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Characterization of Si_(1-x)Ge_x/Si layers and depth profile of their heterobipolar transistor structures by high-resolution x-ray diffractometry and computer simulations

机译:Si_(1-x)Ge_x / Si层的表征及其异质双极晶体管结构的深度轮廓通过高分辨率x射线衍射法和计算机模拟

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摘要

Using high-resolution x-ray diffractometry (HRXRD) and computer simulations, germanium content x, thickness T of pseudomorphic Si_(1-x)Ge_x layers, and Ge depth profile in their advanced heterobipolar transistor (HBT) structures grown on (001)Si substrates have been determined. High-resolution rocking curves (RCs) with well-resolved intensity oscillations have been recorded by using a double-crystal x-ray diffractometer in (+,-) geometry with Cu Kα_1 radiation from a 12-kW rotating anode x-ray generator. The experimental RCs were simulated with the in-house developed computer program based on the semikinematical theory. In addition to the Ge depth profile, the thickness of SiGe layer, Si cap layer, and SiGe plateau layers of the HBT structures have been determined for the best fit of the experimental RCs with the theoretically simulated RCs. Due to the decay of intensity oscillations, in the case of partially relaxed layers, the values of germanium content x and relaxation R were calculated from the perpendicular and parallel (in-plane) lattice constants a_⊥ and a_‖ obtained by recording a pair of RCs from symmetric and asymmetric lattice planes. The simulation method using HRXRD has been described with the help of typical results obtained from samples of different structures. In this method the maximum error values of x and T are, respectively, ±0.5% and 1%. The error in the value of R is ±2% for partially relaxed samples. In the case of HBT structures, the maximum error in the value pf thickness of SiGe and cap layers is ± 1% and that of plateau layer is ± 5%. The method is very convenient, faster, accurate, and nondestructive in comparison with other methods such as transmission electron microscopy and Secondary-ion-mass spectroscopy.
机译:使用高分辨率X射线衍射仪(HRXRD)和计算机模拟,在(001)上生长的先进异质双极晶体管(HBT)结构中的锗含量x,伪晶Si_(1-x)Ge_x层的厚度T和Ge深度分布已经确定了Si衬底。通过使用双晶X射线衍射仪以(+,-)几何形状使用来自12 kW旋转阳极X射线发生器的CuKα_1辐射记录了具有良好解析的强度振荡的高分辨率摇摆曲线(RC)。基于半运动学原理,使用内部开发的计算机程序模拟了实验性钢筋混凝土。除了Ge深度轮廓外,还确定了HBT结构的SiGe层,Si盖层和SiGe平台层的厚度,以使实验RC与理论上模拟的RC最佳匹配。由于强度振荡的衰减,在部分弛豫层的情况下,锗含量x和弛豫R的值是根据记录一对晶格常数而获得的垂直和平行(面内)晶格常数a_⊥和a_‖计算得出的来自对称和不对称晶格平面的RC。借助于从不同结构的样本获得的典型结果,已经描述了使用HRXRD的模拟方法。在这种方法中,x和T的最大误差值分别为±0.5%和1%。对于部分松弛的样品,R值的误差为±2%。对于HBT结构,SiGe和盖层的pf厚度值的最大误差为±1%,而平台层的pf值的最大误差为±5%。与其他方法(例如透射电子显微镜和二次离子质谱法)相比,该方法非常方便,快捷,准确且无损。

著录项

  • 来源
    《Journal of Applied Physics》 |2005年第2期|p.024509.1-024509.6|共6页
  • 作者单位

    Materials Characterization Division, National Physical Laboratory, Dr. K.S. Krishnan Road, New Delhi-110012, India;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 应用物理学;
  • 关键词

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