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Field emission from undoped and nitrogen-doped tetrahedral amorphous carbon film prepared by filtered cathodic vacuum arc technique

机译:通过过滤的阴极真空弧技术制备的未掺杂和氮掺杂四面向非晶碳膜的场发射

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摘要

The field emission results from undoped and nitrogen doped tetrahedral amorphous carbon (ta-C andta-C:N) prepared by the filtered cathodic vacuum arc (FCVA) technique, deposited on both n{sup}+and p{sup}+ -type Si are reported. The effect of different types of Si substrate and the film thicknesson the onset electric field has been investigated. Three sets of ta-C samples with differing dopingconcentrations were used in the study: undoped p-type ta-C (p-ta-C), nitrogen weakly doped intrinsicta-C (i-ta-C) and nitrogen heavily doped n{sup}+ -type ta-C (n{sup}+ -ta-C). The heterojunction-based field emission model gives a reasonable explanation for the behavior of the onset electric fieldmeasured. The heavily doped hetero-Junction n{sup}+ -ta-C/p{sup}+ -Si, demonstrated the lowestonset field of 10 V μm{sup}-1 with current densities of 0.1 mA mm{sup}-2 at 50 V μm{sup}- 1due to the Zener tunneling arising from the severe band bending. A film thickness of 30-40 nm is morefavorable for field emission due to the ease with which the film can be fully depleted. At somelocations of i-ta-C films, various types of craters were formed after an electrical discharge at a highfield (~58 V μm{sup}-1) followed by a subsequent reduction in the onset field to about 15 V μm{sup}-1.
机译:由过滤的阴极真空弧(FCVA)技术制备的未掺杂和氮掺杂的四面体无定形碳(TA-C AndTA-C:N)的场发射产生,沉积在N {SUP} +和P {SUP} + -TYPE上据报道。研究了不同类型的Si衬底和薄膜厚度的效果已经研究了起始电场。在研究中使用了三组具有不同掺杂共同融合的TA-C样品:未掺杂的P型Ta-C(P-TA-C),氮弱掺杂的内壁Irta-C(I-Ta-C)和氮掺杂N { sup} + -type ta-c(n {sup} + -ta-c)。基于异质的场发射模型对起始电场探测器的行为提供了合理的解释。重掺杂的异结合N {sup} + -ta-c / p {sup} + -si,展示了10vμm{sup} -1的Lowestonset字段,其电流密度为0.1 mm mm {sup} -2 50 Vμm{sup} - 从严重带弯曲引起的齐纳隧道的1due。由于薄膜可以完全耗尽,薄膜厚度为30-40nm的薄膜厚度对于场发射。在I-TA-C薄膜的索收下,在高壁处的放电(〜58Vμm{sup} -1)上的放电后形成各种类型的陨石坑,然后在发作场的后续还原到约15vμm{sup } -1。

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