用于产生飞秒压缩态的染料激光器稳定性分析与实验研究

提出一种能产生飞秒脉冲光压缩态的激光器的理论模型，并通过数值计算，详细分析该激光器的稳定性；通过具体的实验研究获得了脉宽为１６０ｆｓ，重复频率为６７ＭＨｚ的稳定的脉冲序列输出，从而为实现飞秒脉冲光压缩态提供了重要的实验手段。 关键词：     

飞秒与皮秒激光脉冲的主动同步及和频产生宽带超短激光的研究

利用主动同步方式实现了飞秒钛宝石激光器与皮秒Nd:YVO₄激光器的同步，得到了时间抖动低于1ps的同步精度.在此基础上进行了两束激光的和频实验研究，产生了波长为460nm的宽带蓝光飞秒脉冲激光.这一技术不仅代表了实现不同波长、不同脉冲宽度激光同步的一般方法，而且也证明了通过和频、差频两束不同激光产生新波长超短脉冲激光的一种全新技术方案. 关键词： 主动同步 超短脉冲 和频 差频     

自锁模Cr：LiSAF激光器的实验研究

以功率为９００ｍＷ，波长为４８８ｎｍ的单线氩离子激光作为泵浦源，在腔内不加任何主动调制器和可饱和吸收体的情况下实现了Ｃｒ：ＬｉＳＡＦ激光器的飞秒级自锁模运转，得到了脉冲宽度为４０ｆｓ，重复频率为１００ＭＨｚ，平均输出功率为４５ｍＷ的稳定的锁模脉冲序列。     

由自锁模钛宝石激光器产生19fs脉冲

由自锁模钛宝石激光器产生１９ｆｓ脉冲林位株，赖天树，陈毓川，郑向阳，徐杏绍，莫党（中山大学物理系，广州５１０２７５）自锁模钛宝石激光器是９０年代发展起来的新型固体可调谐激光器，它以其激光频谱调谐范围宽、能够产生飞秒级短脉冲、输出功率高、装置简单和工作...     

飞秒激光技术的最新进展

详述飞秒激光脉冲技术的最新进展。利用激光系统直接产生的激光超短脉冲达６．５ｆｓ,通过脉冲的压缩放大技术,获得了４．５ｆｓ 的结果。     

飞秒光脉冲的产生,放大和压缩

评述了飞秒光脉冲研究的现状，其包括同步泵浦连续染料激光器、对碰锁模环形染料激光器、飞秒光脉冲的多级放大和超短光脉冲的压缩．     

同步泵浦PML飞秒激光研究

采用CW锁模YAG倍频激光器同步泵浦PML飞秒染料激光器,产生了平均脉宽约55fs、功率为15mW的光脉冲。文章在理论和实验上还研究了同步泵浦飞秒激光脉冲产生技术。     

钛宝石飞秒激光振荡器的稳定性改善

对钛宝石飞秒激光器脉冲序列的强度和时间的稳定性进行了分析.实验比较了钛宝石飞秒激光器底板有无水冷的条件下,输出锁模脉冲序列的稳定性以及中心波长和光谱宽度的变化.结果表明对钛宝石飞秒激光器底板施加水冷可改善锁模脉冲的稳定性. 关键词： 钛宝石激光器 稳定性 飞秒脉冲     

用质谱和光电子能谱研究飞秒强场中的电离动力学

报导了用自制飞秒激光器通过飞秒多光子电离质谱和光电子能谱对飞秒强激光场与分子（氨、苯）相互作用的研究,飞秒激光脉宽约１００ｆｓ,二倍频中心波长４０７．５ｎｍ,聚焦后脉冲功率密度达到１０＾１２Ｗ／ｃｍ＾２,氨的光电子能谱显示了（２＋２）ＲＥＭＰＩ和（２＋２）＋１ＡＴＩ、（２＋２）＋２ＡＴＩ三组电子峰,每组峰又包括伸缩振动ｖ１的带系,ＡＴＩ峰的振动布居出现反转,随着光强增加,谱峰加宽而且振动能级出现平     

多波长单腔型自锁模飞秒钛宝石激光器的运转特性

在自锁模飞秒钛宝石激光器运转状态不变的条件下,仅仅改变所加光阑,便可获得三波长或双波长的飞秒光脉冲运转.在此基础上,我们比较了这两种运转状态下激光器输出脉冲的脉宽,啁啾、中心波长间距和输出功率的差异.给出了在不同条件下运转时的双波长激光器的输出特性.讨论了多波长运转时的一些规律.     

双腔双波长交叉锁模钛宝石飞秒激光器的研究

本文建立了一台双光束泵浦的双腔双波长交叉锁模Ti:Sapphire激光器,实现了中心波长为755nm和845nm的双波长同步锁模输出,得到了脉宽分别为28fs和34fs的锁模脉冲.     

Generation of femtosecond vacuum-ultraviolet pulses

High power femtosecond pulses in the Vacuum Ultra Violet (VUV) have been generated through the nonlinear interaction of femtosecond KrF pulses with xenon and argon gas. Under near resonant two photon excitation of xenon by a femtosecond KrF laser, parametric four wave mixing processes lead to VUV pulses at 147 and 108 nm with pulse energies in the 10 µJ range. Tuning is demonstrated by mixing the KrF pulse with a 500 fs dye laser pulse at 497 nm, resulting in 165 nm emission. In argon, a three photon resonance leads to third harmonic generation at 83 nm and micro joule level pulses near 127 nm generated by a six wave mixing process. Since the spectra of the VUV pulses show an ionization-induced blue shift with increasing KrF laser intensity, the VUV pulses can be shown to have temporal duration less than the pulse width (450 fs) of the KrF laser. Blue shifting of the third harmonic of the KrF laser in argon is dominated by a reduction in the neutral gas density rather than by an increase in the electron density.     

利用三色组合脉冲激光获得孤立阿秒脉冲发射

孤立阿秒脉冲因可以跟踪和控制原子及分子内电子的运动过程而备受关注.本文从理论上开展了氦原子在3束飞秒脉冲激光组合场辐照下产生的高次谐波和阿秒脉冲辐射的研究.组合激光场由16 fs/1600 nm,15 fs/1100 nm和5.3 fs/800 nm的钛宝石脉冲构成.与前两束脉冲合成的双色场产生谐波谱相比,附加钛宝石脉冲的三色场产生的高次谐波发射谱呈现出高转换效率及宽带超连续特性,超连续谱范围覆盖从230—690次谐波,傅里叶变换后实现了128 as高强度孤立短脉冲的产生.该结果归因于合成的三色场呈现出高功率及少周期的中红外飞秒脉冲激光特性,可以有效控制原子电离以及复合发生在中红外飞秒脉冲的一个有效光学周期内.     

Generation of synchronized femtosecond and picosecond laser pulses in a two-beam-pumped Ti:sapphire laser

<正>Two operating modes,independent self-mode-locking and cross-mode-locking,are presented in a two-beampumped double-cavity dual-wavelength femtosecond Ti:sapphire laser.Synchronization of femtosecond and picosecond laser pulses is achieved by properly adjusting the cavity length matching and distributing the pump laser powers in the two laser cavities,and moreover,a timing jitter of 517 fs between femtosecond and picosecond pulses is obtained,with wavelength tuning ranges around 36 and 22 nm in the femtosecond and picosecond cavities,respectively.     

Quantum-dot-based saturable absorber for femtosecond mode-locked operation of a solid-state laser

A quantum-dot-based saturable absorber has been demonstrated to initiate the generation of femtosecond pulses from a passively mode-locked solid-state laser. Control and tuning of the pulse duration from 58 ps to 158 fs was achieved. The 158 fs transform-limited pulses at 1280 nm are the shortest pulses that were produced from the Cr:forsterite laser passively mode locked by an InAs/InGaAs quantum-dot semiconductor saturable absorber mirror.     

Nanosecond and femtosecond ablation of La0.6Ca0.4CoO3: a comparison between plume dynamics and composition of the films

Thin films of La_0.6Ca_0.4CoO₃ were grown by pulsed laser ablation with nanosecond and femtosecond pulses. The films deposited with femtosecond pulses (248 nm, 500 fs pulse duration) exhibit a higher surface roughness and deficiency in the cobalt content compared to the films deposited with nanosecond pulses (248 nm, 20 ns pulse duration). The origin of these pronounced differences between the films grown by ns and fs ablation has been studied in detail by time-resolved optical emission spectroscopy and imaging. The plumes generated by nanosecond and femtosecond ablation were analyzed in vacuum and in a background pressure of 60 Pa of oxygen. The ns-induced plume in vacuum exhibits a spherical shape, while for femtosecond ablation the plume is more elongated along the expansion direction, but with similar velocities for ns and fs laser ablation. In the case of ablation in the background gas similar velocities of the plume species are observed for fs and ns laser ablation. The different film compositions are therefore not related to different kinetic energies and different distributions of various species in the plasma plume which has been identified as the origin of the deficiency of species for other materials.     

Generation of wideband tunable femtosecond laser based on nonlinear propagation of power-scaled mode-locked femtosecond laser pulses in photonic crystal fiber

We implement an experimental study for the generation of wideband tunable femtosecond laser with a home-made power-scaled mode-locked fiber oscillator as the pump source.By coupling the sub-100 fs mode-locked pulses into a nonlinear photonic crystal fiber(NL-PCF),the exited spectra have significant nonlinear broadening and cover a spectra range of hundreds of nm.In experiment,by reasonably optimizing the structure parameters of NL-PCF and regulating the power of the incident pulses,femtosecond laser with tuning range of 900-1290 nm is realized.The research approach promotes the development of femtosecond lasers with center wavelengths out of the traditional laser gain media toward the direction of simplicity and ease of implementation.     

Ultrafast dynamics of o-fluorophenol studied with femtosecond time-resolved photoelectron and photoion spectroscopy

The ultrafast dynamics of o-fluorophenol via the excited states has been studied by femtosecond time-resolved photoelectron imaging. The photoion and photoelectron spectra taken with a time delay between 267 nm pump laser and 800 nm probe laser provide a longer-lived S1 electronic state of about ns timescale. In comparison,the spectra obtained by exciting the S2 state with femtosecond laser pulses at 400 nm and ionizing with pulses at 800 nm suggest that the S2 state has an ultrashort lifetime about 102 fs and reflects the internal conversion dynamics of the S2 state to the S1 state.     

超宽带近红外和蓝光飞秒激光脉冲产生的实验研究

增益介质中泵浦光束提供的软光阑效应对于实现克尔透镜稳定锁模及其超宽带光谱脉冲的产生具有非常重要的作用.实验上首先对半导体泵浦全固化钛宝石飞秒激光器的锁模动态特性进行了研究,在4 W绿光泵浦状态下获得了平均输出功率为570 mW、中心波长在794 nm～835 nm范围内调谐、光谱带宽最大可达135 nm的近红外光脉冲输出,其相应的时域变换极限脉冲宽度均小于10 fs.另外,将光束聚焦在超薄BBO晶体上,获得了中心波长在418 nm～429 nm之间调谐、光谱宽带时域变换极限小于15 fs的蓝光飞秒脉冲.     

Tunable sub-100 femtosecond dye-laser pulses generated with a nanosecond pulsed pumping

Subpicosecond pulses at a fixed wavelength produced with a low-Q cavity dye laser pumped by a single, nanosecond laser (Q-switched Nd:YAG) are converted into tunable high-power sub-100 femtosecond pulses by generation, spectral selection, amplification and compression of a supercontinuum. The tunable, chirped, high-energy pulses obtained are compressed with a prism pair. Energies up to 50 J in sub-100 fs pulses were obtained in the 540 to 650 nm range using 40 mJ of the Nd: YAG-laser pumping pulses at 532 nm. The whole sub-100 fs system including the low-Q dye laser uses only one Nd:YAG laser as a pump source.