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GaN/SiC heterojunctions grown by LP-CVD

机译:LP-CVD生长的GaN / SiC异质结

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Heterojunction bipolar transistors (HJBT) on the basis of GaN/SiC heterostructures have several advantages over group III nitride heterostructur es grown on sapphire. For example 6H-SiC has less of a thermal and structural mismatch to GaN than sapphire has. Furthermore there is not the problem of optical recombination in a highly doped base region as there is for the group III nitrides on account of their direct bandgap. However, despite the well acknowledged potential of the GaN/SiC material system there are still unanswered questions relating to the technology used as well as to some fundamental properties of GaN/SiC heterostructures. Therefore we investigated epitaxial growth and physical properties of n-GaN/p-SiC heterojunctions with respect to their significance to n-GaN/p-SiC-SiC HJBT. We grew n-type GaN (n = 10~18 cm~(-3)) on p-type (p = 2 × 10~18 cm~(-3)) and n-type (n = 4 × 10~18 cm~(-3)) 6H-SiC substrates in a horizontal hot wall reactor. This approach is very similar to the more common HVPE. Instead of synthesizing GaCl in situ from HCl and metallic Ga we used GaCl_3 as the Ga precursor. All our experiments were carried out at low pressures around l mbar resulting in a good homogeneity. As it is common for the more usual HVPE we grew GaN without a buffer layer. From thermal admittance spectroscopy (TAS) as well as temperature dependent IV characteristics we gained knowledge about deep level defects and the role of interface traps. The microstructure of the interface was investigated by transmission electron microscopy (TEM). Furthermore we present details abo
机译:基于GaN / SiC异质结构的异质结双极晶体管(HJBT)与在蓝宝石上生长的III族氮化物异质结构相比具有多个优势。例如,6H-SiC与蓝宝石相比,与GaN的热和结构失配更少。此外,在高掺杂的基极区域中不存在光学复合的问题,因为III族氮化物由于其直接带隙而存在。然而,尽管GaN / SiC材料系统具有公认的潜力,但仍存在与所用技术以及GaN / SiC异质结构的一些基本性能有关的悬而未决的问题。因此,我们研究了n-GaN / p-SiC异质结对n-GaN / p-SiC / n-SiC HJBT的重要性的外延生长和物理性质。我们在p型(p = 2×10〜18 cm〜(-3))和n型(n = 4×10〜18)上生长了n型GaN(n = 10〜18 cm〜(-3))。 cm-(-3))6H-SiC衬底在卧式热壁反应器中。这种方法与更常见的HVPE非常相似。代替由HCl和金属Ga原位合成GaCl,我们使用GaCl_3作为Ga前体。我们所有的实验都是在约1 mbar的低压下进行的,从而实现了良好的均匀性。对于更常见的HVPE,我们通常生长没有缓冲层的GaN。通过热导谱(TAS)以及与温度相关的IV特性,我们获得了有关深层缺陷和界面陷阱的知识。通过透射电子显微镜(TEM)研究了界面的微观结构。此外,我们再次介绍细节

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