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Radiative transition in δ-doped GaAs superlattices with and without Al0.1Ga0.9As barriers is investigated by using photoluminescence at low temperatures. The experimental results show that the transition mechanism of δ-doped superlattices is very different from that of ordinary superlattices. Emission intensity of the transition from the electron first excited state to hole states is obviously stronger than that from the electron ground state to hole states due to larger overlap integral between wavefunctions of electrons in the first excited state and hole states. Based on the effective mass theory we have calculated the self-consistent potentials, optical transition matrix elements and photoluminescence spectra for two different samples. By using this model we can explain the main optical characteristics measured. Moreover, after taking into account the bandgap renormalization energy, good agreement between experiment and theory is obtained.  相似文献   
2.
制备了4.2K下电子迁移率达1~2×10~4cm~2/v·sec的MOS反型层,在强磁场下观察到二维电子系统的一系列典型物理现象:SdH振荡及量子霍尔效应.  相似文献   
3.
采用退火后处理的方法,使SiOx∶H(0<x<2)形成纳米硅与二氧化硅的镶嵌结构.利用红外透射谱、Raman谱和光致发光谱,系统地研究了不同退火温度对薄膜微结构及室温光致发光谱的影响.发现发光谱均由两个Gauss线组成,其中主峰随着退火温度的升高而红移,而位于835nm的伴峰不变.指出退火前在720—610nm的波长范围内强的主峰可能来源于膜中的非晶硅原子团,随退火温度的升高主峰的红移是由于非晶硅原子团的长大.而伴峰可能来自硅过剩或氧欠缺引入的某种发光缺陷.1170℃退火后在850nm附近出现强的谱带与纳米硅的析出有关,支持了量子限制效应发光模型.  相似文献   
4.
Considering the dielectric confinement effect on excitonics of PbSe quantum dots (QDs), a correction factor in the wave function was introduced to propose a new band gap calculation model for QDs. The modified model showed great consistency with the experimental data, especially in small size range. According to the variation of confined barrier, the band gap calculation model of PbSe QDs was analyzed in different solvents. The calculating results showed that the modified model was almost solvent-independent, which was consistent with our experimental results and related reports.  相似文献   
5.
A set of a-SiOx :H (0.52 <x<1.58) films are fabricated by plasma-enhanced-chemical-vapor-deposition (PECVD) method at the substrate temperature of 250℃. The microstructure andlocal bonding configurations of the films are investigated in detail using micro-Raman scattering,X-ray photoelectron spectroscopy (XPS) and Fourier transform infrared spectroscopy (FTIR). It isfound that the films are structural inhomogeneous, with five phases of Si, Si2O:H, SiO:H, Si2O3:Hand SiO2 that coexist. The phase of Si is composed of nonhydrogenated amorphous silicon (a-Si)clusters that are spatially isolated. The average size of the clusters decreases with the increasingoxygen concentration x in the films. The results indicate that the structure of the present films canbe described by a multi-shell model, which suggests that a-Si cluster is surrounded in turn by thesubshells of Si2O:H, SiO:H, Si2O3:H, and SiO2.  相似文献   
6.
SiOx∶H(0<x<2)薄膜光致发光的退火行为研究   总被引:2,自引:0,他引:2       下载免费PDF全文
采用退火后处理的方法,使SiOx∶H(0<x<2)形成纳米硅与二氧化硅的镶嵌结构.利用红外透射谱、Raman谱和光致发光谱,系统地研究了不同退火温度对薄膜微结构及室温光致发光谱的影响.发现发光谱均由两个Gauss线组成,其中主峰随着退火温度的升高而红移,而位于835nm的伴峰不变.指出退火前在720—610nm的波长范围内强的主峰可能来源于膜中的非晶硅原子团,随退火温度的升高主峰的红移是由于非晶硅原子团的长大.而伴峰可能来自硅过剩或氧欠缺引入的某种发光缺陷.1170℃退火后在850n 关键词:  相似文献   
7.
采用等离子增强化学气相沉积 (PECVD)技术制备了一组氧含量不同的氢化非晶氧化硅 (a-SiOx∶H)薄膜 ,室温下在 5 5 0~ 90 0nm的波长范围内观察到了两个强的发光带 :一个是由峰位在 6 70nm( 1 85eV)左右的主峰和峰位在 835nm( 1 46eV)的伴峰组成的包络 ,另一个只能在氮气氛中 1 1 70℃退火后的样品中观测到 ,峰位大约在 85 0nm .通过对红外谱和微区Raman谱的分析 ,认为这两个发光带可能分别与存在于薄膜中的a-Si原子团和Si纳米晶粒有关.  相似文献   
8.
氢化非晶硅氧薄膜微结构   总被引:3,自引:0,他引:3       下载免费PDF全文
以Raman散射、X射线电子能谱和红外吸收光谱细致研究了PECVD法250℃衬底温度下制备的氢化非晶硅氧(a-SiOx∶∶H)薄膜的微结构及键构型. 研究表明, 在0.52≤x≤1.58的氧含量范围内,a-SiOx∶∶H薄膜成分和结构不是均一的,依赖于局域键构型氧化程度的不同,大致存在着5种在一定程度上相互分离的结构组分,即Si, Si2O(∶H), SiO(∶H), Si2O3(∶H)和SiO2. 其中的Si相以非氢化的非晶硅(a-Si)颗粒形式存在,随氧含量x的增加其尺度持续减小但始终存在. 提出一种多壳层模型来描述a-SiOx∶H薄膜的结构,认为a-SiOx∶H薄膜中a-Si颗粒依次为Si2O(∶H), SiO(∶H), Si2O3(∶H)和SiO2壳层所包围. 随薄膜氧含量x的增加,各壳层厚度相应变化但各自的化学构成基本保持不变.  相似文献   
9.
考虑了PbSe量子点介电限域效应对激子的影响,引入了修正因子,提出了一种新的量子点禁带宽度的计算模型.与实验数据比较,两者具有良好的一致性.尤其是在小尺寸量子点的情况下,修正后的模型与实验值表现出更好的一致性.通过调整受限势垒的大小,分析不同溶剂条件下PbSe禁带宽度的计算模型,说明采用的修正模型对溶剂的变化是不敏感的,与实验的结论是一致的.  相似文献   
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