欢迎登录材料期刊网

材料期刊网

高级检索

采用第一性原理的平面波超软赝势方法,对β-Ga2O3掺Al的AlxGa2-xO3(x=0,0.5,1,1.5,2)合金进行结构优化、电子态密度和能带特性的研究。结果显示,Alx Ga2-x O3为间接宽能隙材料,能隙是由导带底Ga 4s态和价带顶 O 2p 态共同决定,其弯曲系数分别为0.452 eV(直接)和0.373 eV(间接)。当增大Al的掺杂量,Alx Ga2-x O3的体积变小,总能量升高,能隙逐渐增大,这与实验结果相一致。

First-principles plan-wave pseudopotential method was used to calculate the optimized parameters,e-lectron density of states and energy band properties of Ga2-xAlxO3(x=0,0.5,1,1.5,2)alloys by doping Al in-toβ-Ga2 O3 .It was found thatβ-Ga2-x Alx O3 was indirect wide-bandgap material,the bowing parameter was 0.452 eV for direct bandgap and 0.373 eV for indirect bandgap.The bandgap ofβ-Ga2-xAlxO3 was determined by O2p state of valence band maximum and Ga4s state of conduction band minimum.When the increase in Al concentration of Ga2-x Alx O3 ,the volumes decreased,the total energies and the bandgap increased,which was consistent with the experimental results.

参考文献

[1] Orita M.;Hirano M.;Hosono H.;Ohta H. .Deep-ultraviolet transparent conductive beta-Ga2O3 thin films[J].Applied physics letters,2000(25):4166-4168.
[2] Naoyuki Ueda;Hideo Hosono;Ryuta Waseda .Synthesis and control of conductivity of ultraviolet transmittingβ-Ga↓(2)O↓(3) single crystals[J].Applied physics letters,1997(25/26):3561-3563.
[3] Varley J B;Weber J R;Janotti A et al.Oxygen vacan-cies and donor impurities inβ-Ga2 O3[J].Applied Physics Letters,2010,97:1421061-1421063.
[4] Shigeo Ohira;Norihito Suzuki;Naoki Arai;Masahiko Tanaka;Takamasa Sugawara;Kazuo Nakajima;Toetsu Shishido .Characterization of transparent and conducting Sn-doped β-Ga_2O_3 single crystal after annealing[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,2008(17):5763-5767.
[5] Naoyuki Ueda;Hideo Hosono;Ryuta Waseda .Synthesis and control of conductivity of ultraviolet transmittingβ-Ga↓(2)O↓(3) single crystals[J].Applied physics letters,1997(25/26):3561-3563.
[6] Li XF;Zhang Q;Miao WN;Huang L;Zhang ZJ .Transparent conductive oxide thin films of tungsten-doped indium oxide[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,2006(4):2471-2474.
[7] Rubio E J;Ramana C V .Tungsten-incorporation induced red-shift in the bandgap of gallium oxide thin films[J].Applied Physics Letters,2013,102:1919131-1919134.
[8] A.A. Dakhel.Investigation of opto-dielectric properties of Ti-doped Ga_2O_3 thin films[J].Solid state sciences,2013:54-58.
[9] Kong, L.;Ma, J.;Luan, C.;Zhu, Z. .Structural and optical properties of Ga2O3:In films deposited on MgO (1 0 0) substrates by MOCVD[J].Journal of Solid State Chemistry,2011(8):1946-1950.
[10] Kokubun Y;Miura K;Endo F et al.Sol-gelprepared-Ga2 O3 thin films for ultraviolet photodetectors[J].Applied Physics Letters,2007,90:0319121-0319123.
[11] Goyal A;Yadav B S;Thakur O P et al.Effect of an-nealing on b-Ga2 O3 film grown by pulsed laser deposi-tion technique[J].Journal of Alloys and Compounds,2014,583:214-219.
[12] 侯清玉,赵春旺.高掺杂N对金红石型TiO2电子结构和红移影响的理论研究[J].功能材料,2011(05):782-784.
[13] 解小玲,曹青,张俊花.电场对改性煤沥青中间相形成的影响[J].功能材料,2013(01):28-31.
[14] Mohamed M;Janowitz C;Unger I et al.The electronic structure of β-Ga2 O3[J].Applied Physics Letters,2010,97:2119031-2119033.
[15] Zhang Y J;Yan J L;Zhao G et al.First-principles study on electronic structure and optical properties of Sn-doped beta-Ga2 O3[J].PHYSICA B,2010,405:3899-3903.
[16] Masahiro Orita;Hiromichi Ohta;Masahiro Hirano .Deep-ultraviolet transparent conductive β-Ga_(2)O_(3) thin films[J].Applied physics letters,2000(25):4166-4168.
[17] He HY;Orlando R;Blanco MA;Pandey R;Amzallag E;Baraille I;Rerat M .First-principles study of the structural, electronic, and optical properties of Ga2O3 in its monoclinic and hexagonal phases[J].Physical review, B. Condensed matter and materials physics,2006(19):5123-1-5123-8-0.
[18] Geller S .Crystal structure of b-form[J].Journal of Chemical Physics,1960,33:676-684.
[19] Huang HC.;de la Rubia TD.;Gilmer GH. .An atomistic simulator for thin film deposition in three dimensions[J].Journal of Applied Physics,1998(7):3636-3649.
[20] Perdew J P;Burke K;Ernzerhof M .Generalized gradient approximation made simple[J].Physical Review,1996,77:3865-3868.
[21] Vanderbilt D .Soft self-consistent pseudopotentials in a generalized eigenvalue formalism[J].Physical Review B:Condensed Matter,1990,41:7892-7895.
[22] Monkhorst H J;Pack J D .Special points for Brillouin-zone integrations- a reply[J].Physical Review B:Condensed Matter,1977,1 6:1748-1749.
[23] Pfrommer B G;Cote M;Louie S G et al.Relaxation of crystals with the quasi-newton method[J].Journal of Computational Physics,1997,131:133-140.
[24] Yoshioka S;Hayashi H;Kuwabara A;Oba F;Matsunaga K;Tanaka I .Structures and energetics of Ga2O3 polymorphs[J].Journal of Physics. Condensed Matter,2007(34):46211-1-46211-11-0.
[25] Shannon R D;Prewitt C T .Effective ionic radii in oxides and fluorides[J].Acta Cryst,1969,B25:925-946.
[26] He H Y;Blanco M A;Pandey R .Electronic and thermo-dynamic properties of β-Ga2 O3[J].Applied Physics Letters,2006,88:2619041-2619043.
[27] Zheng S W;Gan G H;Li S T et al.Study on the lattice constants and energy band properties of Be and Ca doped wurtzite ZnO[J].Acta Phys Sin,2012,61:2371011-2371019.
[28] Laurenti J P;Roentgen P;Wolter K et al.Indium-doped GaAs:a very dilute alloy system[J].Physical Review B:Condensed Matter,1998,37:4155-4163.
[29] Ferhat M;Zaoui A;Ahuja R .Magnetism and band gap narrowing in Cu-doped ZnO[J].Applied Physics Letters,2009,94:1425021-1425023.
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%