欢迎登录材料期刊网

材料期刊网

高级检索

基于密度泛函理论(DFT)的第一性原理方法,在广义梯度近似(GGA)下分别计算了无掺杂和掺杂过渡金属Cr原子的AlN半导体的电磁性质,结果表明,掺杂后AlN由半导体转变为半金属,并具有较宽的半金属能隙.当掺杂浓度为25%、12.5%、5.6%时,半金属能隙分别为0.8eV、1.1eV、1.2eV.以掺杂浓度为12.5%的Cr-AlN(2×2×1)为例,详细分析了其能带结构、态密度分布和电子布居数以及磁矩等.

The electromagnetic properties of transition metal Cr doped AlN semiconductor is studied by densityfunctional theory using the generalized gradient approximation(GGA) for the exchange-correlation potential.The pure AlN crystal and Cr doped AlN are calculated respectively,the results indicate that Cr doped AlN is a semi-metal with a wide range of half-metallic energy gap.When the Cr doped concentration is 25%,12.5%,5.6%,the half-metallic energy gap is 0.8eV,1.1eV and 1.2eV,respectively.In this paper,Cr-AlN(2×2×1)(Cr doped concentration is 12.5%) is taken for an example to analyze its band structures,density of states,electron population and the magnetic moment,etc.

参考文献

[1] 傅英,徐文兰,陆卫.半导体量子电子和光电子器件[J].物理学进展,2001(03):255-277.
[2] 任尚坤,张凤鸣,都有为.半金属磁性材料[J].物理学进展,2004(04):381-397.
[3] Fang CM.;de Wijs GA.;de Groot RA. .Spin-polarization in half-metals (invited)[J].Journal of Applied Physics,2002(10 Pt.3):8340-8344.
[4] C. Y. Fong;M. C. Qian;J. E. Pask;L. H. Yang;S. Dag .Electronic and magnetic properties of zinc blende half-metal superlattices[J].Applied physics letters,2004(2):239-241.
[5] P. A. Dowben;R. Skomski .Are half-metallic ferromagnets half metals? (invited)[J].Journal of Applied Physics,2004(11):7453-7458.
[6] 蔡建旺;赵建高;詹文山 .磁电子学中的若干问题[J].物理学进展,1997,17(02):119.
[7] WU Xue-Wei,NIU Dong-Lin,LIU Xiao-Jun.Photoinduced Spin Disorder in Half-Metal CrO2 films[J].中国物理快报(英文版),2006(11):3072-3075.
[8] 蒋荣华,肖顺珍,李艳.氮化物半导体的研究进展[J].半导体技术,2000(06):16-20.
[9] Jain S C;Willander M et al.Ⅲ-nitrides:Growth,characterization,and properties[J].Applied Physics,2000,87:965.
[10] Adivarahan, V;Sun, WH;Chitnis, A;Shatalov, M;Wu, S;Maruska, HP;Khan, MA .250 nm AlGaN light-emitting diodes[J].Applied Physics Letters,2004(12):2175-2177.
[11] Shi Lijie;Liu Banggui .Half-metallic ferromagnetism in hexagonal MAl7N8 and cubic MAl3N4 (M = Cr and Mn) from first principles[J].Physical Review B:Condensed Matter,2007,76:115201.
[12] 林秋宝,李仁全,曾永志,朱梓忠.TM掺杂的Ⅲ-Ⅴ族稀磁半导体电磁性质的第一原理计算[J].物理学报,2006(02):873-878.
[13] Wu R Q et al.Possible efficient p-type doping of AlN using Be:An ab initio study[J].Applied Physics Letters,2007,91:152110.
[14] Kresse G.;Joubert D. .From ultrasoft pseudopotentials to the projector augmented-wave method[J].Physical Review.B.Condensed Matter,1999(3):1758-1775.
[15] Adolph B;Furthmuller J;Bechstedt F .Optical properties of semiconductors using projector-augmented waves[J].Physical Review.B.Condensed Matter,2001(12):5108-1-5108-8-0.
[16] Blochl P E .Projector augmented-wave method[J].Physical Review B:Condensed Matter,1994,50:17953.
[17] Kresse G;Furthmuller J .Efficiency of ab-initio total energy calculations for metals and semiconductors using a planewave basis set[J].Computational Materials Science,1996,6:15.
[18] Shang G;Peacock P W;Robertson J .Stability and bandoffsets of nitrogenated high-dielectric-constant gate oxides[J].Applied Physics Letters,2004,84:106.
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%