一个简单的量子阱激光器等效电路模型

给出一个新的量子阱激光器等效电路模型,由量子阱激光器单模速率方程推导得到并在电路模拟程序ＳＰＩＣＥ中完成。该模型考虑了热辐射效应和分离限制区域（ＳＣＨ）内的载流子工作情况,给出了新的光增益表达式。并利用该模型对单量子阱激光器的小信号特性和瞬态大信号特性进行了预测,模拟结果表明和速率方程的直接求解结果吻合很好。     

用可饱和布喇格反射器对固体激光器锁模

用可饱和布喇格反射器对固体激光器锁模半导体可饱和吸收体已成功地用於被动锁模固体激光器，产生了稳定的超短光脉冲。其方法包括用单片反共振法－珀可饱和吸收体或内腔多量子阱器件以及用共振可饱和吸收体进行共振被动锁模。某些损耗与所用具体方法有关。由于固体激光器...     

双偏振双波长混合应变量子阱激光器

本文报道了以混合应变量子阱结构为有源区的激光器。对有源区分别采用体材料、匹配量子阱、压应变量子阱和混合应变量子阱结构的激光器进行了比较。混合应变量子阱激光器能同时工作于两种偏振模式，而且两种偏振模式的激射波长不同。结合实验结果，我们可以看出在混合应变量子阱结构中，从偏偏自发辐射谱峰值长差不能推断两种量子陆的能带填充效应大小。     

量子阱激光器计算机模拟系统

文章介绍了了一个量子阱激光器计算机辅助分析系统ＱＷＣＡＤ,该系统集成了增益计算,异质结激光器二维模拟,量子阱激光器二维模拟等几个适用工具,给出了激光器二维结构的描述方法,引入了量子效应及热效应模型,并附有中间及最后结果的一维及二维曲线输出。     

小发散角量子阱激光器研究

使用三层平板波导理论分析了半导体量子阱激光器远场分布。针对大功率激光器讨论了极窄和模式扩展波导结构方法减小垂直方向远场发散角,得到了极窄波导结构量子阱激光器远场分布的简化模型,获得了垂直发散角的理论值,垂直方向远场发散角减小为28.6°;使用传输矩阵方法模拟了模式扩展波导结构量子阱激光器的近场光斑及远场分布,垂直方向远场发散角减小为16°。实验测试了极窄和模式扩展波导结构量子阱激光器的垂直发散角,理论结果与实验测试获得的发散角基本一致,实现了降低发散角的要求,获得了小发散角量子阱激光器。     

基于三层速率方程的单量子阱激光器电路模型

量子阱激光器以其优良的性能,成为光通信领域的一种重要光源.在量子阱激光器模型中引入中间过渡态,能更完整地描述阱中载流子的输运过程.对基于三层速率方程的单量子阱激光器电路模型进行模拟分析,探讨了过渡态在载流子输运过程中的作用.其模型仿真的结果对器件设计及不同模型的选用具有十分重要的参考价值.     

多量子阱半导体激光器的瞬态响应特性分析

根据光增益与载流子密度的对数关系,在受激发射速率中分别引入了增益饱和项和载流子复合项,通过适应于多量子阱激光器的速率方程,从理论上证明了短腔结构存在与阈值电流最小值对应的最佳阱数。给出了多量子阱激光器的瞬态呼应特性的直接仿真结果及相图,分析了注入电流、阱数和腔长对其激射阈值、开关延误时间、弛豫振荡频率和光输出等能量的影响。     

国外信息

国外信息可饱和布喇格反射器锁模的固态激光器半导体可饱和吸收体已经被成功地用于被动锁模固体激光器，以产生稳定的超短光脉冲．锁模方法有：用单片反共振Ｆ－Ｐ可他和吸收体或者腔内多量子阱装置和用腔外可饱和吸收体进行的共振被动锁模．每种方法的损耗各不相同．由于...     

MOCVD生长的硅衬底上GaAlAs/GaAs单量子阱和多量子阱激光器深能级研究

应用深能级瞬态谱(DLTS)技术研究经MOCVD生长的硅衬底上GaAlAs/GaAs 单量子阱和多量子阱激光器深能级.样品的 DLTS谱表明,在激光器的量子阱和 n-GaAlAs 限制层里均存在着一个浓度和俘获截面较大的高温电子陷阱,该陷阱可能与MOCVD生长工艺和质子轰击引进的损伤有关,它直接影响激光器的性能.DX中心和高温电子陷阱在量子阱里可能局域在GaAlAs/GaAs层的界面附近.     

InGaAsP量子阱激光器结构与阈值电流密度的关系

计入俄歇复合过程的影响,从理论上研究了InGaAsP多量子阱激光器的阈值电流密度。在评述辐射和俄歇过程中考虑了二维载流子在量子化次能带间的所有可能跃迁。俄歇复合电流强烈地依赖于量子阱结构,这样就需要对量子阱激光器的结构进行精心的设计。此外,还阐述了能获得最低阈值电流密度的InGaAsP多量子阱激光器的结构设计程序。     

A physical model for mode-locking process of colliding pulsemode-locked multiquantum-well semiconductor laser

In this paper, we first present a physical model for mode-locking process of the colliding pulse mode-locked multiquantum-well laser diode (CPM-MQW-LD). The absorption of saturable absorber on pulse leading edge and the scattering of the transient grating generated in absorption and gain regions on pulse trailing edge are considered. As an example, the mode-locking process of a multiquantum-well structure laser and the effect of transient grating on pulse width and peak power are studied     

Dynamics of monolithic passively mode-locked semiconductor lasers

Monolithic colliding pulse mode-locking (CPM) in semiconductor lasers is compared with self colliding pulse mode-locking (SCPM) through a large signal dynamic computer model which incorporates most of the significant features of semiconductor lasers. These include gain saturation, spontaneous emission, the gain-frequency relation, and the line-width enhancement factor. This new model replicates many of the published experimental results and also gives additional insight into the internal operation of the device. In particular, gain saturation combined with the standing waves created by colliding pulses within the saturable absorber produce a transient gain grating. This is found to have significant effects in locking either the even or the odd modes together in CPM. A performance comparison between CPM and SCPM is completed and some key design parameters of both configurations are explored     

利用半导体可饱和吸收镜实现的全光纤被动锁模激光器

设计了包含半导体可饱和吸收镜(SESAM)、单包层高掺Yb增益光纤和光纤布拉格光栅(FBG)的全光纤激光器,实现了皮秒级,中心波长约为1064 nm,3 dB线宽约为0.4 nm,重复频率约为17.3 MHz的稳定的连续(CW)被动锁模脉冲输出。观察并分析了输出激光随抽运功率升高和降低的变化过程,升高过程中连续锁模启动时抽运功率阈值为50 mW,降低过程中能够实现稳定锁模的最小抽运功率为37 mW。随着抽运功率的加大,首先出现调Q现象。然后出现连续锁模,并伴有很小幅度的调Q现象。继续加大功率,脉冲会出现分裂;抽运功率越大,单脉冲分裂成的多脉冲越多,多脉冲调制越强。在较少脉冲演变为较多脉冲的过程中,会出现调制的不稳定性。当抽运功率足够大时.会出现多脉冲个数及峰值的不稳定现象。半导体可饱和吸收镜被动锁模会使输出激光谱线加宽,随着抽运功率的加大和锁模的加强,输出激光谱线逐渐加宽。随着脉冲分裂个数增多,单个脉冲脉宽变窄。在多脉冲调制阶段,外界微扰会对系统产生一定影响。     

Mode-Locked Bi-Doped All-Fiber Laser With Chirped Fiber Bragg Grating

We demonstrate a bi-doped fiber laser with dispersion compensation provided by a linearly chirped fiber Bragg grating. Reliable self-starting mode-locking was achieved by using an InGaAsN semiconductor saturable absorber mirror. The all-fiber laser generated short optical pulses with a duration of 1.9 ps at ~ 1165 nm. The large anomalous dispersion of the fiber grating ensured operation in the soliton pulse regime. This in turn enabled us to increase the repetition rate of the output pulse train up to 100.6 MHz via harmonic mode-locking.     

Calculation of the colliding pulse mode locking in CW dye ring lasers

A calculation of the influence of a transient absorber grating on the pulse parameters of a dye laser in the "colliding pulse mode-locking" (CPM) regime is given. It is shown that, compared to other passive methods, considerably shorter pulses with a more favorable stability region can be obtained. Within the stability range of single pulse operation the shortest pulses in the CPM are obtained by operating far above threshold where the saturation energy of the amplifier is much greater than that of the absorber. Deviation from an amplifier position that is symmetric with respect to the amplification of the counter-running pulses leads to different energies of the pulses and to a strong decrease of the stability range. Taking the dispersive properties of absorber and amplifier into consideration, equations for the time dependent phase of the laser pulse are established and solved by an analytical ansatz. The resulting pulse chirp is shown to be mainly dependent on the detuning of the pulse frequency from the center frequency of the saturable absorber. The estimated values for the pulse duration and the down-chirp for typical experimental conditions of a rhodamine 6G-DODCI CPM laser agree well with the measured ones.     

对撞锁模中的瞬态饱和光栅问题

本文讨论了饱和光栅的物理机制,分析了对撞锁模中的瞬态饱和光栅现象及其作用。分析表明,瞬态饱和光栅作用不足以用来解释对撞锁模技术提高饱和吸收体脉冲压缩效率的物理机制。     

Single and double mode-locked ring dye lasers--Theory and experiment

A computer model is made of the colliding-pulse ring dye laser for mode-locked production of short pulses. Initial conditions of either noise or a small CW oscillation eventually result in the same final solution. Resolution is 10 ps in the model, and a digital filter represents dispersion. A gain-sharing long pulse mode often results, but large effective absorption cross section in the mode-locking dye and optimum separation of the two dyes (one quarter of the total resonator length) favor the desired short pulse formation. The model does not include the transient grating effect. Experiments with a ring laser using rhodamine 6G and DODCI confirmed the parameters important to the two regions. Double mode locking, in which the mode-locking dye also lases, was also studied both in the model and experimentally. It is not yet clear if the advantages of colliding pulse mode locking apply to double mode locking.     

Theory for passive mode-locking in semiconductor laser structuresincluding the effects of self-phase modulation, dispersion, and pulsecollisions

We present a theory for passive mode-locking in semiconductor laser structures using a semiconductor laser amplifier and absorber. The mode-locking system is described in terms of the different elements in the semiconductor laser structure. We derive mode-locking conditions and show how other mode-locking parameters, like pulse width and pulse energy, are determined by the mode-locking system. System parameters, like bandwidth, dispersion, and self-phase modulation are shown to play an important role in mode-locking conditions and results. We also discuss the effects of pulse collisions and positions of the mode-locking elements inside the cavity on mode-locking stability and show that these effects can be easily included in the presented model. Finally, we give a number of design rules and recommendations for fabricating passively mode-locked lasers     

Theory of mode-locked lasers containing a reverse saturable absorber

An analytic solution is presented for mode-locking a laser using a saturable absorber and reverse saturable absorber with long relaxation times compared to the temporal pulse widths. A reverse saturable absorber is a material with an excited-state absorption cross section larger than the ground-state absorption cross section, where increasing the incident light intensity increases the absorption. The reverse saturable absorber plays an important role in mode-locking laser materials where individual pulses cannot saturate the gain. A numerical example of mode-locking a CW alexandrite laser with a reverse saturable absorber and a saturable absorber is presented.     

Numerical Study of Dynamical Regimes in a Monolithic Passively Mode-Locked Semiconductor Laser

Bifurcation mechanisms of the development and break up of different operation regimes in a passively mode-locked monolithic semiconductor laser are studied by solving numerically partial differential equations for amplitudes of two counterpropagating waves and carrier densities in gain and absorber sections. It is shown that mode-locking regimes with different repetition rates can be multistable for a wide range of laser parameters and that the harmonic mode-locking regime with two counterpropagating pulses in the cavity can exhibit a period-doubling bifurcation leading to different amplitudes and separations of the pulses. The effect of linewidth enhancement factors in gain and absorber sections on the laser dynamics is discussed.