GaAs/Ga1-xAlxAs量子阱线中类氢杂质的束缚能和光致电离截面

通过在波函数中考虑量子线的限制方向和非限制方向的相关性,计算了GaAs/Ga1-xAlxAs量子阱线中类氢杂质的束缚能和光致电离截面.结果表明光致电离截面的大小受量子线尺寸的影响,并且对于相同尺寸的量子线,有限深势阱中杂质态的光致电离截面要比无限深势阱中的大.与他人的结果比较发现,所选波函数改进了体系的束缚能,并使光致电离截面减小,这使得结果更为合理.     

GaInAsP /InP阶梯量子阱中氢施主杂质束缚能

在有效质量近似下,利用变分法对GaxIn1-xAsyP1-y /InP阶梯量子阱中氢施主杂质束缚能进行了理论计算,并研究了外加电场和阶梯阱的高度对阶梯量子阱中氢施主杂质电子态特性的影响。计算结果显示当施主杂质位于阶梯量子阱的中心时,束缚能达到最大值;外加电场使得电子波函数从阱中心偏移,引起束缚能的非对称分布;Ga 与 As组分的变化使得阶梯阱的势能高度发生变化,从而明显的影响阱中氢杂质束缚能。计算结果对一些基于半导体阶梯型量子阱的光电子器件的设计制作有一定的指导意义。     

半导体量子阱和量子线中杂质束缚能的度规法则与维里定理

利用变分法计算了矩形量子线和量子阱中类氢杂质束缚能的度规法则和维里定理值.计算结果表明:的确存在一个参数(杂质有效玻尔半径)可用来完全确定束缚能的值,而不必考虑截面的形状和尺寸;体系的维里定理值并不等于常数,而是随杂质有效玻尔半径变化,在阱宽较小和较大时,维里定理值都趋于2.     

半导体量子阱和量子线中杂质束缚能的度规法则与维里定理

利用变分法计算了矩形量子线和量子阱中类氢杂质束缚能的度规法则和维里定理值.计算结果表明:的确存在一个参数(杂质有效玻尔半径)可用来完全确定束缚能的值,而不必考虑截面的形状和尺寸;体系的维里定理值并不等于常数,而是随杂质有效玻尔半径变化,在阱宽较小和较大时,维里定理值都趋于2.     

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。     

量子点异质结中类氢杂质电子束缚能级的计算

采用球壳结构和渐变有限深谐振子势阱模型,利用镜像电荷的方法分析了不同介电常数下,界面效应对半导体量子点异质结中类氢杂质电子束缚能级的扰动情况.通过计算考虑到杂质对电子的束缚作用前后的电子的基态能,可以看出对于处在弱受限情况下的量子点,异质结厚度在小于10 nm时,界面效应对类氢杂质电子束缚能级的影响明显.当异质结壳层厚度增大的时候,界面效应的影响将逐渐减弱,受扰动的基态能也逐渐减小,最后不同Airy函数零点值所对应的基态能趋向于某一固定值,此时界面效应可以忽略.     

外加电场对GaN/AlxGa1-xN双量子阱中性施主束缚能的影响

在有效质量包络函数理论下,利用变分法计算了未加电场以及加入电场后 双量子阱中施主杂质各种情况下的束缚能,讨论了双量子阱中间势垒高度、施主杂质位置对杂质束缚能的影响。给出了加入电场后施主位置不同时的束缚能和波函数,以及量子阱宽度不同时的束缚能,并且计算了未加电场和加入电场后中间势垒高度变化以及宽度不同时的束缚能。当双量子阱中间垒宽一定时,束缚能随着阱宽的变化会出现一个峰值。在阱宽一定时,随着中间垒宽度的增加,束缚能逐渐减小,并在垒宽增加到一定宽度时双量子阱情况与单量子阱情况相似,束缚能不再明显变化。计算结果对设计和研究 量子阱发光和探测器件有一定的参考价值。     

MBE自组织方法生长InGaAs/AlGaAs量子线FET材料

利用分子束外延 (MBE)技术在高指数面 Ga As衬底上自组织生长了应变 In Ga As/Ga As量子线材料。原子力显微镜 (AFM)观测结果表明量子线的密度高达 4× 1 0 5/cm。低温偏振光致发光谱 (PPL)研究发现其发光峰半高宽 (FWHM)最小为 9.2 me V,最大偏振度可达 0 .2 2。以 Al Ga As为垫垒 ,In Ga As/Ga As量子线为沟道 ,成功制备了量子线场效应管 (QWR-FET)结构材料 ,并试制了器件 ,获得了较好的器件结果     

在深量子阱中的库仑杂质态

对处于深量子阱中的库仑杂质态进行了变分计算,给出了基态束缚能作为量子阱厚度和杂质中心位置的函数.计算结果与Bastard的结果作了详细的比较.     

表面势垒层厚度对量子阱束缚电子态的影响

采用包络函数方法在四带k·p模型基础上计算了晶格匹配的量子阱 InP/Ca_(0.47)In_(0.53)As/InP中束缚电子能级及波函数,讨论了表面势垒层厚度对量子阱中束缚电子能级、波函数以及相应于电子基态能级与重空穴基态能级间的荧光谱峰位置的影响.文中也讨论了在势阱与势垒边界处的不同衔接条件对量子阱中束缚电子能级计算结果的影响.     

在磁场作用下氮化物抛物量子阱中杂质态能量

采用变分法研究了在外磁场作用下GaN／AlxGa1-xN无限抛物量子阱（PQW）中类氢杂质态能级,给出不同磁场下杂质态基态能、结合能随阱宽的变化关系以及能量随磁场强度变化的函数关系。数值结果表明：外磁场对类氢杂质能量和结合能均有明显的影响,杂质态能量随磁场的增强而显著增大,并且随阱宽的增大而增大;GaN／Al0.3Ga0.7 N PQW对杂质态的束缚程度比GaAs／Al0.3Ga0.7As PQW强。     

Binding energies of shallow impurities in asymmetric strained wurtzite AlxGa1-xN/ GaN/Aly Ga1-yN quantum wells

The ground state binding energies of hydrogenic impurities in strained wurtzite AlxGa1-xN/GaN/AlyGa1-y>N quantum wells are calculated numerically by a variational method. The de-pendence of the binding energy on well width, impurity location and Al concentrations of the left and right barriers is discussed, including the effect of the built-in electric field induced by spontaneous and piezoelectric polarizations. The results show that the change in binding energy with well width is more sensitive to the impurity position and barrier heights than the barrier widths, especially in asymmetric well structures where the barrier widths and/or barrier heights differ. The binding energy as a function of the impurity position in symmetric and asymmetric structures behaves like a map of the spatial distribution of the ground state wave function of the electron. It is also found that the influence on the binding energy from the Al concentration of the left barrier is more obvious than that of the right barrier.     

Binding energies of shallow impurities in asymmetric strained wurtzite AlxGa1-xN/GaN/AlyGa1-yN quantum wells

The ground state binding energies of hydrogenic impurities in strained wurtzite Al_xGa_1-xN/GaN/Al_yGa_1-yN quantum wells are calculated numerically by a variational method. The dependence of the binding energy on well width, impurity location and Al concentrations of the left and right barriers is discussed, including the effect of the built-in electric field induced by spontaneous and piezoelectric polarizations. The results show that the change in binding energy with well width is more sensitive to the impurity position and barrier heights than the barrier widths, especially in asymmetric well structures where the barrier widths and/or barrier heights differ. The binding energy as a function of the impurity position in symmetric and asymmetric structures behaves like a map of the spatial distribution of the ground state wave function of the electron. It is also found that the influence on the binding energy from the Al concentration of the left barrier is more obvious than that of the right barrier.     

Effect of a magnetic field on the energy levels of donor impurities in the ZnO parabolic quantum well

Energy levels of a donor impurity in the ZnO parabolic quantum well under the magnetic field are investigated using the variational method.The binding energy of the ground state,the energies of 2p±state and 1 s→2p±transition energies of a hydrogenic donor in the ZnO parabolic quantum well are numerically calculated as a function of the strength of magnetic field for different parabolic potential fields.The results show that the external magnetic field has an obvious influence on the binding energies and the 1 s→2p±transition energies of a hydrogenic donor.The Is to 2p±transition energy increases linearly with the strength of magnetic field,but the Is to 2p_ transition energy decreases when the strength of magnetic field increases for the small field strength. Compared to the GaAs parabolic well,the donors are more tightly bound to the ZnO parabolic well and the influence of external magnetic field on the binding energy of a donor is much stronger in the ZnO parabolic well.     

Effects of electron-and impurity-ion-LO phonon couples on the impurity states in cylindrical quantum wires

The variational method and the effective mass approximation are used to calculate the phonon effects on the hydrogenic impurity states in a cylindrical quantum wire with finite deep potential by taking both the couplings of the electron-confined bulk longitudinal optical（LO） phonons and the impurity-ion-LO phonons into account.The binding energies and the phonon contributions are calculated as functions of the transverse dimension of the quantum wire.The results show that the polaronic effect induced by the electron-LO phonon coupling and the screening effect induced by the impurity-ion-LO phonon coupling tend to compensate each other and the total effects reduce the impurity binding energies.     

Effects of electron- and impurity-ion-LO phonon couples on the impurity states in cylindrical quantum wires

The variational method and the effective mass approximation are used to calculate the phonon effects on the hydrogenic impurity states in a cylindrical quantum wire with finite deep potential by taking both the couplings of the electron-confined bulk longitudinal optical (LO) phonons and the impurity-ion-LO phonons into account.The binding energies and the phonon contributions are calculated as functions of the transverse dimension of the quantum wire. The results show that the polaronic effect induced by the electron-LO phonon coupling and the screening effect induced by the impurity-ion-LO phonon coupling tend to compensate each other and the total effects reduce the impurity binding energies.