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The temperature dependence of 1.3- and 1.5-Μm compressivelystrained InGaAs(P) MQW semiconductor lasers

机译:1.3和1.5 Mm压缩应变InGaAs(P)MQW半导体激光器的温度依赖性

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We have studied experimentally and theoretically the spontaneousnemission from 1.3- and 1.5-Μm compressively strained InGaAsPnmultiple-quantum-well lasers in the temperature range 90-400 K tondetermine the variation of carrier density n with current I up tonthreshold. We find that the current contributing to spontaneous emissionnat threshold IRad is always well behaved and has ancharacteristic temperature T0 (IRad)≈T, asnpredicted by simple theory. This implies that the carrier density atnthreshold is also proportional to temperature. Below a breakpointntemperature TB, we find I Α nZ, where Z=2.nAnd the total current at threshold Ith also has ancharacteristic temperature T0 (Ith)≈T, showingnthat the current is dominated by radiative transitions right up tonthreshold. Above TB, Z increases steadily to Z≈3 andnT0 (Ith) decreases to a value less than T/3. Thisnbehavior is explained in terms of the onset of Auger recombination abovenTB; a conclusion supported by measurements of the pressurendependence of Ith. From our results, we estimate that, at 300nK, Auger recombination accounts for 50% of Ith in then1.3-Μm laser and 80% of Ith in the 1.5-Μm laser.nMeasurements of the spontaneous emission and differential efficiencynindicate that a combination of increased optical losses and carriernoverflow into the barrier and separate confinement heterostructurenregions may further degrade T0 (Ith) above roomntemperature
机译:我们已经在理论和实验上研究了在90-400 K的温度范围内1.3和1.5 Mm压缩应变InGaAsPn多量子阱激光器的自发发光,以确定载流子密度n随着电流I up tonthreshold的变化。我们发现,有助于自发发射阈值IRad的电流始终表现良好,并且具有简单理论所预测的特征温度T0(IRad)≈ T。这意味着载流子密度阈值也与温度成正比。在断点温度TB以下,我们发现I A nZ,其中Z = 2.n,并且在阈值Ith处的总电流也具有特征温度T0(Ith)≈ T,这表明电流主要由向tonthreshold处的辐射跃迁控制。在TB之上,Z稳定地增加到Z≈ 3,nT0(Ith)减小到小于T / 3的值。这种行为是根据高于TB的俄歇重组的发生来解释的。由Ith的压力依赖性测量支持的结论。根据我们的结果,我们估计在300nK时,俄歇复合在1.3μm激光中占Ith的50%,在1.5μm激光中占Ith的80%.n自发发射和差分效率的测量表明,增加的光损耗和载流子溢出进入势垒和单独的限制异质结构区域可能会进一步在室温以上降低T0(Ith)

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