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.     

InGaAs/GaAs应变量子阱的光谱研究

分别用光致发光谱（PL），光伏谱（PV）及时间分辨谱（TRPL）的方法，测量了应变InGaAs/GaAs单量子阱和多量子阱在不同温度下的光谱，发现单量子阱与多量子阱有不同的光学4性质。多量子阱PL谱发光峰和PV谱激子峰的强度与半高宽都比单量子阱的大，但单量子阱的半高宽随着温度的升高增大很快，这是由激子－声子耦合引起的，通过时间分辨谱研究发现了量子阱子能级之间的跃迁，多量子阱的发光寿命明显比单量子阱的长，我们利用形变势模型对量子阱的能带进行了计算，很好地解释了实验结果。     

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。     

高功率AlGaAs/GaAs单量子阱远结激光器及其老化特性

为了提高器件的可靠性和使用寿命,设计并研制了一种将p-n结和有源层分开的高功率AlGaAs／GaAs单量子阱远异质结(SQW-RJH)激光器,发射波长为808nm,腔长900μm,条宽100μm,其外延结构与通常的808nm AlGaAs／GaAs单量子阱半导体激光器的结构不同,在p-n结和有源区间多了一层p型AlGaAs层,其厚度约为0．1μm。为减小衬底表面位错对外延层质量的影响,在n^ -GaAs衬底和n-Al0．5Ga0．5As下包层间加一层n^ -GaAs缓冲层。对器件进行了电导数测试及恒流电老化实验。与常规AlGaAs／GaAs大功率半导体激光器相比,远结大功率半导体激光器具有阈值电流Ith偏大、导通电压Vth偏高的直流特性。3000h的恒流电老化结果表明,器件在老化初期表现出阈值电流随老化时间缓慢下降,输出功率随老化时间缓慢上升的远结特性。     

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。     

InxGa1－xAs缓冲层上InyGa1－yAs/(Al)Ga

本文中,发现在In_xGa_1-xAs缓冲层上非故意掺杂的In_yGa_1-yAs/(Al)GaAs超晶格样品中存在着两个互相反向的自建电场区,一个位于样品表面,另一个位于In_xGa_1-xAs缓冲层和超晶格界面。据此,合理地解释了样品的光伏测试结果,并对此类样品的MOCVD生长工艺给予指导。     

带有非吸收窗口的高性能InGaAs/AlGaAs量子阱激光二极管

为了解决限制近红外单发射区InGaAs/AlGaAs量子阱半导体激光二极管失效阈值功率提升的腔面光学灾变损伤问题,研制了一种带有Si杂质诱导量子阱混杂非吸收窗口的新型激光二极管,并对其性能进行了测试分析.首先,对于带有非吸收窗口的二极管,在其谐振腔上方前后腔面附近的窗口区域覆盖50 nm Si/100 nm SiO2组...     

In_xGa_（1－x）As缓冲层上In_yGa_（1－y）As／（Al）Ga

本文中，发现在Ｉｎ＿ｘＧａ＿(１－ｘ)Ａｓ缓冲层上非故意掺杂的ＩｎｙＧａ＿(１－ｙ)Ａｓ／（Ａｌ）ＧａＡｓ超晶格样品中存在着两个互相反向的自建电场区，一个位于样品表面，另一个位于Ｉｎ＿ｘＧａ＿(１－ｘ)Ａｓ缓冲层和超晶格界面．据此，合理地解释了样品的光伏测试结果，并对此类样品的ＭＯＣＶＤ生长工艺给予指导．     

High Performance AlGaAs Quantum Well Lasers with Low Beam Divergence Grown by Molecular Beam Epitaxy

ＨｉｇｈＰｅｒｆｏｒｍａｎｃｅＡｌＧａＡｓＱｕａｎｔｕｍＷｅｌｌＬａｓｅｒｓｗｉｔｈＬｏｗＢｅａｍＤｉｖｅｒｇｅｎｃｅＧｒｏｗｎｂｙＭｏｌｅｃｕｌａｒＢｅａｍＥｐｉｔａｘｙ￥ＹＡＮＧＧｕｏｗｅｎ；ＸＩＡＯＪｉａｎｗｅｉ；ＸＵＺｕｎｔｕ；ＸＵＪｕｎｙｉ...     

InGaAs/GaAs应变量子阱激光器线宽展宽因子的理论研究

详细地介绍了计算线宽展宽因子(α因子)的理论基础及推导过程, 建立了α因子的简便模型. 该模型分别考虑了带间跃迁、带隙收缩和自由载流子效应对α因子的影响, 利用不同载流子浓度下的增益曲线得到光子能量随载流子浓度的变化速率以及微分增益, 进而对α因子进行近似计算. 模拟计算了InGaAs/GaAs量子阱激光器的增益曲线及α 因子的大小, 计算结果与文献报道的实验值相符. 进一步讨论了InGaAs/GaAs量子阱阱宽及In组分对α 因子的影响. 结果表明, α 因子随In组分和阱宽的增加而增加.     

高功率905 nm InGaAs隧道结串联叠层半导体激光器

设计出了隧道结串联叠层半导体激光器结构,采用分子束外延进行激光器材料的外延生长,材料经过光刻、腐蚀、欧姆接触、解理、腔面镀高反射/减反射膜、焊装等工艺,制作成条宽200 m、腔长800 m 的半导体激光器。两隧道结激光器在脉冲宽度100 ns,重复频率10 kHz,30 A工作电流下输出功率达到80 W,峰值发射波长为905.6 nm,器件的阈值电流为0.8 A,水平和垂直方向的发散角分别为7.8和25。     

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.     

InGaAs/GaAs应变量子阱结构在1 054 nm激光器中的应用

采用金属有机物化学气相淀积(MOCVD)方法生长了InGaAs/GaAs应变量子阱,通过优化生长条件和采用应变缓冲层结构获得量子阱,将该量子阱结构应用于1 054 nm激光器的制备。经测试该器件具有9 mA低阈值电流和0.4 W/A较高的单面斜率效率,在驱动电流为50 mA时测得该应变量子阱光谱半宽为1.6nm,发射波长为1 054 nm。实验表明:通过优化工艺条件和采用应变缓冲层等手段,改善了应变量子阱质量,该结果应用于1 054 nm激光器的制备,取得了较好的结果。     

The beam properties of high-power InGaAs/AlGaAs quantum well lasers

The vertical beam quality factor of the fundamental TE propagating mode for InGaAs/AlGaAs SCH DQW lasers emitting at 940 nm is investigated by using the transfer matrix method and the non-paraxial vectorial moment theory for non-paraxial beams. An experimental approach is given for the measurement of the equivalent vertical beam quality factor of an InGaAs/AlGaAs SCH DQW laser. It has been shown that the vertical beam quality factor M_x² is always larger than unity, whether the thickness of the active region of LDs is much smaller than the emission wavelength or not.     

MOCVD的InGaAs/GaAs应变层量子阱的低温光致发光研究

本文中利用MOCVD方法得到了高质量的InGaAs/GaAs应变层量子阱材料,4.3nm量子阱10KPLFWHM仅为3.49meV.通过对样品荧光谱在变激发强度,变温时的峰位、峰形研究,我们发现,合金组分起伏散射是样品低温荧光谱展宽的主要原因,因而是MOCVD生长中应该首先解决的问题,实验结果还表明,在讨论低温PL谱形时,必需考虑光生载流子由随机起伏势中高能位置向低能位置的迁移过程。     

InGaAs/GaAs量子链的光学特性研究

研究了InGaAs/GaAs量子链的稳态和瞬态光谱特性,特别是载流子的动力学过程.实验发现荧光寿命有很强的探测能量依赖关系,荧光寿命随发光能量的增加而减小;实验还发现,当激发功率较小时,荧光寿命随激发功率增大而增大,当激发功率足够大时,荧光寿命趋于饱和.这些结果清楚地表明,在量子链结构中,参与发光的载流子之间存在明显的耦合和输运现象,进一步分析表明,这种输运主要是由于载流子沿量子链方向的耦合造成的.发光的偏振特性研究进一步证实了载流子沿量子链方向输运过程. 关键词： InGaAs/GaAs 量子点 量子链     

Photo-pumped lasing from low density self-assembled InGaAs/GaAs quantum dots within a high-Q vertical cavity

A high-Q cavity containing three layers of self-assembled InGaAs/GaAs quantum dots has been prepared. Emission occurs in the wavelength range 1275–1285 nm over the wafer surface. We have observed lasing thresholds in the power-in-versus-power-out characteristics, with associated changes in the angular emission profile, when the structure is optically pumped CW at 300 K. At high pump powers spectrally resolved lateral modes are seen in the emission spectra of a planar cavity and this is discussed in terms of the index change induced by the pump laser.     

Oscillator strength of type-II light-hole exciton in InxGa1−xAs/GaAs strained single quantum wells

We have investigated the excitonic properties of In_0.15Ga_0.85As/GaAs strained single quantum wells by using photoreflectance spectroscopy and a variational calculation method. We clearly detected the photoreflectance signal of the type-II light-hole exciton, which consists of an electron confined in the InGaAs layer and a light hole located in the thick GaAs layer, in addition to the type-I heavy-hole exciton confined in the InGaAs layer. The calculated results of the overlap integral of the envelope function in the type-II light-hole exciton predict that the oscillator strength is remarkably enhanced with decreasing the InGaAs-layer thickness. This is demonstrated by the layer-thickness dependence of the photoreflectance intensity of the type-II light-hole exciton.     

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。     

MBE-grown Ridge-waveguide InGaAs/InGaAsP Strained Quantum Well Lasers at 2 μm Wavelength

1 horottionFor a long time GaSh--based IILV antimonial material is the main material systemfor nddinfrared semiconductor l...[l' 2] because of its wide wavelength range Of 1. 7 4. 5 mp offering a convenient choice for different applications. HOwever there aredifficuhies in its material growth and device fabrication. Iall--based InGaAs/InGaAsPstrained QW Inaterial become attractive for nddinfrared semiconductor lasers because ithas relatively loW thermcrresistance and serial resistance a…