d</mi> </mrow> <mn>7</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> and Ni <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq3.gif" Format="GIF" Height="18" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\(-{3d}^{8}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <msup> <mrow> <mn>3</mn> <mi>d</mi> </mrow> <mn>8</mn> </msup> </mrow> </math></EquationSource> </InlineEquation>) in transition metals are responsible for highest portion of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="32" /> </InlineMediaObject> <EquationSource Format="TEX">\({m}_{tot}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>m</mi> <mrow> <mi mathvariant="italic">tot</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>. Based on <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="35" /> </InlineMediaObject> <EquationSource Format="TEX">\(n(\omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> values of LiXO<sub>2</sub> (<i>X</i> = Co, Ni) delafossite compounds, we can infer that these compounds are optically active materials, as their values are between 1.0 and 2.0. The <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="13538_2025_1815_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="39" /> </InlineMediaObject> <EquationSource Format="TEX">\({\varepsilon }_{2}(\omega )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>ε</mi> <mn>2</mn> </msub> <mrow> <mo stretchy="false">(</mo> <mi>ω</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> spectra demonstrate that LiXO<sub>2</sub> (<i>X</i> = Co, Ni) compounds are auspicious entrants for solar cell appliances working in visible and UV regions. It can be inferred from the computed results that these crystalline materials are promising candidates for prospective photovoltaic appliances.</p>

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Quantum-Engineered LiXO₂ (X = Co, Ni) Delafossites: First-Principles Design of Structural, Optoelectronic, Thermodynamic, and Magnetic Frameworks for Next-Generation Energy Harvesting

  • Zeesham Abbas,
  • Samah Al-Qaisi,
  • Afaf Khadr Alqorashi,
  • Khalida Bibi,
  • Mohd Taukeer Khan,
  • Amna Parveen

摘要

The structural, optoelectronic, and magnetic properties of LiXO2 (X = Co, Ni) delafossite compounds are evaluated using first-principles based DFT calculations to investigate their potential applications in optoelectronic and spintronic devices. Based on calculated ground state energies, LiNiO2 is a more stable compound, compared to LiCoO2. The indirect energy band gap for LiCoO2 and LiNiO2 are 4.95 and 5.02 eV, respectively, in spin (↑) direction. However, in spin (↓) direction, the values of energy band gaps are 2.05 and 1.82 eV for LiCoO2 and LiNiO2, respectively. The total magnetic moment \({m}_{tot}\) m tot values for LiCoO2 are higher, compared to LiNiO2. Unfilled d-orbitals (Co \(-{3d}^{7}\) - 3 d 7 and Ni \(-{3d}^{8}\) - 3 d 8 ) in transition metals are responsible for highest portion of \({m}_{tot}\) m tot . Based on \(n(\omega )\) n ( ω ) values of LiXO2 (X = Co, Ni) delafossite compounds, we can infer that these compounds are optically active materials, as their values are between 1.0 and 2.0. The \({\varepsilon }_{2}(\omega )\) ε 2 ( ω ) spectra demonstrate that LiXO2 (X = Co, Ni) compounds are auspicious entrants for solar cell appliances working in visible and UV regions. It can be inferred from the computed results that these crystalline materials are promising candidates for prospective photovoltaic appliances.