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Electro-optical characteristics of 808nm ridge-waveguide lasers operated with high-current nanosecond pulses

机译:大电流纳秒脉冲操作的808nm脊形波导激光器的电光特性

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摘要

The aim of this paper is to present detailed experimental and theoretical investigations of the behavior of ridge-waveguide (RW) lasers emitting at 808 nm under injection of 3 ns long current pulses with amplitudes higher than 10 A. The RW lasers are based on tensile-strained GaAsP quantum wells embedded in asymmetric and extremely asymmetric AlGaAs based waveguide structures, which differ mainly in the ratio between the thicknesses of the p-and n-type confinement layers. The width of the ridges is 4.4 mu m and the length of the cavities is 3.9 mm. The laser diodes are mounted on an in-house developed high-frequency unit electrically driven by nearly rectangular shaped current pulses with a length of 3 ns and a repetition frequency of 1MHz. At a pulse current of 15 A maximum pulse powers of 4.0 and 5.4W are reached for the asymmetric and extremely asymmetric structures, respectively. After turning off the bias a pronounced negative current superimposed by current oscillations caused by the external circuitry appears. Two-dimensional simulations based on a solution of the time-dependent drift-diffusion, waveguide and power-balance equations reveal that a part of the carriers injected into the laser diode does not recombine in the active region and accumulates under the ridge in the bulk layers and beyond the ridge in the active layer. At the end of the electrical pulse the electrons flow back and generate a reverse (negative) current. The simulation exaggerates the achievable output power, in particular for the extremely asymmetric structure. Further theoretical studies are needed to resolve this discrepancy.
机译:本文的目的是对在3 ns长的振幅大于10 A的长电流脉冲的注入下在808 nm处发射的脊形波导(RW)激光器的行为进行详细的实验和理论研究。RW激光器基于拉伸应变的GaAsP量子阱嵌入不对称和极不对称的基于AlGaAs的波导结构中,其主要区别在于p型和n型约束层的厚度之比。脊的宽度为4.4μm,腔的长度为3.9mm。激光二极管安装在内部开发的高频单元上,该高频单元由长度为3 ns,重复频率为1MHz的近似矩形电流脉冲驱动。在15 A的脉冲电流下,非对称和极不对称结构的最大脉冲功率分别达到4.0和5.4W。关闭偏置后,会出现由外部电路引起的电流振荡叠加的明显负电流。基于随时间变化的漂移扩散,波导和功率平衡方程的解的二维仿真显示,注入激光二极管的部分载流子不会在有源区中重新结合,而是聚集在主体的脊下。层和有源层中的脊之外。在电脉冲结束时,电子流回并产生反向(负)电流。该模拟夸大了可达到的输出功率,特别是对于极不对称的结构。需要进一步的理论研究来解决这种差异。

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  • 来源
    《Semiconductor science and technology》 |2017年第4期|045016.1-045016.11|共11页
  • 作者单位

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, Germany;

    Leibniz Inst Hochstfrequenztech, Ferdinand Braun Inst, Gustav Kirchhoff Str 4, D-12489 Berlin, 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);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    diode laser; ridge waveguide laser; gain switching; short pulses; high power;

    机译:二极管激光器;脊形波导激光器;增益切换;短脉冲;高功率;

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