首页> 外文期刊>Journal of Applied Physics >Optical characterization of digital alloy In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P multi-quantum-wells grown by molecular beam epitaxy
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Optical characterization of digital alloy In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P multi-quantum-wells grown by molecular beam epitaxy

机译:通过分子束外延生长的数字合金In_(0.49)Ga_(0.51)P / In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P多量子阱的光学表征

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An In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P multi-quantum-well (MQW) structure grown by molecular beam epitaxy using a digital alloy method was parametrically investigated by photoluminescence (PL) measurement performed in a temperature range of 10-290 K. The PL peak energies did not change with increasing temperature up to 60 K, while the PL peak energy monotonously decreased with increasing temperature beyond 60 K. From the curve fit of the linewidth full width at half maximum of the PL peak, it was observed that the homogeneous broadening of In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P MQW with digital alloy barriers due to scattering by longitudinal optical phonons was smaller than that of InGaAs/InGaAlAs MQW with digital alloy barriers. This is in accordance with the existence of a relatively weak phonon-related PL peak in the PL spectrum of InGaAlP digital alloy, as compared with InGaAlAs digital alloy. The fit of the integrated PL intensity shows the occurrence of a nonradiative recombination process with an activation energy E_1=24A meV up to 60 K. On the other hand, the process of nonradiative recombination with an activation energy E_2=109 meV occurred above 60 K, which is in good agreement with one-half of the calculated total confinement energy ΔE of the electron-hole pair in the quantum well (~108 meV). The In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P MQW structure with digital alloy barriers has larger activation energy (E_2= 109 meV) than In_(0.49)Ga_(0.51)P/In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P MQW (E_2=90 meV) with analog alloy barriers. Therefore, the thermal emission of carriers into the barrier can be reduced at temperatures above 60 K due to the high effective barrier height.
机译:使用数字合金方法通过分子束外延生长的In_(0.49)Ga_(0.51)P / In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P多量子阱(MQW)结构为通过在10-290 K的温度范围内执行的光致发光(PL)测量进行参数研究。PL峰值能量在温度升高至60 K时不会随温度升高而变化,而PL峰值能量在温度超过60 K时会单调降低。在PL峰的最大值的一半处的线宽全宽的曲线拟合表明,In_(0.49)Ga_(0.51)P / In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51由于纵向光学声子的散射,具有数字合金势垒的P MQW比具有数字合金势垒的InGaAs / InGaAlAs MQW小。与InGaAlAs数字合金相比,这是由于InGaAlP数字合金的PL光谱中存在相对弱的与声子有关的PL峰。积分PL强度的拟合显示了激活能量E_1 = 24A meV至60 K的非辐射重组过程的发生。另一方面,激活能量E_2 = 109 meV的非辐射重组的过程发生于60 K以上,这与计算出的量子阱中电子-空穴对的总限制能量ΔE的一半(约108 meV)非常吻合。具有数字合金势垒的In_(0.49)Ga_(0.51)P / In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P MQW结构比In_(0.49)具有更大的活化能(E_2 = 109 meV)具有模拟合金势垒的)Ga_(0.51)P / In_(0.49)(Ga_(0.6)Al_(0.4))_(0.51)P MQW(E_2 = 90 meV)。因此,由于高的有效势垒高度,在高于60 K的温度下,可以减少载流子进入势垒的热辐射。

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