Wei Xiao-Ping, Du Lan-Lan, Meng Jiang-Liu, Tao Xiaoma
The School of Mathematics and Physics, Lanzhou Jiaotong University, Lanzhou 730070, P. R. China.
Lanzhou Center for Theoretical Physics, Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University, Lanzhou, Gansu 730000, P. R. China.
Phys Chem Chem Phys. 2024 Aug 22;26(33):22099-22111. doi: 10.1039/d4cp01665c.
Two-dimensional room-temperature intrinsic ferromagnetic semiconductors have attracted widespread attention due to their applications in spintronic devices. However, it is difficult for the material to have a Curie temperature above room temperature according to the Mermin-Wagner theorem. By using the method of band engineering, we design a new promising two-dimensional room-temperature intrinsic ferromagnetic semiconductor CrXP (X = P, As, Sb) with large magnetization. The formation of a semiconducting gap for CrXP is discussed in terms of hybridization, occupation and distribution of electronic states and charge transfer. Large magnetic moments of about 6.16-6.37 originate from the occupation of Cr-d electrons in the crystal field. Competition between Cr-d-Cr-d and Cr-d-X-p-Cr-d exchange interactions leads to the emergence of a ferromagnetic order phase. Furthermore, Curie temperatures, approaching 278 K, 464 K and 1590 K for CrP, CrAsP and CrSbP, are estimated by employing Monte Carlo simulations based on the Heisenberg model. The magnetic anisotropy energy of CrXP is discussed using magnetic second-order perturbation theory. In addition, CrXP possesses excellent thermodynamic, dynamical, thermal and mechanical stabilities and can overcome its own gravity to retain its planar structure without the support of the substrate. These above-mentioned advantages will offer some valuable insights into two-dimensional intrinsic ferromagnetic semiconductor CrXP in spintronic devices.
二维室温本征铁磁半导体因其在自旋电子器件中的应用而受到广泛关注。然而,根据默明 - 瓦格纳定理,该材料很难具有高于室温的居里温度。通过能带工程方法,我们设计了一种具有大磁化强度的新型二维室温本征铁磁半导体CrXP(X = P、As、Sb)。从电子态的杂化、占据和分布以及电荷转移的角度讨论了CrXP半导体间隙的形成。约6.16 - 6.37的大磁矩源于晶体场中Cr - d电子的占据。Cr - d - Cr - d和Cr - d - X - p - Cr - d交换相互作用之间的竞争导致了铁磁有序相的出现。此外,通过基于海森堡模型的蒙特卡罗模拟估计,CrP、CrAsP和CrSbP的居里温度分别接近278 K、464 K和1590 K。利用磁二阶微扰理论讨论了CrXP的磁各向异性能量。此外,CrXP具有优异的热力学、动力学、热稳定性和机械稳定性,并且在没有衬底支撑的情况下能够克服自身重力保持其平面结构。上述优点将为自旋电子器件中的二维本征铁磁半导体CrXP提供一些有价值的见解。