Semiconducting and magnetic lanthanide MXenes from intercalated halides.

Fang, Qian; Wang, Liming; Chang, Kai; Yang, Hongxin; Yan, Pu; Cao, Kecheng; Li, Mian; Xue, Jianming et al. · Nature · 2026

basic_science · Level V

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Abstract

Two-dimensional (2D) magnetic semiconductors are crucial for next-generation information storage and spintronic technologies<sup>1,2</sup>. MXenes, owing to compositional diversity and tunable properties, provide a platform for designing functional materials<sup>3-5</sup>. Incorporating lanthanides (Ln) introduces localized 4f electrons with strong spin polarization, while potentially enabling semiconducting behaviour, offering a viable route to magnetic semiconductors<sup>6,7</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>8</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 d-electron states around the Fermi level (E<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 4f electrons in Ln<sub>2</sub>CT<sub>2</sub>, located far from the E<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.