首页> 外文学位 >Noise in gallium nitride-based quantum well structures used for nanometer devices in the frequency range 1 Hz--3 Mhz and temperature range 77K--324K.
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Noise in gallium nitride-based quantum well structures used for nanometer devices in the frequency range 1 Hz--3 Mhz and temperature range 77K--324K.

机译:用于频率为1 Hz--3 Mhz和温度范围为77K--324K的纳米器件的基于氮化镓的量子阱结构中的噪声。

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摘要

Electronic noise has been investigated in AlxGa1−x N/GaN Modulation-Doped Field Effect Transistors (MODFETs) of submicron dimensions, grown for us by MBE (Molecular Beam Epitaxy) techniques at Virginia Commonwealth University by Dr. H. Morkoç and coworkers. Some 20 devices were grown on a GaN substrate, four of which have leads bonded to source (S), drain (D), and gate (G) pads, respectively. Conduction takes place in the quasi-2D layer of the junction (xy plane) which is perpendicular to the quantum well (z-direction) of average triangular width ∼3 nm. A non-doped intrinsic buffer layer of ∼5 nm separates the Si-doped donors in the AlxGa1−xN layer from the 2D-transistor plane, which affords a very high electron mobility, thus enabling high-speed devices. Since all contacts (S, D, and G) must reach through the AlxGa1−xN layer to connect internally to the 2D plane, parallel conduction through this layer is a feature of all modulation-doped devices. While the shunting effect may account for no more than a few percent of the current IDS, it is responsible for most excess noise, over and above thermal noise of the device.; The excess noise has been analyzed as a sum of Lorentzian spectra and 1/f noise. The Lorentzian noise has been ascribed to trapping of the carriers in the AlxGa1−xN layer. A detailed, multitrapping generation-recombination noise theory is presented, which shows that an exponential relationship exists for the time constants obtained from the spectral components as a function of 1/kT. The trap depths have been obtained from Arrhenius plots of log (τT2) vs. 1000/T. Comparison with previous noise results for GaAs devices shows that: (a) many more trapping levels are present in these nitride-based devices; (b) the traps are deeper (farther below the conduction band) than for GaAs. Furthermore, the magnitude of the noise is strongly dependent on the level of depletion of the AlxGa1−xN donor layer, which can be altered by a negative or positive gate bias VGS.; Altogether, these frontier nitride-based devices are promising for bluish light optoelectronic devices and lasers; however, the noise, though well understood, indicates that the purity of the constituent layers should be greatly improved for future technological applications.
机译:已经通过MBE(分子束)为我们开发了亚微米尺寸的Al x Ga 1-x N / GaN调制掺杂场效应晶体管(MODFET),研究了电子噪声H.Morkoç博士及其同事在弗吉尼亚联邦大学的外延技术。在GaN衬底上生长了大约20个器件,其中四个器件的引线分别与源极(S),漏极(D)和栅极(G)焊盘相连。导电发生在结的准二维层( xy 平面)中,该层垂直于平均三角形宽度约为3 z 方向)。 > nm 。约5 nm 的非掺杂本征缓冲层将Al x Ga 1-x N层中的Si掺杂施主与二维晶体管平面,具有很高的电子迁移率,因此可实现高速设备。由于所有触点(S,D和G)必须穿过Al x Ga 1-x N层到达内部以连接到2D平面,因此通过该层的平行传导是所有调制掺杂器件的功能。尽管分流效应可能只占当前IDS的百分之几,但它是造成大多数超额噪声的原因,这些噪声超出了器件的热噪声。多余的噪声已被分析为洛伦兹谱和1 / f 噪声之和。洛伦兹噪声归因于载流子在Al x Ga 1-x N层中的俘获。提出了详细的多陷阱生成-重组噪声理论,该理论表明,从频谱分量获得的时间常数与1 / kT呈指数关系。陷阱深度从log的阿伦尼乌斯图(τT 2 )对1000 / T获得。与以前的GaAs器件噪声结果比较表明:(a)这些基于氮化物的器件中存在更多的俘获能级; (b)阱比GaAs更深(比导带更远)。此外,噪声的大小强烈依赖于Al x Ga 1-x N供体层的耗尽程度,可以通过负或正改变栅极偏置VGS。总的来说,这些基于氮化物的 frontier 器件有望用于带蓝光的光电器件和激光器。然而,尽管噪声已被很好地理解,但它表明对于未来的技术应用,应当大大提高组成层的纯度。

著录项

  • 作者

    Duran, Rolando Silvano.;

  • 作者单位

    Florida International University.;

  • 授予单位 Florida International University.;
  • 学科 Engineering Electronics and Electrical.; Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2002
  • 页码 139 p.
  • 总页数 139
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 无线电电子学、电信技术;工程材料学;
  • 关键词

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