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About the physical meaning of the critical temperature for catastrophic optical damage in high power quantum well laser diodes

机译:关于大功率量子阱激光二极管中灾难性光学损伤的临界温度的物理含义

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It is usually assumed that the catastrophic optical damage of high power laser diodes is launched when a critical local temperature (Tc) is reached; temperatures ranging from 120 degrees C to 200 degrees C were experimentally reported. However, the physical meaning of Tc in the degradation process is still unclear. In this work we show that, in the presence of a local heat source in the active region, the temperature of the laser structure, calculated using finite element methods, is widely inhomogeneously distributed among the different layers forming the device. This is due to the impact that the low dimensionality and the thermal boundary resistances have on the thermal transport across the laser structure. When these key factors are explicitly considered, the quantum well (QW) temperature can be several hundred degrees higher than the temperature of the guides and cladding layers. Due to the size of the experimental probes, the measured critical temperature is a weighted average over the QW, guides, and claddings. We show the existence of a large difference between the calculated average temperature, equivalent to the experimentally measured temperature, and the peak temperature localized in the QW. A parallel study on double heterostructure lasers is also included for comparison.
机译:通常认为,当达到临界局部温度(Tc)时,会引发大功率激光二极管的灾难性光学损坏;实验报道的温度范围为120摄氏度至200摄氏度。但是,Tc在降解过程中的物理含义仍不清楚。在这项工作中,我们表明,在有源区域中存在局部热源的情况下,使用有限元方法计算出的激光结构的温度在形成器件的不同层之间分布广泛且不均匀。这是由于低尺寸和热边界电阻对跨激光器结构的热传输的影响。明确考虑这些关键因素后,量子阱(QW)温度可能会比波导层和覆层的温度高数百度。由于实验探针的尺寸,所测得的临界温度是QW,导轨和包层上的加权平均值。我们表明,计算出的平均温度(相当于实验测量的温度)与QW中的峰值温度之间存在很大差异。还包括对双异质结构激光器的并行研究,以进行比较。

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