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。     

在外电场作用下有限抛物量子阱中类氢杂质态结合能

采用变分方法研究GaAs/AlxGa1-xAs有限抛物量子阱中类氢杂质态能量和结合能随外电场和阱宽的变化关系.在计算中考虑了电子有效带质量和介电常数随空间坐标(或合金组分)的变化因素.结果表明,外电场对类氢杂质态能量和结合能均有明显的影响,并且这些影响随着阱宽的增大而增大.电子有效带质量和介电常数随空间坐标的变化效应使得类氢杂质态基态能量减小,结合能增大,此效应随着阱宽的增大明显变小.     

在外电场作用下有限抛物量子阱中类氢杂质态结合能

采用变分方法研究GaAs/AlxGa1-xAs有限抛物量子阱中类氢杂质态能量和结合能随外电场和阱宽的变化关系.在计算中考虑了电子有效带质量和介电常数随空间坐标(或合金组分)的变化因素.结果表明,外电场对类氢杂质态能量和结合能均有明显的影响,并且这些影响随着阱宽的增大而增大.电子有效带质量和介电常数随空间坐标的变化效应使得类氢杂质态基态能量减小,结合能增大,此效应随着阱宽的增大明显变小.     

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.     

磁场对ZnO抛物量子阱中施主态的影响

ZnO半导体是宽带隙半导体领域继GaAs和GaN之后的研究热点。ZnO对于蓝光、紫光、近紫外波段的光电子器件是一种极具潜力的宽带隙光电子半导体材料。因此,对于ZnO半导体材料构成的抛物量子阱材料物理特性的研究有深远的意义。本文利用变分法研究了在磁场作用下ZnO抛物量子阱中类氢杂质的基态结合能、2p()态能量及1s→2p()跃迁能。结果表明,基态结合能、2p( )态能量以及1s→2p( )跃迁能随磁场单调增加,而2p(-)态能量和1s→2p(-)跃迁能随磁场的变化出现了极小值,然后随磁场的增加线性增加。     

外场对InPBi量子阱中激子结合能的影响

在有效质量近似下运用变分法计算了InAlAs/InPBi/InAlAs量子阱中的激子结合能随阱宽、Al组分、Bi组分的变化情况,分析了外加电场和磁场对激子结合能的影响。结果表明：激子结合能随阱宽增大呈现先增大后减小的趋势;随Al、Bi组分的增大,激子结合能也逐渐增大;外加电场较小时对激子结合能的影响很小,外加电场较大时破坏了激子效应;激子结合能随外加磁场增大呈现单调增大的趋势。计算结果对InAlAs/InPBi/InAlAs量子阱在光电子器件方面的应用有一定指导意义。     

像势对量子阱中类氢杂质Stark效应的影响

在考虑像势影响的情况下，利用变分方法计算了垂直电场下量子阱中类氢杂质的结合能，给出了像势引起的结合能增量随阱宽、杂质位置和电场的变化曲线．结果表明：考虑像势对量子阱中类氢杂质结合能及其Ｓｔａｒｋ效应的影响是很必要的，而且自像势和互像势对类氢杂质结合能Ｓｔａｒｋ效应的影响是相反的．     

压力下屏蔽对有限深量子阱中施主结合能的影响

考虑电子有效质量、材料介电常数及禁带宽度随流体静压力的变化,以及准二维电子气对杂质库仑势的屏蔽影响,利用变分法讨论有限深量子阱中的施主杂质态能级.对GaAs/AlxGa1-xAs量子阱系统中的杂质态结合能进行了数值计算,给出结合能随铝组分、阱宽和压力的变化关系,并讨论了有无屏蔽时的区别.结果表明,屏蔽效应随着压力增加而增加且显著降低杂质态的结合能.     

压力下屏蔽对有限深量子阱中施主结合能的影响

考虑电子有效质量、材料介电常数及禁带宽度随流体静压力的变化,以及准二维电子气对杂质库仑势的屏蔽影响,利用变分法讨论有限深量子阱中的施主杂质态能级.对GaAs/AlxGa1-xAs量子阱系统中的杂质态结合能进行了数值计算,给出结合能随铝组分、阱宽和压力的变化关系,并讨论了有无屏蔽时的区别.结果表明,屏蔽效应随着压力增加而增加且显著降低杂质态的结合能.     

纤锌矿GaN/AlxGa1-xN量子阱中自由极化子能级

采用Lee-Low-Pines (LLP)变分法研究了纤锌矿GaN/Al0.3Ga0.7N量子阱中自由极化子能量和电子-声子相互作用对自由极化子能量的影响.理论计算中考虑了量子阱中定域声子模(Confined phonon modes)和半空间声子模(Half-space phonon modes)的影响以及电子有效质...     

Binding energies of shallow impurities in asymmetric strained wurtzite Al_x Ga_(1-x)N/GaN/AIy Ga1-y N 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.     

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.     

纤锌矿GaN/AlxGa1-xN量子阱中激子能量

考虑了纤锌矿GaN/Al<,x>Ga<,1-x>N量子阱(QW)材料中空穴带质量和光学声子模的各向异性以及声子频率随波矢变化的效应,采用改进的LLP变分法计算了纤锌矿氮化物QW中激子的基态能量和结合能.给出了激子的基态能量和结合能随着QW宽度和Al组分变化的函数关系,并对闪锌矿和纤锌矿GaN/Al<0.3>Ga<,0....     

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.     

In_(0.15)Ga_(0.85)As/GaAs和GaAs/Al_(0.3)Ga_(0.7)As量子阱的静压下光致发光的对照研究

在77K,0—60kbar范围内对在同一衬底上生长的In_(0.15)Ga_(0.85)As/GaAs和GaAs/Al_(0.3)Ga_(0.7)As量子阱的静压下的光致发光进行了对照研究。在GaAs/Al_(0.3)Ga_(0.7)As量子阱中同时观察到导带到轻重空穴子带的跃迁。而在In_(0.15)Ga_(0.85)As/GaAs阱中只观察到导带到重空穴子带的跃迁。与GaAs/Al_(0.3)Ga_(0.7)As的情况相反,In_(0.15)Ga_(0.85)As/GaAs 量子阱的光致发光峰的压力系数随阱宽的减小而增加。在压力大于48kbar时观察到多个与间接跃迁有关的发光峰,对此进行了简短的讨论。     

Influence of strain on hydrogenic impurity states in a GaN/ Al_xGa_(1-x)N quantum dot

Within the effective-mass approximation, we calculated the influence of strain on the binding energy of a hydrogenic donor impurity by a variational approach in a cylindrical wurtzite GaN/AlxGa1-xN strained quantum dot, including the strong built- in electric field effect due to the spontaneous and piezoelectric polarization. The results show that the binding energy of impurity decreases when the strain is considered. Then the built-in electric field becomes bigger with the Al content increasing and the bin...     

AlGaN /GaN分布布拉格反射镜的设计与表征

设计了反射中心波长为500nm的Al0.3Ga0.7N/GaN和AlN/GaN两种分布布拉格反射镜（DBR）,并采用光学传递矩阵方法对其光谱反射率进行了理论上的模拟.采用金属有机物化学气相淀积（MOCVD）技术在蓝宝石衬底上制备了样品.实际测量的样品反射谱中有明显的反射峰,但峰值波长与理论设计有偏差,峰值反射率也比理论设计值偏低.SEM和AFM测量结果表明：这是由生长层厚与设计的偏差和界面不平整引起的.