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首页> 外文期刊>Journal of Applied Physics >Band structure and absorption properties of (Ga, In)/(P, As, N) symmetric and asymmetric quantum wells and super-lattice structures: Towards lattice-matched Ⅲ-Ⅴ/Si tandem
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Band structure and absorption properties of (Ga, In)/(P, As, N) symmetric and asymmetric quantum wells and super-lattice structures: Towards lattice-matched Ⅲ-Ⅴ/Si tandem

机译:(Ga,In)/(P,As,N)对称和不对称量子阱和超晶格结构的能带结构和吸收特性:朝向晶格匹配的Ⅲ-Ⅴ/ Si串联

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摘要

Quaternary dilute nitride compound semiconductors like GaAsyP1-x-yNx and Ga1-zInzP1-xNx are lattice matched with silicon when y = 4.7*x - 0.1 and z = 2.2*x - 0.044 and also have direct bandgaps (with N 0.6%), thus allowing for monolithic integration of III-V optoelectronics with silicon technology as well as III-V/Si tandem junction solar cells. By applying an eight-band k.p strained (tensile or compressive) Hamiltonian and a Band Anti-crossing model (to account for small amounts of nitrogen impurities) to the conduction band, the electronic band structure and the dispersion relation of these alloys can be determined near the center of Brillouin Zone. In this work, by minimizing the total mechanical energy of the stack of alternating layers of GaP1-xNx and GaAs1-xNx, we have evaluated the ratio of thickness of the respective layers for a strainbalanced superlattice GaAs1-xNx/GaP1-xNx structure on silicon. We calculated the confinement energies and the corresponding states of the respective carriers inside a quantum well (with and without resonantly coupled) or in the miniband of a superlattice structure as a function of the nitrogen composition using a transfer matrix approach under the envelope function approximation. Incorporating only a small amount of nitrogen (5%), the bandgap of these lattice matched structures fulfils the optimum bandgap requirement of (1.65-1.8) eV for III-V/Si tandem solar cells and optoelectronic devices. The optical-absorption coefficient, in both symmetric and asymmetric quantum wells, is then evaluated with respect to nitrogen composition and temperature by using the Fermi-golden rule for both TE and TM polarization of incident light, including the effect of excitons and thermal broadening. Published by AIP Publishing.
机译:当y = 4.7 * x-0.1和z = 2.2 * x-0.044时,诸如GaAsyP1-x-yNx和Ga1-zInzP1-xNx的四元稀氮化物化合物半导体与硅晶格匹配,并且具有直接带隙(N> 0.6%) ,因此可以将III-V光电与硅技术以及III-V / Si串联结太阳能电池进行单片集成。通过对导带应用八能带kp应变(拉伸或压缩)哈密顿量和能带反交叉模型(考虑到少量氮杂质),可以确定这些合金的电子能带结构和色散关系在布里渊区的中心附近。在这项工作中,通过最小化GaP1-xNx和GaAs1-xNx交替层堆叠的总机械能,我们评估了硅上应变平衡超晶格GaAs1-xNx / GaP1-xNx结构的各层的厚度比。我们使用包络函数近似下的转移矩阵方法计算了量子阱内部(具有和不具有共振耦合的)或超晶格结构的微带中的约束能和相应载流子的状态,作为氮组成的函数。这些晶格匹配结构的带隙仅掺入少量氮(<5%),即可满足III-V / Si串联太阳能电池和光电器件的最佳带隙要求(1.65-1.8)eV。然后,通过对入射光的TE和TM偏振(包括激子和热展宽的影响)使用费米-黄金法则,对对称和不对称量子阱中的光吸收系数进行氮含量和温度方面的评估。由AIP Publishing发布。

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  • 来源
    《Journal of Applied Physics》 |2018年第9期|095104.1-095104.12|共12页
  • 作者

    Kharel K.; Freundlich A.;

  • 作者单位

    Univ Houston, Phys Dept, Houston, TX 77204 USA;

    Univ Houston, Phys Dept, Houston, TX 77204 USA;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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