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On the optical polarization properties of semipolar (2021) and (2021) InGaN/GaN quantum wells

机译:半极性(2021)和(2021)InGaN / GaN量子阱的光偏振特性

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In the framework of k . p-theory, semipolar (20 (2) over bar1) and (20 (2) over bar(1) over bar) InGaN/GaN quantum wells (QWs) have equivalent band structures and are expected to have identical optical polarization properties. However, (20 (2) over bar1) QWs consistently exhibit a lower degree of linear polarization (DLP) than (20 (2) over bar(1) over bar) QWs. To understand this peculiarity, we investigate the optical properties of (20 (2) over bar1) and (20 (2) over bar(1) over bar) InGaN/GaN single QW light-emitting diodes (LEDs) via resonant polarization-resolved photoluminescence microscopy. LEDs were grown on bulk substrates by metal organic vapor phase epitaxy with different indium concentrations resulting in emission wavelengths between 442 nm and 491 nm. We discuss the origin of their DLP via k . p band structure calculations. An analytical expression to estimate the DLP in the Boltzmann-regime is proposed. Measurements of the DLP at 10 K and 300 K are compared to m-plane LEDs and highlight several discrepancies with calculations. We observe a strong correlation between DLPs and spectral widths, which indicates that inhomogeneous broadening affects the optical polarization properties. Considering indium content fluctuations, QW thickness fluctuations, and the localization length of charge carriers, we argue that different broadenings apply to each subband and introduce a formalism using effective masses to account for inhomogeneous broadening in the calculation of the DLP. We conclude that the different DLP of (20 (2) over bar1) and (20 (2) over bar(1) over bar) QWs might be related to different effective broadenings of their valence subbands induced by the rougher upper QW interface in (20 (2) over bar1), by the larger sensitivity of holes to this upper interface due to the polarization field in (20 (2) over bar, and/or by the different degrees of localization of holes. Published by AIP Publishing.
机译:在k的框架中。 p理论,半极性(bar1上方为20(2)和bar(1)上方为(20(2)))InGaN / GaN量子阱(QW)具有等效的能带结构,并且有望具有相同的光偏振特性。但是,(bar1)QW上的(20(2))始终比bar(1)bar(Q1)上的(20(2))高。为了理解这种特性,我们通过共振偏振分辨技术研究了(1 bar上方的(20(2))和(1 bar上方的bar(1))(20(2))的光学特性光致发光显微镜。通过具有不同铟浓度的金属有机气相外延在大块基板上生长LED,从而产生442 nm至491 nm的发射波长。我们通过k讨论其DLP的起源。 p带结构计算。提出了一种估计玻尔兹曼体制中DLP的解析表达式。将DLP在10 K和300 K时的测量结果与m平面LED进行了比较,并通过计算突出了几个差异。我们观察到DLP与光谱宽度之间有很强的相关性,这表明不均匀加宽会影响光学偏振特性。考虑到铟含量的波动,QW厚度的波动以及电荷载流子的定位长度,我们认为不同的展宽适用于每个子带,并采用有效质量引入形式主义以解决DLP计算中的不均匀展宽。我们得出结论,(bar1)上方(20(2)和bar(1)上方bar(1)上方)(20(2))的不同DLP可能与由(由于在杆上方(20(2)中的极化场)和/或由于孔的本地化程度不同,孔对上部接口的敏感性较高,和/或由于孔的局部化程度不同,因此在bar1)上方具有20(2)。

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  • 来源
    《Journal of Applied Physics》 |2018年第8期|085705.1-085705.10|共10页
  • 作者单位

    Univ Freiburg, Dept Microsyst Engn IMTEK, Freiburg, Germany;

    Tech Univ Berlin, Inst Solid State Phys, Berlin, Germany;

    Tech Univ Berlin, Inst Solid State Phys, Berlin, Germany;

    Tech Univ Berlin, Inst Solid State Phys, Berlin, Germany;

    Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Elect & Comp Engn Dept, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Elect & Comp Engn Dept, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA;

    Univ Calif Santa Barbara, Dept Mat, Santa Barbara, CA 93106 USA;

    Tech Univ Chemnitz, Inst Phys, Chemnitz, Germany;

  • 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);
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  • 正文语种 eng
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