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TEM study of defects in Al_xGa_(1-x)N layers with different polarity

机译:不同极性Al_xGa_(1-x)N层中缺陷的TEM研究

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摘要

Transmission electron microscopy (TEM) studies of defects in Al_xGa_(1-x)N layers with various Al mole fractions (x=0.2, 0.4) and polarities were carried out. The samples were grown by ammonia molecular beam epitaxy on sapphire substrates and consisted of low-temperature A1N (LT-AIN) and high-temperature A1N (HT-AIN) buffer layers, a complex AIN/AlGaN superlattice (SL) and an Al_xGa_(1-x)N layer (x=0.2, 0.4). It was observed that at the first growth stages a very high density of dislocations is introduced in both Al-polar and N-polar structures. Then, at the interface of the LT-AIN and HT-AIN layers half-loops are formed and the dislocation density considerably decreases in Al-polar structures, whereas in the N-polar structures such a behavior was not observed. The AIN/AlGaN superlattice efficiently promotes the bend and annihilation of threading dislocations and respectively the decrease of the dislocation density in the upper Al_xGa_(1-x)N layer with both polarities. The lattice relaxation of metal-polar Al_(0.8)Ga_(0.2)N was observed, while N-polar Al_(0.8)Ga_(0.2) did not relax. The dislocation densities in the N-polar Al_(0.8)Ga_(0.2)N and Al_(0.4)Ga_(0.6)N layers were 5.5 × 10~9 cm~(-2) and 9 × 10~9 cm~(-2), respectively, and in metal-polar Alo^Gao^N and Alo.4Gao.6N layers these were lxl010cm"2 and 6 × 10~9 cm~(-2), respectively. Moreover, from TEM images the presence of inversion domains (IDs) in N-polar structures has been observed. The widths of IDs varied from 10 to 30 ran. Some of the IDs widen during the growth of the A1N buffer layers. The IDs formed hills on the surface of the N-polar structures.
机译:透射电子显微镜(TEM)研究了具有不同Al摩尔分数(x = 0.2,0.4)和极性的Al_xGa_(1-x)N层中的缺陷。样品通过氨分子束外延在蓝宝石衬底上生长,并由低温AlN(LT-AIN)和高温AlN(HT-AIN)缓冲层,复杂的AIN / AlGaN超晶格(SL)和Al_xGa_( 1-x)N层(x = 0.2,0.4)。据观察,在第一生长阶段,在Al-极性和N-极性结构中都引入了非常高的位错密度。然后,在LT-AIN和HT-AIN层的界面处形成半环,并且在Al-极性结构中位错密度显着降低,而在N-极性结构中未观察到这种行为。 AIN / AlGaN超晶格有效地促进了具有两种极性的上位Al_xGa_(1-x)N层中螺纹位错的弯曲和an没,并分别降低了位错密度。观察到金属极性的Al_(0.8)Ga_(0.2)N的晶格弛豫,而N极性的Al_(0.8)Ga_(0.2)没有弛豫。 N极Al_(0.8)Ga_(0.2)N和Al_(0.4)Ga_(0.6)N层中的位错密度分别为5.5×10〜9 cm〜(-2)和9×10〜9 cm〜(- 2)分别在金属极性的Alo ^ Gao ^ N和Alo.4Gao.6N层中分别为1xl010cm“ 2和6×10〜9 cm〜(-2)。此外,根据TEM图像,已经观察到N极结构中的反转区(IDs),IDs的宽度从10到30nm不等,一些IDs在AlN缓冲层的生长过程中变宽,IDs在N-表面上形成了丘陵。极性结构。

著录项

  • 来源
    《Journal of Crystal Growth》 |2012年第1期|p.30-34|共5页
  • 作者单位

    Institute of Semiconductor Physics, Siberian Branch of the Russian Academy of Sciences, Lavrentieva Avenue 13, 630090 Novosibirsk, Russia;

    Institute of Semiconductor Physics, Siberian Branch of the Russian Academy of Sciences, Lavrentieva Avenue 13, 630090 Novosibirsk, Russia;

    Institute of Semiconductor Physics, Siberian Branch of the Russian Academy of Sciences, Lavrentieva Avenue 13, 630090 Novosibirsk, Russia;

    Research Institute for Technical Physics and Materials Science, Hungarian Academy of Sciences, P.O. Box 49, H-1525 Budapest, Hungary;

    Research Institute for Technical Physics and Materials Science, Hungarian Academy of Sciences, P.O. Box 49, H-1525 Budapest, Hungary;

  • 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
  • 关键词

    A1. Defects; A1. Nucleation; A3. Molecular beam epitaxy; B1. Nitrides;

    机译:A1。缺陷;A1。成核;A3。分子束外延;B1。氮化物;
  • 入库时间 2022-08-17 13:17:02

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