用氮分子激光器泵浦的绿光区染料激光

用氮分子激光器作泵浦源,对新合成的六种吡喃鎓盐染料的丙酮溶液,获得在501—585nm波段内连续可调激光输出。本文对这些染料的激光特性进行了分析和讨论,并对它们的热化学和光化学稳定性进行了研究。     

308nmXeCl准分子激光双侧面对称泵浦之形腔染料激光器研究

描述了用３０８ｎｍＸｅＣｌ准分子激光双侧面对称泵浦之形腔染料激光器，重点探讨了这种激光器的输出光束质量改善问题，实验发现这种双侧面对称泵浦较传统的横向泵浦，光束质量有较好的改善，对于２×１０－３ｍｏｌ／ｌ浓度的ｃｏｕｍａｒｉｎ４６０染料甲醇溶液，在波长４６０ｎｍ处，实验得到１１．７％的能量转换效率     

用腔倒空Nd：YAG激光器对fs超短脉冲的同步放大

实现了用腔倒空Nd:YGA激光器对fs超短脉冲放大器的同步泵浦。由碰撞锁模环形染料激光器产生的80fs脉冲经二级染料放大后,实现放大倍数6.2×10~4,输出超短脉冲峰值功率～2×10~7W。     

皮秒短脉冲光参量啁啾脉冲放大中泵浦信号高精度同步主动控制技术研究

在皮秒短脉冲泵浦的光参量啁啾脉冲放大(ps-OPCPA)系统中,泵浦光与信号光之间的高精度时间同步是需要解决的关键问题之一.本文基于中国工程物理研究院激光聚变研究中心的全OPCPA激光装置,对用于前端ps-OPCPA中泵浦光与信号光的高精度同步主动控制技术进行了详细研究.采用大啁啾信号光窄光谱光参量放大的主动反馈方式,通过合理设计反馈光路信号光的时域展宽啁啾系数,将泵浦光与信号光的同步时间抖动从ps量级降低至百fs量级的时间范围,从而极大地改善了前端ps-OPCPA的能量和光谱不稳定性:7 min测试时间内泵浦光与信号光相对同步时间抖动的均方根值(RMS)从458 fs改善至93 fs,输出能量RMS不稳定性从30.3%改善至3.15%,且维持光谱宽度大于100 nm的稳定宽光谱输出.     

短脉冲强X光泵浦产生光电离三体复合X光激光

 介绍了激光打靶产生短脉冲强X光辐射的方法,给出了打钠靶的数值模拟结果。 数值研究短脉冲强钠X光泵浦氖激光介质的X光激光,通过在氖中加氢的办法降低了电子温 度,有效地提高了激光增益。研究了短脉冲强X光泵浦的高增益光电离三体复合X光激光机 制,提出了在大中型激光器上开展这种X光激光研究的想法。     

短脉冲强X光泵浦产生光电离三体复合X光激光

介绍了激光打靶产生短脉冲强X光辐射的方法,给出了打钠靶的数值模拟结果。 数值研究短脉冲强钠X光泵浦氖激光介质的X光激光,通过在氖中加氢的办法降低了电子温 度,有效地提高了激光增益。研究了短脉冲强X光泵浦的高增益光电离三体复合X光激光机 制,提出了在大中型激光器上开展这种X光激光研究的想法。     

脉冲激光二极管泵浦调Q激光器泵浦时间特性研究

从调Q激光器的速率方程出发,对脉冲激光二极管泵浦的调Q激光器在不同泵浦功率及不同透过率情况下的最佳泵浦时间进行了理论分析。计算结果表明,在透过率为20%,腔内损耗为0.05的条件下,1—3倍阈值泵浦功率时,最高效率对应的最佳泵浦时间为1—1.5倍Nd∶YAG荧光寿命;7倍阈值泵浦功率及以上时,最佳泵浦时间约为荧光寿命的一半或者更短。在脉冲泵浦能量相同时,采用较短的泵浦时间(即泵浦功率较高),调Q输出的能量转换效率较高。     

308nmXeCl准分子激光泵浦猝灭式可调谐染料激光器研究

描述了获得准分子激光超脉冲的一种方法，理论上扼要地介绍了淬来式染料激光器产生超短脉冲激光的机理。实验上以香豆素４９８染料得到波长为４９６ｎｍ，脉宽１ｎｓ，能量１．１ｍＪ的染料激光。     

Transform-limited behavior from the synchronously pumped cw dye laser

We report for the first time transform limited behavior from the picosecond synchronously pumped cw dye laser. This is accomplished by the use of an inexpensive, low-loss intra-cavity etalon. The Fourier relationship between pulse frequency width and time duration is shown to be obeyed quantitatively at three different wavelengths. The pulse profile changes as a function of wavelength and does not follow an analytical functionality at any wavelength studied. For each wavelength, the optical cavity length producing transform limited pulses is shown to be the same.     

Picosecond pulses produced by synchronously pumped cavity dumped pyridine 1 dye laser

Nearly transform limited picosecond pulses have been produced with a synchronously pumped cavity dumped dye laser using pyridine 1 laser dye. The observed tuning range of 678 to 790 nm extends the usefulness of cavity dumped systems pumped by mode locked argon ion lasers. Pulse autocorrelation widths as short as 3.85 ps were observed. The effects of the variation of bandwidth and net gain on autocorrelation shape and width are presented. Observed autocorrelation traces are compared to transform limited autocorrelation traces calculated from the corresponding power spectra.     

Time evolution of synchronously pumped dye laser pulses: Picosecond pulse formation studies

The pulse-by-pulse evolution and compression of the output of a synchronously pumped dye laser as a function of the number of pump pulses was investigated with a high resolution, variably triggered streak camera. The measured pulse durations and energies for the pulse compression process are demonstrated to be in disagreement with the predictions of recent classical rate equation models. This is shown not to be due to the complete breakdown of the model but, rather, is caused by the failure to include two key loss terms in the rate equation treatment, namely, excited state absorption and thermal lensing. In addition, a highly durable dye laser compatible with the 100 MHz output of commercially available QS and ML YAG lasers is presented which is capable of 50 μJ, 20–30 ps transform limited pulses without the need of amplification. Further refinements of this laser system are discussed, based on the experimental work reported, which will lead to tunable ～ 100 fs pulses with energies in the μJ range from a single laser pump source.     

Rate equation simulation of a synchronously pumped dye laser

A simple rate equation model of a standing wave synchronously pumped dye laser yields output pulses which agree qualitatively and quantitatively with recent experimental observations. The shape, amplitude and temporal position of the simulated pulse varies dramatically, not only with cavity length detuning, but also with the gain to loss ratio. Features of pulse formation and stability are predicted which are precluded by the steady-state assumption present in most other models.     

Theory of the synchronously pumped picosecond dye laser

The circulation of a synchronously mode locked dye laser pulse in a linear cavity configuration containing a dye cell as an active medium and a bandwidth-limiting element is treated. The condition that the pulse shape reproduces after each cavity round-trip provides a nonlinear integro-differential equation for the steady-state pulse shape. For the solution of this equation an approximate method, not limited to small pulse energies, is given and the pulse duration, intensity, energy, asymmetry of the pulse shape, stable regions and other interesting parameters are discussed.     

Frequency offset locking of a synchronously pumped mode-locked dye laser

We have developed a scheme of frequency offset locking for transferring the frequency stability of a commercial dye laser to a synchronously pumped mode-locked dye laser. By observing the beat frequency between the two dye lasers, mode stability of less than 2 MHz has been observed for the mode-locked dye laser mode. The use of the mode-locked system as a spectroscopic tool has been demonstrated by observing Doppler-free multiple pulse two photon spectra of the sodium 3S-4D transition.     

板条放大器同步泵浦的宽调谐MgO:PPLN中红外光参量振荡器（英）

搭建了Nd:YVO4/SESAM锁模激光器,采用LDA泵浦的Innoslab对其进行功率放大,最后同步泵浦MgO:PPLN实现了宽调谐皮秒中红外光参量运转。通过改变MgO:PPLN的温度和通道,实现了信号光1415~1557 nm、闲频光3362~4290 nm范围的宽调谐输出,其中最高的光光转换效率为17.5%。同步泵浦功率为16 W,脉冲重复频率为116.9 MHz时,同时获得1.33 W的1518 nm信号光和1.26 W的3558 nm闲频光输出。     

Amplified spontaneous emission from nitrogen laser pumped dye lasers

The nitrogen laser pumped dye laser output has been studied with emphasis on the behaviour of amplified spontaneous emission (ASE) with respect to the tuning wavelength, pump energy, dyes and their concentration and solvents. Spectral spread of ASE is narrower than fluorescence and its maximum is shifted towards the red side. However, lasing occurs beyond the ASE region. ASE is small at high gain wavelength and increases at the edges of the gain curve. Laser energy is highest at the ASE peak with minimum ASE present in the output. ASE is reduced with increased laser energy in the energy transfer dye lasers.     

Timing and detuning studies of a synchronously pumped mode-locked dye laser

The timing relationship between a synchronously pumped mode-locked dye laser and its pump laser is explored experimentally and theoretically. The experimental data is in quantitative agreement with numerical solutions of a semiclassical model that includes no free parameters. The data also agrees qualitatively with an approximate, analytic distillation of this model which is presented here for the first time. Our study has a direct bearing on the jitter and the long term stability of these important ultrashort pulse lasers.