欢迎登录材料期刊网

材料期刊网

高级检索

使用基于密度泛函理论的第一性原理方法,计算研究了Fe掺杂CdTe的晶格结构与电磁性质变化.研究发现,掺杂体系的晶格常数与电子结构等随掺杂Fe原子的位置不同而异.通过能带结构与电子态密度的分析表明,不同占据位的Fe原子表现出迥异的电子能级分布、轨道杂化等,从而引起体系电子性质与原子磁矩的显著变化.其中,替代位与间隙位Fe杂质的原子磁矩分别为3.76和3.14玻尔磁子.这一研究对深入理解掺杂CdTe类稀磁半导体的物理性质有重要意义.

参考文献

[1] H. Ohno.Making Nonmagnetic Semiconductors Ferromagnetic[J].Science,19985379(5379):951-956.
[2] Jamet M;Barski A;Devillers T;Poydenot V;Dujardin R;Bayle-Guillemaud P;Rothman J;Bellet-Amalric E;Marty A;Cibert J.High-Curie-temperature ferromagnetism in self-organized Ge1-xMnx nanocolumns[J].Nature materials,20068(8):653-659.
[3] Mirbt S.;Sanyal B.;Mohn P..Magnetic properties of 3d impurities substituted in GaAs[J].Journal of Physics. Condensed Matter,200212(12):3295-3302.
[4] Luo X;Martin RM.Jahn-Teller distortion and ferromagnetism in the dilute magnetic semiconductors GaAs : Mn and cubic GaN : Mn[J].Physical review, B. Condensed matter and materials physics,20053(3):5212-1-5212-6-0.
[5] Sato K.;Katayama-Yoshida H..First principles materials design for semiconductor spintronics[J].Semiconductor Science and Technology,20024(4):367-376.
[6] Dudarev SL.;Savrasov SY.;Humphreys CJ.;Sutton AP.;Botton GA..Electron-energy-loss spectra and the structural stability of nickel oxide: An LSDA+U study[J].Physical Review.B.Condensed Matter,19983(3):1505-1509.
[7] F. Kuwen;R. Leitsmann;F. Bechstedt.Mn and Fe doping of bulk Si: Concentration influence on electronic and magnetic properties[J].Physical review, B. Condensed matter and materials physics,20094(4):045203:1-045203:7.
[8] AlZahrani, AZ;Srivastava, GP;Garg, R;Migliorato, MA.An ab initio study of electronic and structural properties of Mn in a GaAs environment[J].Journal of Physics. Condensed Matter,200948(48):485504:1-485504:10.
[9] Li, Zhaoning;Wang, Weiping;Zhao, Shicao.Mn-Mn interaction induced metallic or insulating character of doped silicon: An ab initio study[J].Computational Materials Science,2015:186-192.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%