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Current carrier lifetime in doping superlattice crystals

机译:掺杂超晶格晶体的电流载体寿命

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It is shown, that the lifetime of nonequilibrium current carriers in the luminescence process in doping superlattice structures changes in a wide range with increasing the excitation level of the crystal. Two effects are important, i.e., (1) low-dimensional character of the carrier distribution and (b) change in the overlap of electron and hole wave functions. At low excitation, non-radiative recombination can play principal cause in the stabilization of the effective lifetime of current carriers. At high excitation, the effective lifetime of current carriers approaches the value in the bulk crystal. The major attention was given to the compensated GaAs doping superlattices with i-layers (n-i-p-i crystals) and to the structures with no i-layers (n-p-n-p structures). The layer thickness of n-, p-, and i-type were 20, 40, or 60 nm and the concentrations of the dopants Te and Zn made up to 10~(18) cm~(-3). Photoluminescence spectra and the decay time of the spontaneous emission intensity in the superlattices were measured at the temperature interval from 11 to 300 K. The influence of α-particle irradiation and thermal annealing on the luminescence spectra and the carrier lifetime was also investigated.
机译:示出了,在掺杂超晶格结构中的发光过程中非QuibiRibrim载流子的寿命随着晶体的激发水平而变化宽范围。两个效果很重要,即(1)载波分布的低维特征和(B)电子和孔波函数重叠的变化。在低励磁下,非辐射重组可以在稳定目前载体的有效寿命的稳定中起主要原因。在高励磁上,电流载体的有效寿命接近散装晶体中的值。用I层(N-I-P-I晶体)和没有I层的结构(N-P-N-P结构)的补偿GaAs掺杂超晶格的主要注意力。 N-,P-和I型层厚度为20,40或60nm,掺杂剂TE和Zn的浓度高达10〜(18)cm〜(-3)。在11至300k的温度间隔下测量超晶片中的自发发射强度的光致发光光谱和衰减时间。还研究了α-颗粒照射和热退火对发光光谱和载体寿命的影响。

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