含Cr离子饱和吸收体被动调Q解析解

讨论了慢恢复饱和吸收体的被动调Ｑ过程，在合理简化被动调Ｑ速率方程组的基础上，得到了能反映激发态吸收效应的慢恢复饱和吸收体被动调Ｑ的判据，以及调Ｑ脉冲的峰值功率，脉冲能量，脉冲宽度和能量利用率等调Ｑ重要参量的解析表达式，结果具有一定的普遍性，有助于这类被动调Ｑ激光器的优化设计。     

半导体激光泵浦预激光锁模调Q固体激光器研究

报道半导体激光侧面泵浦预激光锁模调Ｑ的Ｎｄ：ＹＡＧ固体板条激光器，预激光锁模调Ｑ的激光脉冲宽度为３６ｐｓ，调Ｑ包纤各心的锁模单脉冲能量超过７μＪ，相应的峰值功率达２００ｋＷ。     

饱和吸收休调Q的反转粒子数条件

本文从描述饱和吸收体调Ｑ的速率方程出发，推导实现有激发态吸收的饱和吸收体调Ｑ所需的反围粒子数理论上应满足的条件，并对其进行讨论分析。     

饱和吸收体调Q的反转粒子数条件

本文从描述饱和吸收体调Ｑ的速率方程出发，推导实现有激发态吸收的饱和吸收体调Ｑ所需的反转粒子数理论上应满足的条件，并对其进行讨论与分析。     

Cr^4＋：YAG的可饱和吸收特性与被动Q开关性能研究

运用速率方程计算了Ｃｒ＾４＋：ＹＡＧ晶体的可饱和吸收特性参数，包括初始吸收系数，饱和吸收系数，饱和光强和损耗调制度，用Ｃｒ＾４＋：ＹＡＧ对脉冲和连续Ｎｄ：ＹＡＧ激光器进行了被动调Ｑ，在脉冲Ｎｄ：ＹＡＧ激光器上得到了８ｎｓ的调Ｑ激光脉冲，在连续Ｎｄ：ＹＡＧ激光器的调Ｑ中得到了间隔和幅度抖动小于５％的输出脉冲充列。     

半导体激光泵浦锁模调QNd：YAG板条激光器

报道准连续６０Ｗ半导体激光二极管侧面泵浦的锁模调ＱＮｄ：ＹＡＧ板条激光器，调Ｑ锁模的激光脉冲宽度（ＦＷＨＭ）为６０ｐｓ，调Ｑ脉冲包络宽度为２５０ｎｓ，积分能量１６３μＪ，最大锁模脉冲的峰值功率超过１００ｋＷ。     

吉瓦级“力光”可调式钕玻璃激光器

介绍“力光”装置上采用的ＰＴＭ电光调Ｑ技术，不改变光路而将ＰＴＭ与ＰＲＭ电光调Ｑ及长脉冲能量运转方式集成一体，从而方便地实现了四个脉宽的激光输出。     

激光二极管泵浦预激光调QNd：YAG单纵模激光器研究

用国产连续输出功率为１．５Ｗ的半导体激光泵浦Ｎｄ：ＹＡＧ激光器，获得了预激光调Ｑ单纵模激光输出，调Ｑ脉冲幅度起伏小于±１％，输出单纵模线宽小于２５ＭＨｚ。     

微型饵玻璃激光器研究

报道了微型饵玻璃激光器的阶段性研究成果，研究在自由振荡情况下输出膜片反射率，氙灯气压及激光电容的大小对激光输出的影响，采用电光调Ｑ，获得了８ｍＪ的巨脉冲输出，采用转镜调Ｑ，获得了１２ｍＪ的巨脉冲输出，脉宽８０ｎｓ。     

全光纤波长可调谐调Q激光器

实现了全光纤波长可调谐主动调Ｑ和自调Ｑ激光脉冲输出。波长可调谐范围为５．７ｎｍ。主动调Ｑ激光脉冲的最高峰值功率可达２．６Ｗ,平均功率１ｍＷ。观察到了自调Ｑ现象,且对自调Ｑ现象给予了初步的解释。     

采用声光频移器反馈控制实现激光强度稳定

本文基于声光频移器,采用光电反馈方式实现了激光强度的稳定控制。根据声光频移器的布拉格衍射对激光强度的调节作用,以光电反馈得到的反馈电信号控制驱动声光频移器的射频功率大小,进而对声光频移器的输出激光强度进行稳定,激光在47 kHz以下的低频噪声实现最大抑制比为15 dB。实验结果基本满足了所要求的激光稳定度。此外还分析了整个回路的响应特性,测试了除反馈电路之外其他部分的相移特性。     

一种耐静压分布反馈式光纤激光水听器探头设计

大深度工作环境下,静水压会引起分布反馈式光纤激光水听器反射中心波长漂出解调系统的复用窗口,使水听器无法解调目标声压信号;不同的静水压也会引起分布反馈式光纤激光水听器灵敏度的变化,影响光纤激光水听器阵列的一致性。基于电力声类比理论,提出带静压补偿的分布反馈式光纤激光水听器探头,建立结构的声压传递函数,分析各结构参数对传递函数的影响,为分布反馈式光纤激光水听器探头频率响应平坦化设计提供理论依据。加工制作了耐静压分布反馈式光纤激光水听器样品进行测试,在0 kHz～10 kHz频率范围内声压灵敏度波动范围不大于±2.4 dB,2.3 MPa内出射激光中心波长漂移量不大于0.06 nm,对深水光纤激光水听器的研究具有指导意义。     

Amplified feedback DFB laser for 40 Gb/s all-optical clock recovery

A monolithic integrated amplified feedback semiconductor laser (AFL) was fabricated based on quantum well intermixing (QWI) technique. The AFL works as a self-pulsation laser. It consists of a gain-coupled multiple quantum well distribute feedback (DFB) laser diode (LD) section, a passive phase section and an amplified feedback section. The free-running repetition frequency of the AFL can be tuned from 32 GHz to 51 GHz via controlling the feedback strength. All-optical 40 Gb/s clock recovery was experimentally demonstrated using the AFL with a low timing jitter.     

半导体激光器混沌输出的延时特征和带宽

外腔延时特征和带宽是影响混沌激光应用的两个重要参量.本文将一个单路光反馈的半导体激光器输出的激光部分地注入到另一个双路滤波光反馈的半导体激光器中,从而构成一个具有外光注入的双路滤波光反馈半导体激光器系统,即主从激光器系统,用于抑制混沌激光的延时特征并研究其带宽.数值研究了外光注入系数、反馈强度、抽运因子和滤波器带宽对系统输出混沌激光的延时特征的影响,然后将该系统对延时特征的抑制效果和具有外光注入的单路光反馈半导体激光器系统、具有外光注入的双路光反馈半导体激光器系统、具有外光注入的单路滤波光反馈半导体激光器系统以及无光注入双路滤波光反馈半导体激光器系统进行对比和分析,结果表明本文提出的方案对延时特征的抑制效果最好.然后在本文提出的具有外光注入的双路滤波光反馈半导体激光器系统中,延时特征被有效抑制的参数条件下研究系统输出混沌激光的带宽,结果表明,通过适当选择参数的取值,本文提出的方案可以提高系统输出混沌激光的带宽.     

Light-induced grating formation in dye solutions by two independent laser beams

The distributed feedback laser effect was used for the detection of light-induced gratings created in organic dye solutions due to the interference of actively mode-locked ruby laser radiation and that of electrooptically Q-switched ruby laser. Radiation kinetics in different regions of the dye superfluorescence spectrum was studied. The distributed feedback effect was shown to be caused by the amplification coefficient grating in the conditions under discussion.     

Experimental control of a chaotic semiconductor laser

We have experimentally controlled the chaotic output of a single-mode semiconductor laser pumped near threshold and subject to optical feedback. We used a novel technique called dynamic targeting, which was theoretically proposed by Wieland et al. [Opt. Lett. 22, 469 (1997)]. Optical feedback causes the semiconductor laser to undergo a bifurcation cascade that exhibits regions of stability, periodicity, chaos, and coherence collapse. By adjusting the feedback phase simultaneously as the feedback strength was varied we steered the laser into the stable maximum gain mode, and thus we stabilized the system at maximum intensity.     

1550nm-VCSELs在偏振保持光反馈和正交光注入下的偏振转换特性

基于自旋反转模型,研究了1550 nm垂直腔面发射激光器(1550 nm-VCSELs)在偏振保持光反馈和正交光注入下的偏振转换特性.结果表明:正交光注入下的从激光器会随着注入强度的增加产生偏振转换.在归一化注入电流较小时,改变反馈强度,会使从激光器发生偏振转换的注入强度出现规律不同的变化;改变频率失谐,会使从激光器发生偏振转换的注入强度出现规律相同的变化.     

分布反馈光纤激光器阵列中外腔反馈特性研究

以半导体激光器中的复合腔模型和实测的分布反馈光纤激光器的外腔端面反射率为基础,对不同反射率条件下分布反馈光纤激光器的输出功率进行了仿真,同时搭建了二基元分布反馈光纤激光器阵列实验平台,对仿真结果进行了验证.仿真与实验结果表明:外腔反馈光重新注入分布反馈光纤激光器会增加激光器的输出功率,降低了阵列的输出功率平坦性.并且外腔端面反射率越大,这种平坦性降低的效果越明显.在构建分布反馈光纤激光器阵列时,应考虑外腔反馈对阵列输出功率平坦性造成的影响,尽量选择外腔端面反射率较小的激光器进行组阵.     

利用振幅调制器进行光电负反馈抑制激光强度噪声

采用振幅调制器作为抑制激光强度噪声的元件，首先对光电负反馈回路进行了简要的理论分析，然后利用该光电负反馈进行抑制激光二极管抽运全固化单频环形Nd:YVO4红外激光器强度噪声的实验。结果表明，在0－1MHz的低频段，强度噪声大幅度降低，最大降低约15dB。     

Sensitivity to external optical feedback of circular-side hexagonal resonator microcavity laser

The sensitivity to fault reflection is very important for larger dynamic range in fiber fault detection technique. Using time delay signature (TDS) of chaotic laser formed by optical feedback can solve the sensitivity limitation of photodetector in fiber fault detection. The TDS corresponds to the feedback position and the fault reflection can be detected by the laser diode. The sensitivity to feedback level of circular-side hexagonal resonator (CSHR) microcavity laser is numerically simulated and the feedback level boundaries of each output dynamic state are demonstrated. The peak level of TDS is utilized to analyze the sensitivity. The demonstration is presented in two aspects:the minimum feedback level when the TDS emerges and the variation degree of TDS level on feedback level changing. The results show that the CSHR microcavity laser can respond to the feedback level of 0.07%, corresponding to -63-dB feedback strength. Compared to conventional distributed feedback laser, the sensitivity improves almost 20 dB due to the shorter internal cavity length of CSHR microcavity laser. Moreover, 1% feedback level changing will induce 1.001 variation on TDS level, and this variation degree can be influenced by other critical internal parameters (active region side length, damping rate, and linewidth enhancement factor).