压力下极化子效应对有限深量子阱中施主结合能的影响

考虑压力及屏蔽效应,同时计入量子阱结构中三类光学声子模(局域类体光学声子、半空间类体光学声子和界面光学声子)的作用,利用改进的LLP中间耦合方法处理电子-声子相互作用,讨论有限深量子阱中极化子效应对杂质态结合能的影响.结果表明,极化子效应使杂质态结合能明显降低,但压力使极化子效应减弱,屏蔽对极化子效应的影响不明显.     

压力下极化子效应对有限深量子阱中施主结合能的影响

考虑压力及屏蔽效应,同时计入量子阱结构中三类光学声子模(局域类体光学声子、半空间类体光学声子和界面光学声子)的作用,利用改进的LLP中间耦合方法处理电子-声子相互作用,讨论有限深量子阱中极化子效应对杂质态结合能的影响.结果表明,极化子效应使杂质态结合能明显降低,但压力使极化子效应减弱,屏蔽对极化子效应的影响不明显.     

纤锌矿氮化物半导体束缚极化子及压力效应

考虑到纤锌矿结构的氮化物半导体材料的单轴异性,采用变分法研究了两支异常光学声子LO-like和TO-like对杂质态结合能的影响,即极化子效应.计及电子有效质量,材料介电常数及晶格振动频率随流体静压力的变化,讨论了束缚极化子结合能的压力效应,数值结果表明,极化子效应使杂质态结合能明显降低,极化子效应的主要贡献来自杂质态与LO-like声子的相互作用.压力使得结合能增加,且增强了结合能的各向异性.     

纤锌矿氮化物半导体束缚极化子及压力效应

考虑到纤锌矿结构的氮化物半导体材料的单轴异性,采用变分法研究了两支异常光学声子LO-like和TO-like对杂质态结合能的影响,即极化子效应.计及电子有效质量,材料介电常数及晶格振动频率随流体静压力的变化,讨论了束缚极化子结合能的压力效应,数值结果表明,极化子效应使杂质态结合能明显降低,极化子效应的主要贡献来自杂质态与LO-like声子的相互作用.压力使得结合能增加,且增强了结合能的各向异性.     

磁场对GaAs/Al_xGa_(1-x)As异质结系统中束缚极化子的影响

对GaAs/AlxGa1-xAs单异质结系统引入三角势近似异质结势,同时考虑体纵光学(LO)声子和有效近似下两支界面光学(IO)声子的影响,采用变分法讨论了外界恒定磁场对束缚于近界面杂质的光学极化子结合能的影响.利用改进的Lee-Low-Pines(LLP)中间耦合方法处理电子-声子和杂质-声子的相互作用,计算了杂质态结合能随杂质位置、磁场强度、电子面密度的变化关系.结果表明,极化子结合能随磁场呈现增加的趋势,其中LO声子对结合能的负贡献受磁场影响显著,而IO声子的负贡献受磁场的影响并不明显,但当杂质靠近界面时,杂质-IO声子相互作用对磁场的影响很敏感.结果还表明,     

磁场对GaAs/AlxGa1-xAs异质结系统中束缚极化子的影响

对GaAs/AlxGa1-xAs单异质结系统引入三角势近似异质结势,同时考虑体纵光学(LO)声子和有效近似下两支界面光学(IO)声子的影响,采用变分法讨论了外界恒定磁场对束缚于近界面杂质的光学极化子结合能的影响.利用改进的Lee-Low-Pines(LLP)中间耦合方法处理电子-声子和杂质-声子的相互作用,计算了杂质态结合能随杂质位置、磁场强度、电子面密度的变化关系.结果表明,极化子结合能随磁场呈现增加的趋势,其中LO声子对结合能的负贡献受磁场影响显著,而IO声子的负贡献受磁场的影响并不明显,但当杂质靠近界面时,杂质-IO声子相互作用对磁场的影响很敏感.结果还表明,导带弯曲作用不容忽略;电子像势对结合能的影响很小,可以忽略.     

电场下应变纤锌矿GaN/AlxGa1-xN异质结中束缚极化子的压力效应

对应变纤锌矿GaN/AlxGa1-xN异质结系统,引入简化相干势近似,利用改进的LLP变换和变分法计算了流体静压力和外场作用下束缚极化子的结合能。考虑由于晶格失配所致的单、双轴应变以及界面光学声子模和半空间光学声子模与电子和杂质之间的相互作用,讨论了结合能随压力、杂质位置和流体静压力的变化关系以及声子对于斯塔克能量移动的影响。数值计算结果表明,高频支界面声子模和类LO半空间声子模对于结合能和斯塔克能移的影响是主要的,且随压力的增加而显著增大,而低频支界面声子模和类TO声子模的作用则很小,且对于杂质位置和流体静压力的变化不敏感。计算还表明,导带的弯曲也不容忽视。     

电子及杂质离子-LO声子耦合对柱形量子线中杂质态的影响

采用有效质量近似和变分方法,同时考虑电子-约束型体纵光学声子(LO)及杂质离子-LO声子耦合,计算了有限深柱形量子线中杂质的极化效应。计算得到杂质结合能及声子贡献随量子线半径的关系。结果表明由电子-LO声子相互作用引发的极化效应的行为与杂质离子-LO声子相互作用引起的屏蔽效应相反,两种效应最终使杂质的结合能降低。     

磁场对氮化物抛物量子阱中束缚极化子的影响

采用改进的Lee-Low-Pines中间耦合方法研究了在外磁场作用下纤锌矿氮化物抛物量子阱中极化子能级,给出不同磁场下极化子基态能量、结合能随阱宽L的变化关系以及能量随磁场强度B变化的函数关系。在计算抛物量子阱材料中考虑了纤锌矿GaN和Al0.3Ga0.7N构成的抛物量子阱中材料中准LO和准TO声子模的各向异性以及外磁场对极化子能量的影响。结果表明:纤锌矿氮化物抛物量子阱材料中电子-声子相互作用和外磁场对极化子能级有明显的影响。极化子基态能量、结合能随阱宽的增加而减小,随磁场的增加而增大,电子-声子相互作用使极化子能量降低,并且GaN/Al0.3Ga0.7N抛物量子阱对极化子的束缚程度比GaAs/Al0.3Ga0.7As抛物量子阱强,因此,在GaN/Al0.3Ga0.7N抛物量子阱中束缚于杂质中心处的电子比在GaAs/Al0.3Ga0.7As抛物量子阱中束缚于杂质中心处的电子稳定。     

抛物量子线中极化子的温度依赖性

研究了抛物量子线中极化子的温度效应.采用改进的线性组合算符法、Lagrange乘子和变分法,在考虑电子与LO声子相互作用情况下,分别研究了抛物量子线中强耦合和弱耦合两种情况下极化子的有效质量和光学声子平均数的温度依赖性.对RbCl晶体和CdTe晶体进行了数值计算,结果表明,两种情况下极化子的有效质量随温度的升高而减少,光学声子平均数均随温度的增高而增大.     

Bound polaron in a strained wurtzite GaN/Aix Ga1-xN cylindrical quantum dot

Within the effective-mass approximation, a variational method is adopted to investigate the polaron effect in a strained GaN/AlxGa1-xN cylindrical quantum dot. The electron couples with both branches of longitudinal optical-like (LO-like) and transverse optical-like (TO-like) phonons and the built-in electric field are taken into account. The numerical results show that the binding energy of the bound polaron is reduced obviously by the polaron effect on the impurity states. Furthermore, the contribution of LO-like phonons to the binding energy is dominant, and the anisotropic angle and Al content influence on the binding energy are small.     

Bound polaron in a strained wurtzite GaN/Al_xGa_(1-x)N cylindrical quantum dot

Within the effective-mass approximation,a variational method is adopted to investigate the polaron effect in a strained GaN/Al_xGa_1-xN cylindrical quantum dot.The electron couples with both branches of longitudinal optical-like（LO-like）and transverse optical-like（TO-like）phonons and the built-in electric field are taken into account.The numerical results show that the binding energy of the bound polaron is reduced obviously by the polaron effect on the impurity states.Furthermore,the contribution of LO-like phonons to the binding energy is dominant,and the anisotropic angle and Al content influence on the binding energy are small.     

非对称应变纤锌矿AlxGa1-xN/GaN/AlyGa1-yN量子阱中浅杂质态的结合能

本文采用变分法数值计算应变纤锌矿AlxGa1−xN/GaN/AlyGa1−yN量子阱中类氢杂质的基态结合能. 计及由自发极化和压电极化引起的内建电场, 讨论阱宽、杂质位置以及左右垒中Al组分对结合能的影响. 结果表明, 尤其在非对称量子阱即势垒宽度或（和）高度不一样的情形下, 杂质位置和垒高对结合能随阱宽变化关系的影响比垒宽更为明显. 对称或非对称结构中, 结合能随杂质位置的变化形如电子基态波函数的空间分布. 此外, 左垒中Al组分对结合能的影响较右垒更甚.     

多层柱形 AlxGa1-xAs/GaAs量子线的一阶声子拉曼散射

We have presented a theoretical calculation of the differential cross section（DCS） for the electron Raman scattering（ERS） process associated with the interface optical（10） and surface optical（SO） phonons in multilayer coaxial cylindrical Al_xGa_1-xAs/GaAs quantum cables（QC）.We consider the Fr（o|¨）hlich electron-phonon interaction in the framework of the dielectric continuum approach.The selection rules for the processes are studied. Singularities are found to be sensitively size-dependent and by varying the size of the QC,it is possible to control the frequency shift in the Raman spectra.A discussion of the phonon behavior for the QC with different size is presented.The numerical results are also compared with those of experiments.     

Sn掺杂对(In0.95-xSnxFe0.05)2O3薄膜的结构、电学及磁特性的影响

我们利用脉冲激光沉积的方法制备了一系列(In0.95-xSnxFe0.05)2O3 (x=0~0.09)薄膜,并在其中发现了室温铁磁性。X射线衍射结果表明锡与铁离子已掺入氧化铟晶格。随着锡的掺入,样品内的载流子浓度得到了很大的提高,但相应的铁磁性却几乎没有变化。我们认为氧空位相关的束缚磁极化子模型能够跟好的解释我们的铁掺杂氧化铟薄膜中的铁磁耦合的机制,而载流子传导的RKKY相互作用则不适用于这一系统。     

ZnO1-xTex and ZnO1-xSx semiconductor alloys as competent materials for opto-electronic and solar cell applications:a comparative analysis

ZnO_1-xTe_x ternary alloys have great potential to work as a photovoltaic (PV) absorber in solar cells. ZnO_1-xS_x is also a ZnO based alloy that have uses in solar cells. In this paper we report the comparative study of various parameters of ZnO_1-xTe_x and ZnO_1-xS_x for selecting it to be a competent material for solar cell applications. The parameters are mainly being calculated using the well-known VCA (virtual crystal approximation) and VBAC (Valence Band Anti-Crossing) model. It was certainly being analysed that the incorporation of Te atoms produces a high band gap lower than S atoms in the host ZnO material. The spin-orbit splitting energy value of ZnO_1-xTe_x was found to be higher than that of ZnO_1-xS_x. Beside this, the strain effects are also higher in ZnO_1-xTe_x than ZnO_1-xS_x. The remarkable notifying result which the paper is reporting is that at a higher percentage of Te atoms in ZnO_1-xTe_x, the spin-orbit splitting energy value rises above the band gap value, which signifies a very less internal carrier recombination that decreases the leakage current and increases the efficiency of the solar cell. Moreover, it also covers a wide wavelength range compared to ZnO_1-xS_x.     

Characterization of AlxInyGa1−x−yN quaternary alloys grown on sapphire substrates by molecular-beam epitaxy

High-resolution X-ray diffraction (HR-XRD) with rocking curve, atomic force microscopy (AFM) and photoluminescence (PL) spectroscopy have been performed on high-quality quaternary Al_xIn_yGa_1−x−yN thin films at room temperature. The Al_xIn_yGa_1−x−yN films were grown on c-plane (0 0 0 1) sapphire substrates with AlN as buffer layers using a molecular beam epitaxy (MBE) technique with aluminum (Al) mole fractions x ranging from 0.0 to 0.2 and constant indium (In) mole fraction y=0.1. HR-XRD measurements confirmed the high crystalline quality of these alloys without any phase separation. The X-ray rocking curve of Al_xIn_yGa_1−x−yN films typically shows full widths at half maximum (FWHM) intensity between 14.4 and 28.8 arcmin. AFM measurements revealed a two-dimensional (2D) growth mode with a smooth surface morphology of quaternary epilayers. PL spectra exhibited both an enhancement of the integrated intensity and an increasing blueshift with increased Al content with reference to the ternary sample In_0.1Ga_0.90N. Both effects arise from Al-enhanced exciton localization. PL was used to determine the behavior of the energy band gap of the quaternary films, which was found to increase with increasing Al composition from 0.05 to 0.2. This trend is expected since the incorporation of Al increases the energy band gap of ternary In_0.1Ga_0.90N (3.004 eV). We have also investigated the bowing parameter for the variation of energy band gaps and found it to be very sensitive on the Al composition. A value of b=10.4 has been obtained for our quaternary Al_xIn_yGa_1−x−yN alloys.     

The effect of single-phonon and plasmon recombination on the lifetime in n-Hg1−xCdxTe with magnetically tuned bandgap

Theoretical investigations have predicted a great enhancement of electron-hole recombinations by adjusting the bandgap of narrow-gap semiconductors to the energy of elementary excitation in solids such as phonons or plasmons. Such an enhancement of the recombination rate of excess carriers is very important in constructing far-I.R. devices and might be used to generate high densities of LO-phonons and plasmons. We report experimental evidence of the influence of these recombination channels on the photoconductivity and the excess carrier lifetime in semimetallic n-Hg_1−xCd_xTe alloys, whose induced bandgap is magnetically tuned through the relevant energies of the elementary excitations. Both from a comparison of theoretically estimated lifetimes with Auger lifetimes and from experimental observations the new recombination channels prove to be very efficient and dominate the behaviour near their resonance with the band-gap.     

AlxGa1-xAs量子线中的浅杂质态的研究

利用变分方法研究柱型量子线中浅杂质态的极化效应。给出AlxGa1-xAs柱型量子线中浅杂质态的结合能随组份x,杂质位置的变化关系。结果表明电子-声子相互作用明显降低了杂质态的结合能,且结合能随组份x的增加而增加。