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Effect of ridge waveguide etch depth on laser threshold of InGaN MQW laser diodes

机译:脊形波导蚀刻深度对InGaN MQW激光二极管激光阈值的影响

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摘要

The laser threshold and lateral mode confinement of blue (440 ran) InGaN multiple quantum well (MQW) laser diodes have been investigated. Ridge-waveguide (RW) laser diodes with different ridge etch depth ranging from 25 nm above the active region (deep-ridge waveguide) to 200 nm above the active region (shallow-ridge waveguide) have been fabricated. The comparison of devices with the same resonator length shows that the threshold current densities are significantly lower for deep-ridge waveguide laser diodes. The difference in lasing threshold becomes more eminent for narrow ridges, which are required for single mode operation. For shallow-ridge devices the threshold current density increases by more than a factor of three when the ridge width is decreased from 20μm to 1.5μm. For the deep-ridge waveguide devices instead, the lasing threshold is almost independent of the ridge waveguide width. The effect has been analyzed by 2D self-consistent electro-optical simulations. For deep-ridge devices, the simulated thresholds and far-field patterns are in good agreement with the simulations. For shallow-ridge devices, however, questionable theoretical assumptions are needed. Two possible causes are discussed: extremely large current spreading and strong index anti-guiding.
机译:研究了蓝色(440 ran)InGaN多量子阱(MQW)激光二极管的激光阈值和横向模式限制。已经制造了具有不同的脊蚀刻深度的脊波导(RW)激光二极管,其蚀刻范围从有源区上方25 nm(深脊波导)到有源区上方200 nm(浅脊波导)。具有相同谐振器长度的器件的比较表明,深脊波导激光二极管的阈值电流密度明显较低。对于单模式操作所需的窄脊,激射阈值的差异变得更加明显。对于浅脊型器件,当脊宽从20μm减小到1.5μm时,阈值电流密度将增加三倍以上。对于深脊波导器件,激射阈值几乎与脊波导宽度无关。已经通过2D自洽电光仿真分析了该影响。对于深脊器件,模拟的阈值和远场模式与模拟非常吻合。然而,对于浅脊器件,需要有可疑的理论假设。讨论了两种可能的原因:极大的电流扩展和强指数反导。

著录项

  • 来源
    《Gallium nitride materials and devices VII》|2012年|p.826219.1-826219.8|共8页
  • 会议地点 San Francisco CA(US)
  • 作者单位

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Technische Universitaet Berlin, Hardenbergstrasse 36, 10623 Berlin, Germany;

    NUSOD Institute LLC, Newark, Delaware 19714-7204, USA;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany,Technische Universitaet Berlin, Hardenbergstrasse 36, 10623 Berlin, Germany;

    Ferdinand-Braun-Institut, Leibniz-Institut fuer Hoechstfrequenztechnik, Gustav-Kirchhoff-Strasse 4,12489 Berlin, Germany;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 材料;
  • 关键词

    InGaN laser diodes; threshold current density; ridge width; ridge depth; far field pattern; current spreading; index anti-guiding;

    机译:InGaN激光二极管;阈值电流密度;脊宽垄深远场模式电流扩散;指数反导;

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