欢迎登录材料期刊网

材料期刊网

高级检索

采用反应磁控溅射法在不同工作气压(0.5~2.0 Pa)下沉积了一系列氮化铝(AIN)薄膜.研究发现,在保持其他工艺参数不变的条件下,工作气压对薄膜厚度的影响很小.场发射性能测试表明,在较低的工作气压(0.5 Pa和0.7 Pa)下制备的A1N薄膜具有一定的场发射性能.扫描电子显微镜(SEM)图像显示,在较高的工作气压(2.0 Pa)下制备的薄膜易产生空位及微空洞等缺陷,使薄膜致密性下降.电子在薄膜中的输运因受到缺陷的散射而不能隧穿表面势垒进行发射.研究表明,为获得具有良好场发射性能的A1N薄膜,若采用反应磁控溅射法,应选取较低的工作气压;同时,对于薄膜型阴极,具有紧密晶粒结构及较小缺陷的薄膜可能具有更优异的场发射性能.

参考文献

[1] Brodie I,Schwoebel P R.Vacuum microelectronic devices[J].Proceeding of the IEEE,1994,82(7):1006-1034.
[2] Mahanandia P,Arya V,Bhotla P V,et al.semialigned carbon nanofibers grownon cylindrical copper surface[J].Appl.Phys.Lett.,2009,95(8):083108(1-3).
[3] Joseph P T,Tai N H,Lee C Y,et al.Field emission enhancement in nitrogen-ion-implanted ultrananocrystalline diamond films[J].J.Appl.Phys.,2008,103(4):043720(1-7).
[4] You J B,Zhang X W.Enhancement of field emission of the ZnO film by the reduced work function and the increased conductivity via hydrogen plasma treatment[J].Appl.Phys.Lett.,2009,94(26):262105(1-3).
[5] Thapa R,Saha B,Chattopadhyay K K.Enhanced field emission from Si doped nanocrystalline A1N thin films[J].Appl.Surf.Sci.,2009,255(8):4536-4541.
[6] Huang A P,Paul K,Wu X L,et al.Enhanced electron field emission from oriented columnar A1N[J].Appl.Phys.Lett.,2006,88(25):251103(1-3).
[7] Zhao Q,Feug S Q,Zhu Y Z,et al.Annealing effects on the field emission properties of A1N nanorods[J].Nanotechnology,2006,17 (11):S351-S354.
[8] Tang Y B,Cong H T,Wang Z M,et al.Catalyst-seeded synthesis and field emission properties of flowerlike Sidoped A1N nanoneedle array[J].Appl.Phys.Lett.,2006,89(25),253112(1-3).
[9] Wang Y X,Li Y A,Feng W,et al.Influence of thickness on field emission characteristics of A1N thin films[J].App.Surf.Sci.,2005,243(1-4):394-400.
[10] Ji X Y,Zhang Q Y,Lau S P,et al.Temperature-dependent photoluminescence and electron field emission properties of A1N nanotip arrays[J].Appl.Phys.Lett.,2009,94(17):173106 (1-3).
[11] Bian H J,Chen X F,Pan J S,et al.Excellent field emission from Effects of sputtering pressure on the field emission properties of N-doped SrTiO3[J].Appl.Surf.Sci.,2009,255(9):4867-4872.
[12] Vashaei Z,Aikawa T,Ohtsuka M,et al.Influence of sputtering parameters on the crystallinity and crystal orientation of A1N layers deposited by RF sputtering using the A1N target[J].Crystal Growth,2009,311(3):459-462.
[13] Yue S L,Shi C Y.Enhanced electron field emission from oriented A1N films[J].J.Appl.Phys.,2006,99(9):094908(1-4).
[14] Lee J H.Effects of sputtering pressure and thickness on properties of ZnO:A1 films deposited on polymer substrates[J].J.Electroceram,2009,23(1-4):512-518.
[15] Hwang D K,Oh M S,Choi Y S,et al.Effect of pressure on the properties of phosphorus-doped p-type ZnO thin films grown by radio frequency-magnetron sputtering[J].Appl.Phys.Lett.,2008,92 (16):161109 (1-3).
[16] Negi S,Bhandari R,Rieth L,et al.Effect of sputtering pressure on pulsed-DC sputtered iridium oxide films[J].Sensor and Actuators B:Chemical,2009,137(1):370-387..
[17] Seki K,Xu X Q.Room-temperature growth of AIN thin films by laser ablation[J].Appl.Phys.Lett.,1992,60(18):2234-2236.
[18] Wu Q,Hu Z,Wang X Z,et al.Synthesis and optical characterization of aluminum nitride Nanobelts[J].J.Phys.Chem.B,2003,107(36):9726-9729.
[19] 程守洙,江之久.普通物理学[M].北京:教育出版社,1982.
[20] 徐学基,诸定昌.气体放电物理[M].上海:复旦大学出版社,1996.
[21] Cutler P H,Miskovsky N M,Lerner P B,et al.The use of internal field emission to inject electronic charge carriers into the conduction band of diamond films:a review[J].Appl.Surf.Sci.,1999,146(1-4):126-133.
[22] Zhao Q,Xu J,Xu X Y,et al.Field emission from AIN nanoneedle arrays[J].Appl.Phys.Lett.,2004,85(22):5331-5333.
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%