同步泵浦飞秒非临界相匹配红外光参量振荡器

采用非临界相匹配方式，制成一台同步泵浦飞秒红外光参量振荡器。其输出波长的调谐是靠改变泵浦光掺钛蓝宝石激光器的输出波长而得以实现的，其调谐范围为１．０８～１．１３ｕｍ。在９０ｆｓ．１．１ｗ左右的掺钛蓝宝石激光器的泵浦下，同步泵浦光参量振荡器的输出功率为１００ｍｗ．而脉竟只有６０ｆｓ左右。     

波面倾斜脉冲泵浦的高效可见光飞秒光参量产生和放大器

利用脉冲波面倾斜技术补偿三波相互作用的群速度失配，建立了掺钛蓝宝石飞秒再生放大器输出倍频光泵浦共线类匹配ＢＢＯ晶体的光参量产生和放大器，其信号和空闲光输出调谐范围为０．４７～２．７μｍ，脉冲宽度为１００～１７０ｆｓ，重复率为１ｋＨｚ。脉冲最大输出能量为６．５μＪ，总能量转换效率大于１５％。     

锁模铒光纤激光器

锁模铒光纤激光器在１９９６年６月加州阿纳海姆举行的激光电光学会议上（ＣＬＥＯ’９６），Ｃｌａｃｋ－ＭＸＲ公司的工程师展示了一种波长为１．５５μｍ的二极管京浦的商品化锁模饵光纤激光振荡器，输出脉宽短于１００ｆｓ。１．５５μｍ波长是高数据率通讯的重要波长...     

重复率运转的闪光灯泵浦掺钛宝石激光器研究

本文简述闪光灯泵浦的掺钛宝石激光器的发展状况和应用前景，描述了我们研制成功的实用型四灯泵浦的掺钛宝石激光器实验装置和实验结果．实验中采用本单位生长的掺钛宝石棒尺寸为φ１００×１６０ｍｍ，有效泵浦长度为１５２ｍｍ；平凹激光谐振腔，腔长３５ｃｍ；自制的四灯聚四氟乙烯聚光筒，漫反射效率９８％；四灯串联泵浦，闪光脉宽为１０μｓ．当输入能量为３２０Ｊ时，激光输出达到１．７Ｊ，激光效率０．６％，重复频率１Ｈｚ，可调谐范围７００～１０００ｎｍ．     

高增益二极管泵浦固体激光放大器

对高增益二极管泵浦固体激光放大器进行了设计,在输入脉冲峰值功率为１～１０００Ｗ级、脉宽为１０～３０ｎｓ的条件下,利用８０８ｎｍ半导体泵浦源对一种新型几何结构的固体增益介质进行泵浦,实现１００ｍＪ级的脉冲能量输出。     

二极管激光侧面泵浦Nd：YAG的色心调Q激光器

报道准连续６０Ｗ线列阵二极管激光器侧面泵浦的Ｎｄ：ＹＡＧ激光器及用ＬｉＦ：Ｆ２－晶体作饱和吸收体的被动调Ｑ激光器。在重复频率为１０Ｈｚ，泵浦脉宽为４００μｓ，峰值功率为６０Ｗ的泵浦速率下，激光弛豫振荡每周期输出的能量为３ｍＪ，相应的全光光效率为１２．５％。在调Ｑ方式下运转时，每周期可得到３个能量为４００μＪ，脉宽为１１．５ｎｓ的脉冲。通过腔结构的调整，实验中还获得能量为２００μＪ的单横模的单脉冲输出。通过数值模拟讨论了脉冲的形成过程和脉冲特性，并对进一步的研究工作提出了改进方案。     

光泵外腔面发射InGaAs／InP半导体激光器

本文报道了外腔面发射ＩｎＧａＡｓ／ＩｎＰ半导体激光器的实验结果．利用面发射ＩｎＧａＡｓ／ＩｎＰ半导体材料作为激活介质，采用锁模（或连续）Ｎｄ＋３：ＹＡＧ激光（波长１．３２μｍ）泵浦．平均输出功率达１８７ｍＷ，同步泵浦获得最窄脉冲宽度为６ｐｓ，输出波长１．５μｍ，利用衍射光栅对脉冲进行压缩获得１８１ｆｓ超短光脉冲．     

激光二极管泵浦Nd：LMA固体激光器

分析了铝酸镁镧晶体用于半导体激光泵浦的优点，用ＬＤＡ纵向泵浦Ｎｄ：ＬＭＡ单块固体激光器，得到波长为１．０５μｍ，连续功率为３０ｍＷ的ＴＥＭ模激光输出，线偏振度为１００％泵浦阈值功率为２５０ｍＷ。     

自启动、低功率泵浦的自锁模Ti：蓝宝石激光器和它的高效连续运转

报道了一台自启动、长时间稳定、低功率泵浦的自锁模Ｔｉ：蓝宝石激光器和它的高效连续运转的实验结果．实验中观测到５３ｎｍ的光谱带宽（ＦＷＨＭ）．此谱宽可支持１３ｆｓ的激光脉冲．受自相光仪测量仪器的限制．测得的脉宽为２４．６ｆｓ．实际脉冲脉宽可能小于２０ｆｓ．此激光器在自启动锁模、低功率泵浦时．脉宽小于５０ｆｓ．激光器在连续运行时获得０．２Ｗ的泵浦阈值．３５％的斜率效率和１．１Ｗ的激光输出（４Ｗ泵浦）．     

声光诱导单向运转的Nd：Glass环形腔激光器

在ＬＤＡ侧面泵浦的Ｎｄ：Ｇｌａｓｓ环形腔激光器中，利用声光调制器控制激光单向运转，消除空间烧孔效应，获得单纵模输出，通过预激光调Ｑ获得脉宽５０ｎｓ能量为１．４ｍＪ的单纵模理论分析的结果在实验上得到极好地验证。     

应用全反射二阶自相关仪测量超短脉冲脉宽

计算了普遍采用的二阶单发自相关仪光路中的分束片的色散引起的超短脉冲展宽量，指出在脉冲极短时该展宽将导致不准确的测量结果(例如，对于脉冲宽度为3fs左右，通过100μm厚度的K9玻璃分束片，脉冲展宽将达到10％)。基于计算结果，提出了一种新型的采用全反射结构的单发二阶自相关仪设计，通过分波面的方法改变了自相关仪的分束方式，避免了采用透射分束光学元件引起的色散。采用这种全反射式结构的二阶单发自相关仪，可以使自相关测量方法测得的脉冲宽度更为准确，计算得出理论上其最小时间分辨率可达3．6fs。     

复合型二元光学器件补偿色散和相位畸变研究

复合型二元光学器件作为一种新型色散和相位补偿元件,由于其色散的特殊性,在超强超短脉冲激光的色散和波前补偿中具有特殊的意义。提出并研究了利用复合型二元光学器件同时补偿全钕玻璃啁啾脉冲放大(CPA)系统中的色散和相位畸变,并利用光线追迹的方法对二元光学器件模拟了设计和补偿效果。在实验中,利用二元光学器件将100 fs的光束补偿至30 fs左右。实验结果验证了此方法的可行性。     

Low-noise operation modes of a passively mode-locked fiber laser

Optimum low-noise operation modes of a passively mode-locked fiber laser are described and characterized. The laser produces 60 fs bandwidth limited pulses with root mean square amplitude fluctuations of 0.4% in a frequency-band from 30 Hz to 100 kHz. It is shown that low-noise operation up to 5 dB below the amplitude noise of the pump laser is possible with overall negative cavity group-velocity dispersion and a large difference between the intracavity loss under free-running and mode-locked laser operation. Additional frequency stabilization reduces the timing jitter to 4 fs in a frequency band from 1 kHz to 100 kHz and 110 fs in the 30 Hz to 100 kHz band     

Sub-100 fs Kerr lens modelocked Cr4+:YAG laser

Sub-100 fs pulse generation from a Kerr lens modelocked Cr⁴⁺ :YAG laser has been demonstrated for the first time, yielding femtosecond pulses tunable from 1.49 to 1.56 μm with pulses as short as 90 fs obtained at 1.53 μm     

石墨烯被动调Q掺Nd3+激光器研究进展

石墨烯是一种具有独特光学特性的2维碳纳米材料,利用其饱和吸收特性制成的被动调Q开关具有稳定性好、响应波长宽(可见光到中红外)、恢复时间短(约100fs)、非饱和吸收损耗少、制作方法简单、价格便宜等优点,广泛地应用于被动调Q脉冲激光领域。重点对石墨烯被动调Q掺Nd3+激光器研究进展进行了总结,分析了发展趋势,并指出性能优良的石墨烯饱和吸收体是其发展的关键。     

Boosting the Non Linear Optical Response of Carbon Nanotube Saturable Absorbers for Broadband Mode‐Locking of Bulk Lasers

Single‐walled carbon‐nanotube absorbers are experimentally demonstrated for laser mode‐locking. A saturable absorber device is used to mode‐lock three different bulk solid‐state lasers in a 500 nm‐wide wavelength interval. The devices exhibit a low saturation fluence of <10 µJ cm^?2, low scattering losses, and an exceptionally rapid relaxation, with time constants reaching <100 fs. The latter two properties are explained by a decreased curling tendency and increased tube‐to‐tube interactions of the nanotubes, respectively. These properties are the result of an optimized manufacturing procedure in combination with the use of a starting material with a higher microscopic order. The decreased scattering enables universal use of these devices in bulk solid‐state lasers, which tend to be highly sensitive against non‐saturable device losses as caused by scattering. The favorable saturable absorption properties are experimentally verified by mode‐locking the three lasers, which all exhibit near transform‐limited performance with about 100 fs pulse duration. The complete and unconditional absence of Q‐switching side bands verifies the small saturation fluence of these devices.     

飞秒染料激光放大器

本文用重复率为10Hz、调Q、Nd∶YAG激光器的二倍频输出泵浦四级染料放大器,把从对撞脉冲锁模(CPM)环形染料激光器中产生的43fs的光脉冲能量放大到100μJ,脉冲宽度为125fs,峰值功率为800MW,在用一组四棱镜系统对放大的光脉冲进行群速度色散补偿以后,得到了宽度为70fs的放大光脉冲输出,峰值功率达GW。     

Dual Semiconductor Laser System With Rapid Time-Delay for Ultrafast Measurements

We present a dual semiconductor laser system at 1.55 mum with femtosecond pulse widths and very low timing jitter for rapid pump-probe measurements. Synchronizing the two lasers to the same low-noise radio frequency-oscillator allows the use of an electrical phase shifter for the relative time delay between the lasers. This leads to a large scanning window that nearly matches the pulse period of 2.5 ns, as well as achieving a discrete time step of below 100 fs. The timing jitter of the complete dual laser system including all electronics is only 540 fs across the whole time delay. The nonlinear pulse compression using especially designed comb-like dispersion profiled fiber leads to autocorrelation widths of 310 fs. The system performance, i.e., the high time resolution is demonstrated by optical cross correlation of the pump and probe pulse, showing a very low full-width at half maximum of 1.3 ps     

超高功率f秒激光器

介绍了 1 0 f秒光脉冲发生器和放大器、 1 0 0 TW低于 2 0 f秒的钛蓝宝石激光器及其应用。