(AlxGa1-x)0.51In0.49P(x=0.29)PL谱的温度反常现象

对与ＧａＡｓ晶格匹配的四元合金（ＡｌｘＧａ１－ｘ）０．５１Ｉ０．４９Ｐ（ｘ＝０．２９）作了变曙和变激发功率密度的ＰＬ谱研究,发现了ＰＬ谱峰值位置不随激发功率密度的变化而移动,但是出现了随温度变化的反常行为。从１９Ｋ开始温,ＰＬ谱峰先向红端移动,到５５Ｋ左右开始出现蓝移,在８４Ｋ左右蓝移达到最大,而后随着温度的继续升高,ＰＬ谱峰再次工端移动。整个过程与温度呈Ｚ－型关系,而不是通常半导体样品所表现的线     

1MeVSi~＋衬底加温注入Al＿（0．3）Ga＿（0．7）As／GaAs超晶格和GaAs的晶格损伤研究

用卢瑟福背散射／沟道技术研究了１ＭｅＶＳｉ￣＋在衬底加温和室温下以不同剂量注入Ａｌ＿（０．３）Ｇ＿（０．７）Ａｓ／ＧａＡｓ超晶格和ＧａＡｓ后的晶格损伤。在衬底加温下，观察到Ａｌ＿（０．３）Ｇａ＿（０．７）Ａｓ／ＧａＡｓ超晶格和ＧａＡｓ都存在一个动态退火速率与缺陷产生速率相平衡的剂量范围，以及两种速率失去平衡的临界剂量。超晶格比ＧａＡｓ更难以损伤，并且它的两种速率失去平衡的临界剂量也大于ＧａＡｓ中的相应临界剂量，用热尖峰与碰撞模型解释了晶格损伤积累与注入剂量和衬底温度的关系。用ＣＮＤＯ／２量子化学方法计算了ＧａＡｓ和Ａｌ＿ｘＧａ＿（１－ｘ）Ａｓ中化学键的相对强度，并根据计算结果解释了注入过程中Ａｌ＿（０．３）Ｇａ＿（０．７）Ａｓ／ＧａＡｓ超晶格和ＧａＡｓ中晶格损伤程度的差别。     

退火及铟含量对InGaAs量子点光学特性的影响

研究了退火条件和 Ｉｎ 组份对分子束外延生长的 Ｉｎ Ｇａ Ａｓ 量子点（分别以 Ｇａ Ａｓ或 Ａｌ Ｇａ Ａｓ 为基体）光学特性的影响。表明：量子点中 Ｉｎ 含量的增加将导致载流子的定域能增加和基态与激发态之间的能量间隔增大。采用垂直耦合的量子点及宽能带的 Ａｌ Ｇａ Ａｓ 基体可增强材料的热稳定性。以 Ａｌ Ｇａ Ａｓ 为基体的 Ｉｎ Ｇａ Ａｓ 量子点,高温后退火工艺 （ Ｔ＝ ８３０℃）可改善低温生长的 Ａｌ Ｇａ Ａｓ 层的质量,从而改善量子点激光器材料的质量。     

Ga1—xAlxAs外延片有源区Al组份的测定方法

由于ＧａＡｓ与ＡｌＡｓ晶格常数相近，ＧａＡｓ晶格常数为０．５６５３５ｎｍ，ＡｌＡｓ的晶格常数为０．５６６０５ｎｍ，当固熔体中Ａｌ组份ｘ值从０变到１时，晶格常数变化约为０．１５％．因此，在ＧａＡｓ衬底上生长Ｇａ１－ｘＡｌｘＡｓ时，在界面处的失配位错少，...     

δ掺杂的赝形高电子迁移率晶体管AlGaAs／InGaAs／GaAs结构中的费密…

报道δ掺杂赝形高电子迁移率晶体管结构Ａｌ０．３０Ｇａ０．７０Ａｓ／Ｉｎ０．１５Ｇａ０．８５Ａｓ／ＧａＡｓ的光致发光光谱研究的实验结果，除了观察到ｎ＝１电子子带到ｍ＝１重空穴子带，ｎ＝２电子子带到ｎ＝１重空穴子带间的强发光峰，还观察到了ｎ＝１电子子带到ｎ＝１轻空穴子带的弱发光峰，通过变化掺杂浓度来改变费密能级的位置，在这种δ掺杂的ＨＥＭＴｓ的系统中观察了费密边奇异性，并把它归结为费密海与费密边附近未     

AlGaN薄膜的微区Raman散射光谱研究

利用微区Ｒａｍａｎ散射技术,对低压ＭＯＣＶＤ生长的不同Ａｌ组分的ＡｌｘＧａ１－ｘＮ薄膜（ｘ＝０,０．０７,０．１５）进行了背散射Ｚ（Ｘ,Ｘ）Ｚ－几何配制下的测量．Ａ１（ＬＯ）模式的声子频移随Ａｌ组分的变化关系为：ω（ＡｌｘＧａ１－ｘＮ）＝（１＋０．２２０ｘ）ω（ＧａＮ）．观察到了Ａ１（ＬＯ）模式由于空间相关效应引起的展宽．Ｅ２模式随Ａｌ组分的的增大产生的移动很微小,但趋于展宽．这被认为是Ｅ２模式的声子频移随Ａｌ组分的增加而增大与其受到的张应力导致的声子频移随Ａｌ组分的增加而减小共同作用的结果．在多种配置下,观察到了Ａｌ０．０７Ｇａ０．９３Ｎ薄膜的Ａ１（ＴＯ）模式、Ａ１（ＬＯ）模式、Ｅ１（ＴＯ）模式和Ｅ２模式．验证了ＡｌｘＧａ１－ｘＮ薄膜的Ｒａｍａｎ选择定则．表明ＡｌｘＧａ１－ｘＮ薄膜具有单模行为．     

后退火对InxGa1xAs 单层量子点光学性质的影响

 研究了以GaAs和Al_0.15Ga_0.85As为基体, 当铟的摩尔分数（x）不同时, 后退火对InxGa1-xAs 单层量子点光致荧光（PL）谱特性的影响。后退火将导致铟含量不同的样品（x=0.23, 0.37, 0.50, 1.0）的PL谱线宽度变窄和蓝移。对于GaAs 基体, 在700℃退火90分钟所造成的PL谱蓝移与退火30分钟相似;(仅当x=0.23时, 退火90分钟所造成的PL谱蓝移小于30分钟)。对于Al0.15Ga0.85As基体, 在700℃退 火30分钟和90分钟, 其PL谱蓝移是不同的。     

J/Ψ衰变中的∧,∧γ和∧π~0产生

利用北京正负电子对撞机（ＢＥＰＣ）上的北京谱仪（ＢＥＳ）收集的７．８×１０６个Ｊ／事例，测量得到Ｊ／－Ａ，ＡＡｖ和八八三个衰变道的分支比分别为Ｂｒ（Ｊ／一Ａ八）：（ｌ．０８：：０．０６：：０．２４）ｘ１０－ａ，（ＶＡＡＮ＜ｌ．６ｘｌ０－‘（９０％Ｃｕ，和＆（Ｕ’）＝（２３ｌ０．７ｌｌ０．８）ｌ１０－ｔ：第一个衰变道的角分布为：（１、ａｃｏｓ‘０），ａ＝０．５２０．３３０．１３。     

快速热退火引起的GaAs／AlGaAs双量子阱中铝原子的扩散研究

用分子束外延生长了ＧａＡｓ／ＡｌＧａＡｓ双量子阱激光器结构样品，并对不同温度快速热退火导致量子阱组分无序即阱和垒中三族元素的扩散过程进行了实验和理论研究 。用光荧光技术测量退火样品的ｎ＝１量子阱能级跃迁峰值位置，结果表明退火前后样品量子阱能级位置发生蓝移，蓝移量随温度的提高而增大，对退火过程中ＧａＡｓ／ＡｌＧａＡｓ量子阱中三族元素的扩散过程中进行了理论分析，并与实验结果相比较，获得了不同退火温度下     

混晶GaAs_（1－x）P_x∶N中N_x发光的声子伴线结构

本文采用荧光窄化技术，对低组分的ＧａＡｓ（１－ｘ）Ｐｘ∶Ｎ（ｘ＝０．７６，０．６５）混晶材料中Ｎｘ束缚激子的声子伴线进行了研究．在低温下，选择激发Ｎｘ带时，我们得到了与ＧａＰ∶Ｎ低温发光谱中类似的声子伴线结构．根据实验结果，给出了混晶中各种声子的能量．另外，对组分为ｘ＝０．７６的ＧａＡｓ（１－ｘ）Ｐｘ∶Ｎ混晶样品，我们还首次观察并分析了多声子重现光谱．     

Effect of In_x Ga_(1-x )N “continuously graded” buffer layer on InGaN epilayer grown by metalorganic chemical vapor deposition

In this paper we report on the effect of an In x Ga1-x N continuously graded buffer layer on an InGaN epilayer grown on a GaN template.In our experiment,three types of buffer layers including constant composition,continuously graded composition,and the combination of constant and continuously graded composition are used.Surface morphologies,crystalline quality,indium incorporations,and relaxation degrees of InGaN epilayers with different buffer layers are investigated.It is found that the In x Ga1-x N continuously graded buffer layer is effective to improve the surface morphology,crystalline quality,and the indium incorporation of the InGaN epilayer.These superior characteristics of the continuously graded buffer layer can be attributed to the sufficient strain release and the reduction of dislocations.     

Defect-induced magnetic structure in (Ga(1)-(x)Mn(x))As

We show that magnetic structures involving partial disorder of local magnetic moments on the Mn atoms in (Ga(1)-(x)Mn(x))As lower the total energy, compared to the case of perfect ferromagnetic ordering, when As defects on the Ga sublattice are present. Such magnetic structures are found to be stable for a range of concentrations of As antisites, and this result accounts for the observed magnetic moments and critical temperatures in (Ga(1)-(x)Mn(x))As. We propose an explanation for the stabilization of the partially disordered magnetic structures and conclude that the magnetization and critical temperatures should increase substantially by reducing the number of As antisite defects.     

Origin of the tunnel anisotropic magnetoresistance in Ga(1-x)Mn(x)As/ZnSe/Ga(1-x)Mn(x)As magnetic tunnel junctions of II-VI/III-V heterostructures

We investigated spin-dependent transport in magnetic tunnel junctions made of III-V Ga(1-x)Mn(x)As electrodes and II-VI ZnSe tunnel barriers. The high tunnel magnetoresistance (TMR) ratio up to 100% we observed indicates high spin polarization at the barrier/electrodes interfaces. We found anisotropic tunneling conductance having a magnitude of 10% with respect to the direction of magnetization to linearly depend on the magnetic anisotropy energy of Ga(1-x)Mn(x)As. This proves that the spin-orbit interactions in the valence band of Ga(1-x)M(x)As are responsible for the tunnel anisotropic magnetoresistance (TAMR) effect.     

Resonant tunneling in double barrier structures with GaAs and (InGa)As quantum wells

Resonant tunneling through an (AlGa)As/In_XGa_1−XAs/(AlGa)As double barrier structure has been observed. Three crystals with indium concentration x=0, x=0.08 and x=0.13 were grown. For x=0, GaAs wells, we investigated the variation in resonance voltage, i.e. voltage at peak current, between different diodes across a wafer. The resonance voltage exhibited a skew distribution which is interpreted as an effect of lateral alloy variation in the active layers and differences in contact resistance. For (InGa)Asv quantum wells we found a negative differential resistance at 77 K with a peak-to-valley ratio as large as 3:1. The resonance voltage decreased as the indium concentration x was increased. This is an effect of the position of the ground state which is lowered (due to smaller bandgap) compared to the Fermi level. At x=0.13 the ground state was found to be below the conduction band edge of the GaAs contact regions and therefore the ground state resonance was absent.     

Spacer layer thickness fluctuation scattering in a modulation-doped Al_xGa_1-xAs/GaAs/Al_xGa_1-xAs quantum well

We theoretically study the influence of spacer layer thickness fluctuation(SLTF) on the mobility of a twodimensional electron gas(2DEG) in the modulation-doped Al x Ga 1 x As/GaAs/Al x Ga 1 x As quantum well.The dependence of the mobility limited by SLTF scattering on spacer layer thickness and donor density are obtained.The results show that SLTF scattering is an important scattering mechanism for the quantum well structure with a thick well layer.     

Structural and optical properties of CdS/Cu(In,Ga)Se<Subscript>2</Subscript> heterostructures irradiated by high-energy electrons*

Thin films of Cu(In, Ga)Se₂ (CIGS) with a Ga/(Ga + In) ratio of ~0.27 corresponding to the standard elemental composition for solar-energy transducers were grown on Mo-coated glass substrates by the Cu, In, Ga, and Se co-evaporation technique from different sources. Transmission (T), photoluminescence (PL), and photoluminescence excitation (PLE) spectra at 4.2 K were used to analyze electronic properties in the asgrown and electron-irradiated CIGS films. The band-gap energy (E_g) of the CIGS films measured using both transmission and PLE methods was found to be about 1.28 eV at 4.2 K. Two deep bands in the PL spectra of the irradiated CIGS films, P₁ at ~0.91 eV and P₂ at ~0.77 eV, have been detected. These bands are tentatively associated with copper atoms substituting indium (Cu_In) and indium vacancies V_In, respectively, as the simplest radiation-induced defects.     

Effects of confined longitudinal and interface optical phonons on excitons in an asymmetric quantum well

The interaction between exciton and confined longitudinal optical (LO) phonons, interface optical (IO) phonons in an asymmetric Ga 1 x Al x As/GaAs/Ga 0.7 Al 0.3 As square quantum well is investigated. By applying the LLP-like transformation and variational approach, the numerical results are obtained as functions of the well width and asymmetric-degree of well. The exciton-optical phonons interaction-energy has a minimum value with the increase of the well width. It is demonstrated that the LO-phonon energ...     

I型锗基笼合物Ba8Ga16-xSbxGe30的合成及热电性能

用高温熔融结合放电等离子烧结（SPS）方法合成了Sb掺杂的单相n型Ba8Ga16-xSbxGe30化合物，探索了Sb对Ga的取代对其热电性能的影响规律．研究结果表明：随着Sb取代分数x的增加，Seebeck系数逐渐降低，Seebeck系数峰值对应的温度向低温方向偏移．电导率随着x的增加先增大后减小，当x=2时达到最大值．Sb取代Ga后对化合物的热性能有较大影响，其热导率和晶格热导率都有不同程度的降低．在所有n型Ba8Ga16-xSbxGe30化合物中，Ba8Ga14Sb2Ge30化合物的ZT值最大，在950K左右其最大ZY值达1．1．     

Optimization of a solar-blind and middle infrared two-colour photodetector using GaN-based bulk material and quantum wells

This paper calculates the wavelengths of the interband transitions as a function of the Al mole fraction of Al_xGa_1-xN bulk material. It is finds that when the Al mole fraction is between 0.456 and 0.639, the wavelengths correspond to the solar-blind (250~nm to 280~nm). The influence of the structure parameters of Al_yGa_1-yN/GaN quantum wells on the wavelength and absorption coefficient of intersubband transitions has been investigated by solving the Schr?dinger and Poisson equations self-consistently. The Al mole fraction of the Al_yGa_1-yN barrier changes from 0.30 to 0.46, meanwhile the width of the well changes from 2.9~nm to 2.2~nm, for maximal intersubband absorption in the window of the air (3~μm <λ <5~μm). The absorption coefficient of the intersubband transition between the ground state and the first excited state decreases with the increase of the wavelength. The results are finally used to discuss the prospects of GaN-based bulk material and quantum wells for a solar-blind and middle infrared two-colour photodetector.