<p>MXenes, specifically MXene <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, are an emerging class of two-dimensional transition metal carbides that have obtained significant attention due to their versatile properties and potential applications through the surface functionalization approach. The surface functionalization of MXenes offers immense possibilities to tailor their properties for a wide range of applications, making them highly flexible materials for next-generation technologies. The current study, using first-principles calculations, has explored the surface decoration of <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> MXene with transition magnetic metals (Fe, Mn, and Ni) to influence their optical, electrical, and magnetic properties. Energy band structures and associated density of states result confirmed that peaks of the <i>d</i>-orbital dominate the electronic states in the Fe, Mn, and Ni-<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> composite. More interestingly, the optical absorption coefficient within ultraviolet and visible infrared regions may be significantly increased by surface decorating with transition magnetic metals Fe, Mn, and Ni-<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> composite. The remarkably improved optical absorption characteristics over a broad-spectral range may be attributed to the enlargement of the interlamellar space along with more active sites and more electronic mobility. The ferromagnetic simulated results revealed that pristine <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> MXene and Ni-<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({\rm{Fe}}-{{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Fe</mi> <mo>−</mo> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> composites are stable and have magnetic moments of 2.10 µB and 3.04 µB, respectively, and confirmed that Fe, Mn, and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({\rm{Ni}}-{{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ni</mi> <mo>−</mo> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> composite is a soft ferromagnetic material. The doped MXene demonstrated a good improvement in ferromagnetic performance as compared to the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({{Ti}}_{3}{C}_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mrow> <mi mathvariant="italic">Ti</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> <msub> <mrow> <mi>C</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> MXene. These results suggest that 2D M-depoed Ti<sub>3</sub>C<sub>2</sub> MXene (M=Fe, Mn, Ni) materials are superior for solar cell and spintronic device applications.</p><p></p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

A first principles calculations to analysis of ferromagnetic stability in 2-dimensional layered structure M-doped MXene Ti3C2 (M=Fe, Mn, Ni) for solar cell application

  • Muhammad Hasnain Jameel,
  • Jia Luo,
  • Aqeela Yaseen,
  • Samreen Kousar,
  • Hongyan Wang,
  • Mohd Zul Hilmi Bin Mayzan,
  • Khaled Althubeiti,
  • Mohammed Aljohani

摘要

MXenes, specifically MXene \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 , are an emerging class of two-dimensional transition metal carbides that have obtained significant attention due to their versatile properties and potential applications through the surface functionalization approach. The surface functionalization of MXenes offers immense possibilities to tailor their properties for a wide range of applications, making them highly flexible materials for next-generation technologies. The current study, using first-principles calculations, has explored the surface decoration of \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 MXene with transition magnetic metals (Fe, Mn, and Ni) to influence their optical, electrical, and magnetic properties. Energy band structures and associated density of states result confirmed that peaks of the d-orbital dominate the electronic states in the Fe, Mn, and Ni- \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 composite. More interestingly, the optical absorption coefficient within ultraviolet and visible infrared regions may be significantly increased by surface decorating with transition magnetic metals Fe, Mn, and Ni- \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 composite. The remarkably improved optical absorption characteristics over a broad-spectral range may be attributed to the enlargement of the interlamellar space along with more active sites and more electronic mobility. The ferromagnetic simulated results revealed that pristine \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 MXene and Ni- \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 and \({\rm{Fe}}-{{Ti}}_{3}{C}_{2}\) Fe Ti 3 C 2 composites are stable and have magnetic moments of 2.10 µB and 3.04 µB, respectively, and confirmed that Fe, Mn, and \({\rm{Ni}}-{{Ti}}_{3}{C}_{2}\) Ni Ti 3 C 2 composite is a soft ferromagnetic material. The doped MXene demonstrated a good improvement in ferromagnetic performance as compared to the \({{Ti}}_{3}{C}_{2}\) Ti 3 C 2 MXene. These results suggest that 2D M-depoed Ti3C2 MXene (M=Fe, Mn, Ni) materials are superior for solar cell and spintronic device applications.