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Growth of low basal plane dislocation density epilayers of 4H-silicon carbide for stable bipolar diodes.

机译:用于稳定双极二极管的4H-碳化硅的低基面位错密度外延层的生长。

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摘要

Silicon carbide (SiC) offers great promise in future high power, high voltage, high temperature, high frequency and high radiation environment applications. However, currently one key high power device, SiC bipolar diode, experiences degradation of forward voltage drop during operation, which is the major obstacle in the development of this device. It was reported that the degradation is caused by the propagation of stacking faults in the diode structure. The nucleation sites of stacking faults were studied in this work, and the primary nucleation site was found to be basal plane dislocation (BPD). The BPD density in conventional state-of-the-art SiC epilayers is about 100-500 cm-2, that is, a device with the area of 1 mm x 1 mm will cover at least one BPD. In this work, a novel method was developed to eliminate BPDs during epitaxy, and low BPD density (less than 10 cm-2) and BPD-free SiC epilayers were obtained in our laboratory. The key approach is to subject the SiC substrate to defect preferential etching, followed by conventional epitaxial growth. The creation of BPD etch pits on the substrate surface can greatly enhance the conversion of BPDs to threading edge dislocations during epitaxy, and thus low BPD density and BPD-free epilayers are obtained. It was also demonstrated that SiC bipolar diodes fabricated on such a novel epilayer do not exhibit stacking fault propagation and forward voltage drop degradation during operation. A US provisional patent application was filed based on the above results.; The evolution of dislocations during SiC epitaxial growth is investigated. During conventional SiC epitaxy, 70-90% of BPDs in the substrate are converted to become threading edge dislocations as a result of image force, while the other 10-30% of BPDs will propagate into the epilayer. Prior to this work, the reason why only some BPDs get converted during epitaxy, while others still propagate was not clear in the field. This problem was made clear in this work by using a new approach to track dislocations from SiC epilayer to the substrate.; High-quality (0001) SiC epilayers are obtained in our home-built CVD system at a growth rate up to 25 mum/hr. The typical RMS roughness of the 10-30 mum thick epilayers is about 0.6 nm. The net doping concentration (Nd-Na) of the epilayers is controlled to be less than 1015 cm-3 n-type by adjusting the C/Si ratio. Thick epilayers up to 80 mum, and large diameter epilayers up to 2-inch are also obtained.
机译:碳化硅(SiC)在未来的高功率,高电压,高温,高频和高辐射环境应用中具有广阔的前景。然而,当前一种重要的大功率器件SiC双极二极管在运行过程中正向压降下降,这是该器件开发的主要障碍。据报道,这种劣化是由二极管结构中堆叠故障的传播引起的。在这项工作中研究了堆垛层错的成核位置,发现主要成核位置是基底平面错位(BPD)。常规的最新SiC外延层中的BPD密度约为100-500 cm-2,也就是说,面积为1 mm x 1 mm的设备将覆盖至少一个BPD。在这项工作中,开发了一种新的方法来消除外延过程中的BPD,并且在我们的实验室中获得了低BPD密度(小于10 cm-2)和无BPD的SiC外延层。关键方法是对SiC衬底进行缺陷优先刻蚀,然后进行常规的外延生长。在衬底表面上形成BPD刻蚀坑可以极大地增强BPD在外延期间向螺纹边缘位错的转化,从而获得低BPD密度和无BPD外延层。还证明了在这种新颖的外延层上制造的SiC双极二极管在操作过程中不会表现出堆叠故障传播和正向压降降级。基于上述结果,提交了美国临时专利申请。研究了SiC外延生长过程中位错的演变。在常规的SiC外延工艺中,由于图像力的作用,基板中70-90%的BPD转变为穿线边缘的位错,而其他10-30%的BPD将传播到外延层中。在进行这项工作之前,尚不清楚外延过程中只有一些BPD转换而其他BPD仍传播的原因。通过使用一种新的方法来跟踪从SiC外延层到衬底的位错,这一问题在这项工作中得到了明确的体现。高质量(0001)SiC外延层是在我们的自制CVD系统中获得的,增长率高达25 mum / hr。 10-30微米厚的外延层的典型RMS粗糙度约为0.6 nm。通过调节C / Si比,将外延层的净掺杂浓度(Nd-Na)控制为小于1015cm-3 n型。还可以获得高达80毫米的厚外延层和高达2英寸的大直径外延层。

著录项

  • 作者

    Zhang, Zehong.;

  • 作者单位

    University of South Carolina.;

  • 授予单位 University of South Carolina.;
  • 学科 Engineering Electronics and Electrical.; Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2005
  • 页码 133 p.
  • 总页数 133
  • 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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