Ultra-high repetition rate InAs/InP quantum dot mode-locked lasers

We have designed, grown and fabricated InAs/InP quantum dot (QD) waveguides as the gain materials of mode-locked lasers (MLLs). Passive InAs/InP QD MLLs based on single-section Fabry-Perot (F-P) cavities with repetition rates from 10 GHz to 100 GHz have been demonstrated in the C- and L-band. Femtosecond (fs) pulses with pulse duration of 295 fs have been achieved. The average output power is up to 50 mW at the room temperature of 18 °C. By using the external fiber mixed cavities fs pulse train with a repetition rate of 437 GHz has been generated. We have also discussed the working principles of the developed QD MLLs.     

Carrier transport and its effect on the turn-on delay time in strained GalnAsP/InP multiple quantum well lasers

The effects of carrier transport on turn-on delay time in multiple quantum well lasers were investigated both theoretically and experimentally. By using rate equation analysis with two components of the carrier density inside and outside of the quantum wells, we found that carrier transport caused two important effects: one is the stationary effect of a significant reduction in carrier density in quantum wells; the other is an increase in differential carrier lifetime.As an experimental investigation, compressively strained 1.3 m GalnAsP/InP multiple quantum well (MQW) lasers were fabricated and their turn-on delay times were measured and investigated. The short-cavity buried-heterostructure lasers showed low-threshold current (2 to 3 mA) and small turn-on delay time (<200 ps) at biasless 30 mA pulse current. Although these performances are suitable for high-speed digital transmission, it was found that the carrier lifetimes derived from the turn-on delay measurement were larger for strained quantum well lasers than for conventional quantum well lasers and double heterostructure lasers. These phenomena are explained using the carrier transport model and are discussed. The solutions for further reduction in carrier lifetime and turn-on delay are discussed.     

High-temperature operation of AlGaInAs/InP lasers1994

We discuss the design of uncooled lasers which minimizes the change in both threshold current and slope efficiency over the temperature range from–40 to +85°C [1]. To prevent carrier overflow under high-temperature operation, the electron confinement energy is increased by using the Al _x Ga _y In_1–x–y As/InP material system [1] instead of the conventional Ga _x In_1–x As _y P_1–y /InP material system. Experimentally, we have investigated strained quantum well lasers with three different barrier layers and confirmed that the static and dynamical performance of the lasers with insufficient carrier confinement degrades severely under high-temperature operation [2]. With an optimized barrier layer, the Al _x Ga _y In_1–x–y As/InP strained quantum well lasers show superior hightemperature performance, such as a small drop of 0.3 dB in slope efficiency when the heat sink temperature changes from 25 to 100°C [3], a maximum CW operation temperature of 185°C [4], a thermally-limited 3-dB bandwidth of 13.9 GHz at 85°C [2], and a mean-time-to-failure of 33 years at 100°C and 10 mW output power [5].     

Degradation of high-power semiconductor quantum-well lasers

A mechanism of degradation of semiconductor quantum-well lasers with a stripe contact more than 50 µm wide is proposed. This mechanism implies formation of several lasing channels at a carrier ambipolar diffusion length smaller than the contact width. The carrier diffusion length decreases with time due to the increase in the number of defects; as a result, the number of lasing channels increases and lasing spectrum is filled. The shape of the lasing spectrum can be used to predict the laser service life.     

Modal properties of all-active InGaAsP/InP microring lasers

An experimental investigation of the multimode dynamics of 1.55 μm-InGaAsP/InP microring lasers is demonstrated. Different operation regimes are observed, bidirectional multimode, unidirectional single mode, bidirectional single mode and mode-hopping. The extent of each of the above operation regimes is examined with respect to the ring current level, bus waveguide reflectivity and ring radius. The back-reflections generated from the bus waveguide facets are indirectly controlled via the bus waveguide current. In order to clarify the physical mechanisms beyond experimental results, a multimode model based on the rate equation approximation is utilized. The experimental results are in good agreement to those predicted by the multimode model.     

Optical transitions in strained InAsSb/GaInSb interband QC lasers

In this paper a detailed simulation and theoretical analysis based on model-solid theory and the(→κ)·(→ρ)methodare presented to investigate the dependence of the band structure on the strain deformation in a noveltype-Ⅱ quantum well(QW)heterostructure InAs1_ySby/GaxIn1-xSb under the uniaxial approximation,and subsequently the optical transition and the gain in the interband cascade lasers containing it havebeen evaluated with unchanged injection current densities.The simulation results show that the straineffect on the transition in this heterostructure will not behave as a simple monotonic trend with the latticemismatch of InAs1_ySby/GaxIn1_xSb interface,but as a function of the complex strain chain includingthe whole active region.It is important to the subsequent device design and optimization.     

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。     

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1.6 nm,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。     

GaInAsP/InP double-heterostructure lasers for fiber odtic communications

This paper reviews the performance of GaInAsP/InP double-heterostructure diode lasers prepared by liquid-phase epitaxy. These lasers have the advantage that exact lattice-matching between the GaIn-ASP active region and the InP substrate is possible for quaternary alloy compositions giving emission wavelengths over a range that includes 1.1-1.3 μm, the optimum region for optical communication systems utilizing fused silica fibers. Continuous operation at room temperature has been achieved in this region for proton-defined stripe (PDS), oxide-defined stripe (ODs), and junction-defined, buried-stripe (JDBS) lasers. The first three PDS devices to be life-tested have already logged over 6,000, 5,700, and 4,000 h, respectively, of cw operation at room temperature without any degradation.     

GaInAsP/InP double-heterostructure lasers for fiber odtic communications

Abstract

This paper reviews the performance of GaInAsP/InP double-heterostructure diode lasers prepared by liquid-phase epitaxy. These lasers have the advantage that exact lattice-matching between the GaIn-ASP active region and the InP substrate is possible for quaternary alloy compositions giving emission wavelengths over a range that includes 1.1–1.3 μm, the optimum region for optical communication systems utilizing fused silica fibers. Continuous operation at room temperature has been achieved in this region for proton-defined stripe (PDS), oxide-defined stripe (ODs), and junction-defined, buried-stripe (JDBS) lasers. The first three PDS devices to be life-tested have already logged over 6,000, 5,700, and 4,000 h, respectively, of cw operation at room temperature without any degradation.     

Generalised multiple-lateral-mode rate equation modelling of lasers with selective quantum-well intermixing for improved beam quality

A numerical model in terms of rate equations for lateral mode amplitudes for analysing static and dynamic properties of moderately broad stripe (tens of microns) laser diodes is proposed and used for modeling lasers with longitudinally or laterally intermixed passive areas. Introduction of passive diffractive regions is shown to offer some improvement of the laser beam, and the potential of further improvement of the beam by Intermixing lateral fringes along the stripe is discussed.     

Generation of self-sustained pulsations of radiation in InGaAs/GaAs/InGaP quantum-well lasers

We studied the dynamic characteristics of InGaAs/GaAs/InGaP quantum-well lasers generating at two wavelengths of about 1 μm with a spectral separation of 15–40 nm. We observed experimentally regimes of jumplike switching and self-sustained pulsations of radiation. The influence of ballistic transfer of carriers during intraband absorption on the production of positive feedback in the dynamic system is studied theoretically. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 74, No. 4, pp. 533–536, July–August, 2007.     

Anomalous spin-orbit effects in a strained InGaAs/InP quantum well structure

There is currently a large effort to explore spin-orbit effects in semiconductor structures with the ultimate goal of manipulating electron spins with gates. A search for materials with large spin-orbit coupling is therefore important. We report results of a study of spin-orbit effects in a strained InGaAs/InP quantum well. The spin-orbit relaxation time, determined from the weak antilocalization effect, was found to depend nonmonotonically on gate voltage. The spin-orbit scattering rate had a maximum value of 5×10¹⁰ s^?1 at an electron density of n=3×10¹⁵ m^?2. The scattering rate decreased from this for both increasing and decreasing densities. The smallest measured value was approximately 10⁹ s^?1 at an electron concentration of n=6×10¹⁵ m^?2. This behavior could not be explained by either the Rashba or the bulk Dresselhaus mechanisms but is attributed to asymmetry or strain effects at dissimilar quantum well interfaces.     

Ultrafast carrier dynamics in strained In1−xGaxAs/InP heterostructures

The transfer of electrons and holes from barriers to wells is investigated in strained In_1-xGa_xAs/InP multiple quantum wells by time-resolved luminescence upconversion with 300 fs time resolution. The transfer times are in the range of a few ps and independent of the Ga content. The investigation of Ga-rich structures allows to observe directly the hole transfer.     

谱导数法在光谱研究GaInAs/InP和GaInP/AlGaInP多量子阱中的应用

在简要讨论谱导数法物理机理的基础上, 给出了其在光吸收谱和光反射谱方法研究张应变GaInAs/InP和GaInP/AlGaInP多量子阱中的成功应用实例. 比较了不同阶谱导数对测定激子跃 迁能量的影响，论及了其与双调制谱方法、曲线拟合方法的区别. 指出了谱导数法在光谱研 究GaInAs/InP和GaInP/AlGaInP多量子阱中的重要性和易行性. 关键词： 谱导数法 吸收谱 反射谱 多量子阱 激子     

p型GaN/Al0.35Ga0.65N/GaN应变量子阱中二维空穴气的研究

对Ga面p型GaN/Al0.35Ga0.65N/GaN应变异质结构中形成的二维空穴气(2DHG)进行了研究.首先基于半导体-绝缘体-半导体异质结构模型确定了应变异质中的临界厚度,然后自洽求解薛定谔方程和泊松方程,计算了当中间势垒层AlGaN处于完全应变状态和半应变状态两种条件下,顶层GaN及中间层AlGaN厚度的变化对2DHG分布的影响.计算结果表明,势垒层AlGaN和顶层GaN的应变状态和厚度对极化引起的2DHG面密度及分布有重要影响.在此基础上制备了p型GaN/Al0.35 Ga0.65N/GaN应变量子阱结构肖特基器件,并通过器件的C-V测试证实了异质结处2DHG的存在.器件响应光谱的测试结果表明,由于p型GaN/Al0.35Ga0.65N/GaN量子阱中强烈的极化作用和Stark效应使得器件零偏压和反向偏压时的响应光谱都向短波方向移动了10 nm,在零偏压下器件在280 nm处的峰值响应为0.022 A/W,在反向偏压为1 V时,峰值响应达到0.19 A/W,已经接近理论值.