<p>Two-dimensional (2D) magnetic semiconductors are crucial for next-generation information storage and spintronic technologies<sup><CitationRef CitationID="CR1">1</CitationRef>,<CitationRef CitationID="CR2">2</CitationRef></sup>. MXenes, owing to compositional diversity and tunable properties, provide a platform for designing functional materials<sup><CitationRef AdditionalCitationIDS="CR4" CitationID="CR3">3</CitationRef>–<CitationRef CitationID="CR5">5</CitationRef></sup>. Incorporating lanthanides (Ln) introduces localized 4<i>f</i> electrons with strong spin polarization, while potentially enabling semiconducting behaviour, offering a viable route to magnetic semiconductors<sup><CitationRef CitationID="CR6">6</CitationRef>,<CitationRef CitationID="CR7">7</CitationRef></sup>. However, the scarcity of MAX precursors and the susceptibility of Ln to dissolution in common etchants (for example, HF), compared with other M elements such as Mo, hinder the synthesis of lanthanide MXenes (Ln<sub>2</sub>CT<sub>2</sub>) by conventional ‘top-down’ etching<sup><CitationRef CitationID="CR8">8</CitationRef></sup>. Here we propose a general ‘bottom-up’ methodology for synthesizing Ln<sub>2</sub>CT<sub>2</sub> (Ln = Gd, Tb, Dy, Ho, Er, Lu; T = Cl, Br) using layered halides as van der Waals building blocks. Multilayer Ln<sub>2</sub>CT<sub>2</sub> exhibits composition-tunable properties, characterized by optical absorption onsets spanning 1.26–1.71 eV, room-temperature resistivity of 0.329–36.1 Ω cm with a negative temperature coefficient, and low-temperature ferromagnetic hysteresis at 2 K accompanied by positive Curie–Weiss temperatures between 6 K and 59 K. Theoretical calculations show that the <i>d</i>-electron states around the Fermi level (<i>E</i><sub>f</sub>) are largely diminished in bare Ln<sub>2</sub>C, whereas surface terminals further exhaust these states to open band gaps. Meanwhile, the highly localized 4<i>f</i> electrons in Ln<sub>2</sub>CT<sub>2</sub>, located far from the <i>E</i><sub>f</sub>, contribute to the spin splitting for the observed ferromagnetic behaviour. This combination of semiconducting and magnetic properties makes Ln<sub>2</sub>CT<sub>2</sub> a valuable candidate for spintronic device applications.</p>

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Semiconducting and magnetic lanthanide MXenes from intercalated halides

  • Qian Fang,
  • Liming Wang,
  • Kai Chang,
  • Hongxin Yang,
  • Pu Yan,
  • Kecheng Cao,
  • Mian Li,
  • Jianming Xue,
  • Xiaoping Ouyang,
  • Zhifang Chai,
  • Qing Huang

摘要

Two-dimensional (2D) magnetic semiconductors are crucial for next-generation information storage and spintronic technologies1,2. MXenes, owing to compositional diversity and tunable properties, provide a platform for designing functional materials35. Incorporating lanthanides (Ln) introduces localized 4f electrons with strong spin polarization, while potentially enabling semiconducting behaviour, offering a viable route to magnetic semiconductors6,7. However, the scarcity of MAX precursors and the susceptibility of Ln to dissolution in common etchants (for example, HF), compared with other M elements such as Mo, hinder the synthesis of lanthanide MXenes (Ln2CT2) by conventional ‘top-down’ etching8. Here we propose a general ‘bottom-up’ methodology for synthesizing Ln2CT2 (Ln = Gd, Tb, Dy, Ho, Er, Lu; T = Cl, Br) using layered halides as van der Waals building blocks. Multilayer Ln2CT2 exhibits composition-tunable properties, characterized by optical absorption onsets spanning 1.26–1.71 eV, room-temperature resistivity of 0.329–36.1 Ω cm with a negative temperature coefficient, and low-temperature ferromagnetic hysteresis at 2 K accompanied by positive Curie–Weiss temperatures between 6 K and 59 K. Theoretical calculations show that the d-electron states around the Fermi level (Ef) are largely diminished in bare Ln2C, whereas surface terminals further exhaust these states to open band gaps. Meanwhile, the highly localized 4f electrons in Ln2CT2, located far from the Ef, contribute to the spin splitting for the observed ferromagnetic behaviour. This combination of semiconducting and magnetic properties makes Ln2CT2 a valuable candidate for spintronic device applications.