欢迎登录材料期刊网

材料期刊网

高级检索

在类石墨烯结构的Bi2Se3拓扑绝缘体夹层中化学掺杂Cu原子形成CuxBi2Se3.Cu含量为12at%~15at%,温度为3.8~4.2 K时,CuxBi2Se3块体内呈现超导电性,称之为拓扑超导体.CuxBi2Se3拓扑超导体是一种时间反演不变超导体,体电子态为满带能隙超导态,表面为无能隙Andreev束缚态,并且由于强自旋-轨道耦合效应具有三维狄拉克能带结构.科学家在CuxBi2Se3拓扑超导体中捕捉到了长期以来寻找的零质量零电荷的马拉约那费米子.马拉约那费米子不被附近的粒子、原子吸引或排斥,强烈对抗无序和杂质,这种容错特性将有效保护脆弱的量子态不受侵害,为将来自旋量子学和量子计算机的实现提供新平台.本文针对CuxBi2Se3拓扑超导体这一新型量子材料论述其理论和实验研究进展,然后结合材料科学学科特征论述CuxBi2Se3掺杂特性和反位缺陷形成特征,提出通过控制反位缺陷浓度和合理掺杂提高CuxBi2Se3的物理和化学性能的理论.

参考文献

[1] Hasan, M.Z.;Kane, C.L. .Colloquium: Topological insulators[J].Reviews of Modern Physics,2010(4):3045-3067.
[2] Fu L;Kane C L;Mele E J .[J].Physical Review Letters,2007,98:106803.
[3] Hsieh D;Xia Y;Qian D et al.[J].Nature,2009,8:1101.
[4] Kane C L;Mele E J .[J].Physical Review Letters,2005,95:226801.
[5] Hsieh D;Qian D;Wray L;Xia Y;Hor YS;Cava RJ;Hasan MZ .A topological Dirac insulator in a quantum spin Hall phase.[J].Nature,2008(7190):970-974.
[6] Chen Y L;Analytis J G;Chu J H et al.[J].Science,2009,325:178.
[7] He K;Xue Q K .[J].Nature Physics,2010,6:584.
[8] Moore J E .[J].Nature,2010,464:194.
[9] Zhang, HJ;Liu, CX;Qi, XL;Dai, X;Fang, Z;Zhang, SC .Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface[J].Nature physics,2009(6):438-442.
[10] Hor Y S;Williams A J;Checkelsky J G et al.[J].Physical Review Letters,2010,104:057001.
[11] Wray, L.A.;Xu, S.-Y.;Xia, Y.;Hor, Y.S.;Qian, D.;Fedorov, A.V.;Lin, H.;Bansil, A.;Cava, R.J.;Hasan, M.Z. .Observation of topological order in a superconducting doped topological insulator[J].Nature physics,2010(11):855-859.
[12] Moore J E;Balents L .[J].Physical Review B:Condensed Matter,2007,75:121306.
[13] Fu L;Kane C L .[J].Physical Review Letters,2008,100:096407.
[14] Xia, Y;Qian, D;Hsieh, D;Wray, L;Pal, A;Lin, H;Bansil, A;Grauer, D;Hor, YS;Cava, RJ;Hasan, MZ .Observation of a large-gap topological-insulator class with a single Dirac cone on the surface[J].Nature physics,2009(6):398-402.
[15] Noah B A;Stephan H.[J].Physica,2010(03)
[16] Hsieh D;Xia Y;Qian D et al.[J].Physical Review Letters,2009,103:146401.
[17] Sau J D;Lutchyn R M;Tewari S et al.[J].Physical Review Letters,2010,104:040502.
[18] Fu L;Kane C L .[J].Physical Review B:Condensed Matter,2009,79:161408.
[19] Tanaka Y;Yokoyama T;Nagaosa N .[J].Physical Review Letters,2009,103:107002.
[20] Babak Seradjeh;Eytan Grosfeld .[J].Physical Review B:Condensed Matter,2011,83:104513.
[21] Linder J;Tanaka Y;Yokoyana T et al.[J].Physical Review Letters,2010,104:067001.
[22] Urazhdin S;Bilc D;Tessmer S H;S D et al.[J].Physical Review B:Condensed Matter,2002,66:161306.
[23] Navrátil J;Horák J;Plechacek T et al.[J].Journal of Solid State Chemistry,2004,177:1704.
[24] Zhang Y;Chang C Z;He K et al.[J].Applied Physics Letters,2010,97:194102.
[25] Kulbachinskii VA.;Nakagawa H.;Arimoto H.;Ikaida T.;Lostak P. Drasar C.;Miura N. .Conduction-band structure of Bi2-xSbxSe3 mixed crystals by Shubnikov-de Haas and cyclotron resonance measurements in high magnetic fields[J].Physical Review.B.Condensed Matter,1999(24):15733-15739.
[26] Sklenár C Drasar;Krejcová A et al.[J].Crystal Research and Technology,2000,35:1069.
[27] Kulbachinskii V A;Yu A;Kaminskiia A et al.[J].Journal of Magnetism and Magnetic Materials,2004,272-276:1991.
[28] Janicek, P;Drasar, C;Lostak, P;Vejpravova, J;Sechovsky, V .Transport, magnetic, optical and thermodynamic properties of Bi2-xMnxSe3 single crystals[J].Physica. B, Condensed Matter,2008(19/20):3553-3558.
[29] Ka(s)parováJ;Dra(s)ar(E);KrejèováA et al.[J].Journal of Applied Physics,2005,97:103720.
[30] Cho S;Kim Y;DiVenere A et al.[J].Applied Physics Letters,1999,75:1401.
[31] Rudro R;Biswas A;Balatsky V .[J].Physical Review B:Condensed Matter,2010,81:233405.
[32] Park S R;Jung W S;Chul Kim et al.[J].Physical Review B:Condensed Matter,2010,81:041405.
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%