高功率线性梯度折射率GaAs/AlGaAs单量子阱激光器

应用MOVPE研制出梯度折射率分别限GaAs/AlGaAs单量子阱激光器，室温单面连续输出光功率超过500mW,激射波长为820.3nm,并讨论了注入电流和温度改变对波长的影响。     

InGaAsP/InGaP/GaAs单量子阱激光器工作特性

利用低压-金属有机化学汽相沉积(LP-MOCVD)方法研制出InGaAsP/InGaP/GaAs单量子阱大功率激光器并分析了阈值电流密度、特征温度和外微分量子效率与腔长的关系.     

GaAs/AlGaAs量子点阵的制备及其荧光特性

采用电子束曝光和反应离子刻蚀的工艺,将GaAs/AlGaAs量子阱外延材料制成量子点阵,其光荧光谱显示出蓝移,并且蓝移量随着量子点直径尺寸的减少而增大。     

InGaAs/GaAs/InGaP量子阱激光器的温度电压特性

研究了InGaAs/GaAs/InGaP量子阱激光器在不同温度下的电流-电压特性,并建立了一个理论模型进行描述。实验所用激光器腔长为0.3 mm,脊条宽度为3μm。实验测量得到该激光器在15～100 K的电压温度系数(dV/dT)为7.87～8.32 mV/K,在100～300 K的电压温度系数为2.93～3.17 mV/K。由理论模型计算得到该激光器在15～100 K的电压温度系数为2.56～2.75 mV/K,在100～300 K的电压温度系数为3.91～4.15 mV/K。在100～300 K,实验测量与理论模型计算得出的电压温度系数接近,理论模型能较好地模拟激光器的温度电压特性;但在15～100 K相差较大,还需要进一步完善。     

高功率半导体量子阱激光器测试中的突变性损伤

在使用综合参数测试仪测试808nm发射的半导体量子阱激光器的过程中，出现了一种由电浪涌所导致的灾变性损伤。通过测试的功率曲线和伏安特性曲线，断定激光器出现了突变性的损伤，同时测试的发射光谱不再是激射光谱，而是由自发辐射所产生的荧光光谱。由扫描电镜（SEM）观察到了激光器的腔面膜出现了熔化，证实激光器的确发生了灾变性损伤。作为对比，我们引用了另一种在测试中发现的快速退化现象，对两种退化出现的原因进行了理论上的分析，了解到激光器的退化主要还是由器件本身的材料、结构以及后期的工艺过程所决定的，在测试器件过程中电浪涌不只不过会加速或产生突然灾变性退化。通过测试我们建立了一种比较简单的检验一个激光器质量可靠性的方法，所以理解由电浪涌所引起的退化行为是非常重要的。     

量子阱级联激光器

介绍了一种新型的工作于４．２５μｍ的半导体激光器－量子阱级联激光器，这种新型激光器是单极性的，它发光仅依赖于电子而并非正负两种电荷，介绍了这种激光器的结构，工作原理和激光特性。     

高功率单模GaAlAs/GaAs激光器

本文报告了隐埋双脊衬底大光腔结构GaAlAs/GaAs激光器的制备和特性,获得CW光输出的最高功率可达80mW。     

半导体量子器件物理讲座 第六讲 半导体量子阱激光器

量子阱结构是半导体光电子器件的核心组成部分,它是半导体光电子集成的重要基础,文章在描述了量子结构的态密度,量子尺寸效应,粒子数反转的基础上,介绍了量子阱导质结构激光器的工作原理,器件结构,器件性能,并对其在可见光激光器和大功率激光器件中显现出来的优越性作了进一步的说明。     

高功率梯度折射率分别限制异质结构InGaAs/AlGaAs应变双量子阱激光器

采用金属有机化合物气相淀积（ Ｍ Ｏ Ｃ Ｖ Ｄ）方法成功地研制了具有两对梯度折射率（ Ｇ Ｒ Ｉ Ｎ）异质结结构的 Ｉｎ Ｇａ Ａｓ／ Ａｌ Ｇａ Ａｓ 应变双量子阱激光器。该激光器的波长为 ９７０～９８２ ｎｍ ,室温连续工作阈值电流密度为１４０ Ａ／ｃｍ ２, 工作在０．９ Ａ 时单面连续输出光功率为５２０ ｍ Ｗ , 工作在２．０ Ａ 时, 连续输出光功率为 １．４９ Ｗ , 最高功率可达 ２．４ Ｗ 。微分量子效率高达０．８３ Ｗ ／ Ａ。     

InGaAs/GaAs单量子阱PL谱的温度变化特性

采用分子束外延方法制备了InGaAs/GaAs单量子阱,利用自组装的光致荧光探测系统,对其进行了光致荧光谱研究。考察了不同温度下荧光峰波长、峰形的影响。研究结果表明:高温时荧光主要是源于带—带间载流子跃迁,而在低温时则来源于束缚在量子阱中激子的跃迁。     

High Power 980 nm InGaAs/AlGaAs Strained Quantum Well Lasers

1lntroductionCarhan,aIVcolutnnelement,hasmanyadvantagesinGaAsAlGaAsmaterials,suchasIowdiffudricoefficient,relativelowactivateenergyabout26meV,highincmptiOnconcentratboandhighm0bilityduetothelowcomensaterate.SocarbonhasbeenwidelyusedinGaAsAlGaAsheter0unctionbipoartransistors(HBT),modulationdoPingfieldeffecttransistors(m),tunneldiodes,iInPurityinducedlayerdisorderinglaserdiodeS,anddistributedBraggreflectors(DBRs)intheverticalcavitysurfaceedrittinglasers(VCSEL).Ingeneral,therearesever…     

High Power 980 nm InGaAs/AlGaAs Strained Quantum Well Lasers

By low-pressure metalorganic chemical vapor deposition (LP-MOCVD) system,InGaAs/AlGaAs graded-index separate-confinement heterostructure strained quantum well lasers are grown with carbon doped the upper cladding layer and the capping layer. Carbon tetracholride (CCl4) is used as the carbon source. 100 μm oxide stripe lasers are fabricated,and the laser output power per facet (uncoated) reaches 1.2 W with 2A injection current under the room temperature continuous wave (CW) operation. The threshold current density is 150 A/cm2 with 1000 μm cavity length. The slope efficiency per facet reaches 0.53W/A,and the total external differential quantum efficiency is above 85%. The relations between the threshold current densities,the differential quantum efficiency and the cavity length are studied.     

Effect of Quantum Well Width Reduction for GaInNAs/GaAs Lasers

We investigated the function of the quantum well (QW) width for laser characteristics especially for reduction of the well width. We pointed out that such reduction has almost no influence on the optical gain or the carrier overflow for a large conduction band offset system, such as GaInNAs QWs. A thin QW is advantageous for suppression of the carrier overflow to the higher quantized energy levels which results in good temperature and gain characteristics. Thin GaInNAs QWs is a good candidate for an active layer structure of the lasers utilized in the next optical communication systems.     

Temperature Dependence of the Threshold Current and the Lasing Wavelength in 1.3-μm GalnNAs/GaAs Single Quantum Well Laser Diode

Temperature stability of the threshold current and the lasing wavelength is investigated in a 1.3-μm GaInNAs/ GaAs single quantum-well laser. The measured characteristic-temperature was 88 K. The small wavelength shift per change in temperature of 0.35 nm/°C was obtained, indicating the superior lasing-wavelength stability. Therefore, it is shown experimentally that GaInNAs is very promising material for the fabrication of light source with excellent high-temperature performance for optical fiber communications.     

In原子掺入对GaInNAs/GaAs单量子阱光致发光的影响

研究了In掺入GaNAs/GaAs单量子阱对其带间和低于带边发光性质的影响。实验结果显示,随着In浓度的增加,GaInNAs/GaAs量子阱带间发光得到改善,低于带边的发光强度大大地减小。这是由于GaInNAs合金生长在GaAs衬底上,为补偿In和N原子尺度的差异,N原子硬倾向于与In原子形成共价健。GaInNAs/GaAs单量子阱的光调制光谱证实了高能端发光峰来自来征的带边发光。     

Resonant magnetopolaron effects in GaAs/AlGaAs multiple quantum well structures

A detailed experimental study of electron cyclotron resonance (CR) has been carried out at 4.2 K in three modulation-doped GaAs/Al_0.3Ga_0.7As multiple quantum well samples in fields up to 30 T. A strong avoided-level-crossing splitting of the CR energies due to resonant magnetopolaron effects is observed for all samples near the GaAs reststrahlen region. Resonant splittings in the region of AlAs-like interface phonon modes of the barriers are observed in two samples with narrower well width and smaller doping concentration. The interaction between electrons and the AlAs interface optical phonon modes has been calculated for our specific sample structures in the framework of the memory-function formalism. The calculated results are in good agreement with the experimental results, which confirms our assignment of the observed splitting near the AlAs-like phonon region is due to the resonant magnetopolaron interaction of electrons in the wells with AlAs-like interface phonons.     

Photoluminescence and photoluminescence excitation of AlGaAs/GaAs quantum wells with growth-interrupted heterointerfaces grown by molecular beam epitaxy

We have measured the photoluminescence (PL) and PL excitation (PLE) of AlGaAs/GaAs single quantum wells with growth-interrupted heterointerfaces. PLE shows the small Stokes shifts of less than 1 meV indicating the extremely flat heterointerfaces without microroughness. Photoluminescence spectra show four peaks originating from different monolayer terraces. These peaks exhibit a doublet splitting. We assigned this doublet to free excitons and excitons bound to neutral donors from the strong well width dependence of doublet splitting.     

Anomalous dephasing of two-dimensional electrons in an AlGaAs/GaAs parabolic quantum well structure

Magnetoconductivity measurements are performed on a parabolic quantum well structure. The weak localization effect is observed at a low magnetic field for both single-subband and double-subband occupation regimes. Applying weak-localization theory, we have extracted the dephasing rate. The extracted dephasing rate increases with increasing conductivity in the small-energy-transfer regime and shows a similar trend as the electron density is increased in the large-energy-transfer regime. This is in conflict with Fermi-liquid theory, and cannot be attributed to electron–phonon scattering.     

InP基InGaAlAs/InGaAsSb应变量子阱激光器的子带跃迁计算

采用有效质量模型下的4×4 Luttinger-Kohn哈密顿量矩阵对In0.53Ga0.39Al0.08As/InxGa1-xAs0.9Sb0.1量子阱结构的能带进行了计算。求得了C1-HH1跃迁波长随In组分及阱宽的变化关系,并采用力学平衡模型计算了此应变材料体系在生长时的临界厚度。结果表明,在结构设计和材料生长中采用合适的材料组分和阱宽,在InP基InGaAlAs/InGaAsSb应变量子阱激光器中能够实现1.6～2.5 μm近中红外波段的激射波长。     

In0.2Ga0.8As/GaAs单量子阱PL谱温度特性及其机制

测量了不同阱宽In0.2Ga0.8As/GaAs单量子阱的PL谱的峰值波长和荧光谱线半峰全宽随温度的变化。利用Varshni公式对实验峰值波长进行拟合,得到了新的参数。结果表明,无位错应变量子阱带隙仍具有其体材料的特性:荧光谱线半峰全宽随温度升高迅速展宽,这主要归因于声子关联作用增强和激子热离化为自由载流子所致;阱宽越窄荧光峰值能量越高,将其与量子尺寸效应的理论计算结果进行了比较。文中还考察了谱线半峰全宽和阱宽的关系,利用合金无序对这一现象进行了解释。