首页> 外文会议>Information and Communication Technologies, 2006. ICTTA '06. 2nd >InAs self-assembled quantum dot and quantum dash lasers on InP for 1.55μm optical telecommunications
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InAs self-assembled quantum dot and quantum dash lasers on InP for 1.55μm optical telecommunications

机译:用于1.55μm光通信的InP上的InAs自组装量子点和量子破折号激光器

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1.3 mum quantum dot (QD) lasers grown on GaAs substrates have recently shown promising performances. For the 1.55 mum wavelength range, QD structures grown on InP substrates have been proposed to produce lasers for long haul telecom. At this wavelength, the progress has been delayed by the difficulties to obtain high density of small QDs by molecular beam epitaxy. On (100) InP substrates, elongated structure named quantum dash (QDH) are achieved in the standard conditions. The growth on high index substrates allows the achievement of a higher density of smaller quantum dots. In this paper, we compare laser performance of devices elaborated on both substrates. After quantum dot elaboration optimization, on (311) B substrates, laser emission at 1.59 mum on the ground state transition is obtained at room temperature (RT), A very low threshold current density (Jth) of 21 A/cm2 for the best QD lasers is measured. This value can be compared to the Jth of quantum well (QW) laser, which are in the few hundred A/cm2. On (100) substrates laser emission is observed at 1.45 mum for a current density of 375 A/cm2 at RT. The evolution of the Jth and of the emission wavelength as a function of temperature is studied on both structures. The changes are interpreted in terms of density of states and of form of the gain curve
机译:在GaAs衬底上生长的1.3微米量子点(QD)激光器最近显示出令人鼓舞的性能。对于1.55微米的波长范围,已提出在InP衬底上生长的QD结构可生产用于长途电信的激光器。在此波长下,由于难以通过分子束外延获得高密度的小QD而延缓了进展。在(100)InP衬底上,在标准条件下获得了称为量子破折号(QDH)的细长结构。在高折射率衬底上的生长允许实现更高密度的较小量子点。在本文中,我们比较了在两种基板上加工的器件的激光性能。经过量子点精细化优化后,在(311)B衬底上,在室温(RT)下获得了基态跃迁上1.59 mum的激光发射,极低的阈值电流密度(Jth)为21 A / cm 2 测量最佳QD激光器。该值可以与几百A / cm2的量子阱(QW)激光器的Jth进行比较。在(100)基板上,在RT下以1.45 mum的电流密度为375 A / cm2观察到激光发射。在两种结构上都研究了Jth和发射波长随温度的变化。根据状态的密度和增益曲线的形式来解释这些变化。

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