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Cadmium Zinc Oxide Based Optoelectronics Materials and Devices.

机译:氧化镉锌基光电材料和器件。

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摘要

Cadmium Znic Oxide (CdZnO) based optoelectronics materials and devices are studied and discussed in this dissertation. CdZnO thin films with various Cd:Zn mol ratios were grown by molecular-beam epitaxy (MBE) on silicon (Si) and c-plane sapphire substrates, respectively. Room temperature (RT) photoluminescence (PL) showed the peak position of the near band edge (NBE) emission of the CdZnO thin films shifted from 3.30eV to 2.59eV on Si (100) substrates, while it shifted from 3.26eV to 2.40eV on c-plane sapphire substrates. The color of the RT PL emission of the CdZnO thin films covers from ultraviolet (UV) to blue region on Si (100) substrates, and to green region on c-plane sapphire substrates. The NBE emission peak energy was estimated to be the band gap energy of the CdZnO thin films at RT. Energy-dispersive X-ray spectroscopy (EDS) study of the CdZnO thin films showed Cd:Zn ratio increased with the decrease of the band gap energy of the CdZnO. X-ray diffraction (XRD) studies showed the crystal structure of the CdZnO thin films changed from the pure wurtzite (wz) structure to mixture of wz and rocksalt (rs) structure, and finally to pure rs structure with the increases of Cd:Zn ratio. Temperature dependent PL measurements were performed on three typical CdZnO samples having pure wz, pure rs, and wz-rs mixture structures, respectively. The temperature dependence of the CdZnO bandgap change was investigated and analyzed based on the empirical Varshni and Bose-Einstein fitting on the NBE PL peak positions. The temperature dependence of the integral PL intensity in the CdZnO samples was also fitted, where fitting equation with hopping term showed a closer fit to the experimental data. The possible hopping processes in the CdZnO thin films may be related to the band tail states due to alloying effect and nonuniformity of Cd distribution in the CdZnO samples. Rapid thermal annealing (RTA) at different temperature was performed on in situ annealed CdZnO thin films to study the thermal stability of the CdZnO. Pure wz CdZnO showed insignificant NBE PL peak shift after RTA, while mixture structure CdZnO showed evident blue shifts due to phase change after annealing, indicating the rs phase CdZnO changes to wz phase CdZnO during RTA process. On the other hand, CdZnO thin films without in situ annealing showed dramatic NBE emission peak energy increase with increasing RTA temperature. RT PL and temperature dependent PL showed phase separations in the samples after the annealing process. Secondary ion mass spectroscopy (SIMS) measurements showed redistribution of Cd in the as-annealed sample, which is believed to be the reason of PL peaks shift. ZnO heterojunction samples with CdZnO active layers were grown on p-type Si (100) substrate and n-type Si (100) substrate, with structures of n-ZnO/i-CdZnO/ p-Si and p-ZnO/i-CdZnO/ n-ZnO/n-Si, respectively. Light emitting diodes (LEDs) fabricated from both samples showed typical diode rectifying I-V curves. Blue and cyan color emissions were observed under forward bias at RT. RT PL measurements at different thicknesses on the sample showed the existence of CdZnO active layer. Temperature dependent electroluminescence (EL) showed that the change of EL peak energy agree with Varshni equation, while RT PL verified that the EL emission come from the CdZnO layer. Devices with metal-insulator-semiconductor structure and ZnO p-n junction with CdZnO quantum well structure were grown and fabricated respectively. Random laser emissions were observed from both of the devices under forward bias. Closely packed column structures are believed to serve as random resonance cavities for the laser emissions.
机译:本文研究和讨论了基于氧化镉镉(CdZnO)的光电材料和器件。通过分子束外延(MBE)在硅(Si)和c面蓝宝石衬底上分别生长具有各种Cd:Zn摩尔比的CdZnO薄膜。室温(RT)光致发光(PL)显示在Si(100)衬底上CdZnO薄膜的近带边缘(NBE)发射的峰值位置从3.30eV移至2.59eV,而从3.26eV移至2.40eV在c面蓝宝石衬底上。 CdZnO薄膜的RT PL发射的颜色覆盖了从紫外线(UV)到Si(100)衬底上的蓝色区域以及c面蓝宝石衬底上的绿色区域。 NBE发射峰能量估计为CdZnO薄膜在室温下的带隙能量。 CdZnO薄膜的能量色散X射线光谱(EDS)研究表明,随着CdZnO带隙能的减小,Cd:Zn比值增加。 X射线衍射(XRD)研究表明,随着Cd:Zn的增加,CdZnO薄膜的晶体结构从纯纤锌矿(wz)结构变为wz和岩盐(rs)结构的混合体,最终变为纯rs结构。比。对三个具有纯wz,纯rs和wz-rs混合物结构的典型CdZnO样品分别进行了温度依赖性PL测量。基于经验值Varshni和Bose-Einstein对NBE PL峰位置的拟合,研究和分析了CdZnO带隙变化的温度依赖性。还拟合了CdZnO样品中PL积分强度的温度依赖性,其中带有跳跃项的拟合方程显示出与实验数据更接近。由于合金化效应和CdZnO样品中Cd分布的不均匀性,CdZnO薄膜中可能的跳跃过程可能与带尾态有关。在原位退火的CdZnO薄膜上进行了不同温度下的快速热退火(RTA),以研究CdZnO的热稳定性。纯wz CdZnO在RTA后显示出微不足道的NBE PL峰移动,而混合结构CdZnO由于退火后的相变而显示出明显的蓝移,表明在RTA过程中rs相CdZnO变为wz相CdZnO。另一方面,未经原位退火的CdZnO薄膜显示出显着的NBE发射峰能量随RTA温度的升高而增加。退火处理后,RT PL和温度依赖性PL在样品中显示出相分离。二次离子质谱(SIMS)测量表明,退火样品中Cd的重新分布,这被认为是PL峰移动的原因。具有CdZnO有源层的ZnO异质结样品在具有n-ZnO / i-CdZnO / p-Si和p-ZnO / i-CdZnO结构的p型Si(100)衬底和n型Si(100)衬底上生长/ n-ZnO / n-Si。由两个样品制成的发光二极管(LED)显示出典型的二极管整流I-V曲线。在RT的正向偏压下观察到蓝色和青色的发射。在样品上不同厚度的RT PL测量表明存在CdZnO活性层。与温度有关的电致发光(EL)表明,EL峰值能量的变化与Varshni方程相符,而RT PL验证了EL的发射来自CdZnO层。生长并制造了具有金属-绝缘体-半导体结构和具有CdZnO量子阱结构的ZnO p-n结的器件。在正向偏压下,两个器件均观察到随机激光发射。据信紧密堆积的柱结构可以用作激光发射的随机共振腔。

著录项

  • 作者

    Li, Lin.;

  • 作者单位

    University of California, Riverside.;

  • 授予单位 University of California, Riverside.;
  • 学科 Engineering Electronics and Electrical.;Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2011
  • 页码 122 p.
  • 总页数 122
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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