利用KTP晶体实现1.08μmNd：YAP激光器锁模

本文描述了利用ＫＴＰ晶体和腔的基波输出镜构成非线性镜实现１．０８μｍＮｄ：ＹＡＰ激光器的被动锁模。实验表明，这种新的锁模技术比用染料作可饱和吸收体的被动锁模技术有很多突出的优点，具有很大的发展潜力。实验测得锁模时基波１．０８μｍ输出２．４ｍＪ，二次谐波０．５４μｍ输出０．５ｍＪ（同样条件下的静态输出为２．５ｍＪ），基波脉冲的平均脉宽为４０ｐｓ。     

1.319μm连续固体锁模激光器

报道了１．３１９μｍＮｄ：ＹＡＧ连续锁模激光器的技术研究。激光器的谐振腔为低热敏腔，用声光振幅调制器作为锁模元件，泵浦腔具有较高的泵浦效率和输出稳定性，获得了重复频率１００ＭＨｚ，平均功率～０．５４Ｗ，脉宽＜１７０ｐｓ的光脉冲。     

一种输出三波长超短光脉冲的激光源

利用对撞脉冲锁模非稳腔Ｎｄ：ＹＡＧ激光器，采用ＫＴＰ非线性晶体作腔外倍频，结合受激拉曼散射技术，在一台锁模激光器同时得到１．０６μｍ，０．５３μｍ，０．６３μｍ超短光脉冲的输出。     

High Quality Factor Q and Low Timing Jitter from MLLD Using Optical Injection

采用１０ＧＨｚ基准时钟光和１０Ｇｂｉｔ／ｓ的数据脉冲信号光注入到锁模激光二极管，降低了周期抖动，当注入功率为－５ｄＢｍ，在基准时钟光波长等于锁模激光二极管的光波长时，获得的最小抖动为０．２５ｐｓ，采用混合锁模激光二极管，在注入功率为＋２７ｄＢｍ时，其Ｑ值达３０００．     

用光脉冲注入从锁模激光二极管再生低抖动高Q值光时钟

采用１０ＧＨＺ基准时钟光和１０Ｇｂｉｔ／ｓ的数据脉冲信号光注入到锁模激光二极管，降低了周期抖动，当注入功率为－５ｄＢｍ，在基准时钟光波长等于锁模激光二极管的光波长时，获得的最小抖动为０．２５ｐｓ，采用给锁模激光二极管，在注入功率为＋２７ｄＢｍ时，其Ｑ值达３０００。     

Nd：YLF激光器中以负反馈强迫的自锁模技术

本文乎次利用ＧａＡｓ光电导开关，控制Ｎｄ：ＹＬＦ激光器腔内的Ｑ值，实现自锁模。稳态自锁脉冲序列长５０μｓ，单脉冲脉宽为１０ｐｓ，能量为０．１μＪ。     

氢化—AFS法测定青藏高原中草药中的微量砷,锑,硒和汞

本文研究了氢化物发生无色散原子荧光法测定青藏高原中草药中的微量砷，锑，硒和汞的方法，在选定的最佳工作条件下，１４种干扰元素的含量低于允许存在量，不影响测定，检出限（μｇ／ｍＬ）为：Ａｓ１．３，Ｓｂ０．３９，Ｓｅ０．２４，Ｈｇ０．４４，９次测定的相对标准偏差（％）的为Ａｓ２．４～４．２Ｓｂ２．５～５．６，Ｓｅ３．１～５．０，Ｈｇ３．８～５．９。４个元素的回收率为９４．７～１０５．４％本方法简便，快速     

37 fs、 0.94 μm钛宝石自锁模激光器的研究

报道了低增益区Ｔｉ＾３＋：Ａｌ２Ｏ３红外飞秒激光器的连续及自锁模运转情况,采用四镜折叠像散补偿腔,对于连续波运转,泵浦阈值功率为５．８Ｗ,其调谐范围为０．９－０．９７μｍ。     

激光二极管泵浦的准连续运转飞秒Cr:LiSAF激光器

报道国内第一台用６７０ｎｍ激光二极管泵浦的准连续锁模运转的Ｃｒ：ＬｉＳＡＦ激光器。对于连续运转,泵浦阈值功率２４０ｍＷ,当吸收功率为３６８ｍＷ的输出,输出波长８５０ｎｍ,斜效率为３．５％。在准连续运转（１００ＨＺ,占空比１／５时）,泵清阈值功率４５ｍＷ,斜效率为９．８％,用染料作为锁模妄动介质,实现了准连续锁模运转,光脉冲输出的中心波长为８５０ｎｍ。     

激光二极管泵浦的准连续运转飞秒CrvLiSAF激光器

报道国内第一台用６７０ ｎｍ 激光二极管泵浦的准连续锁模运转的ＣｒｖＬｉＳＡＦ激光器。对于连续运转, 泵浦阈值功率２４０ ｍ Ｗ, 当吸收功率为３６８ ｍ Ｗ 时, 得到４ ｍ Ｗ 的输出, 输出波长８５０ ｎｍ , 斜效率为３．５％ 。在准连续运转（１００ Ｈｚ, 占空比１／５）时, 泵浦阈值功率４６ ｍ Ｗ, 斜效率为９．８％ 。用染料作为锁模启动介质, 实现了准连续锁模运转, 光脉冲输出的中心波长为８５０ ｎｍ 。     

紧凑型L波段磁绝缘线振荡器的实验设计

 设计加工了一个L波段磁绝缘线振荡器(MILO)，并进行了实验研究。在二极管电压为515~538kV, 二极管电流为58~61kA的条件下, 获得了频率为1.76~1.78GHz，功率为2.2~2.5GW的TM₀₁模高功率微波辐射, 功率转换效率为7.3%~7.9%。实验结果与模拟结果符合得较好。     

紧凑型L波段磁绝缘线振荡器的实验研究

 设计加工了一个紧凑型L波段磁绝缘线振荡器(MILO)并进行了实验研究。该MILO具有一个新型收集极和一个新型模式转换器，射频扼流腔减为一个，同时将阴极杆设计成变阻抗结构，该MILO由一台自建的600kV,8Ω，100ns加速器SPARK01驱动。在二极管电压为515～538kV, 二极管电流为58～61kA的条件下, 该MILO在实验中获得了1.76～1.78GHz， 2.2～2.5GW的TM₀₁模高功率微波辐射, 功转换效率为7.3%～7.9%。在30ns的有效电压脉宽下，实验中测得微波脉冲半高宽为15ns。实验结果与模拟结果符合得较好。     

强流四脉冲电子束源实验研究

 为了进行强流多电子束源研究，对现有2MeV LIA 注入器进行了四脉冲改造，二极管脉冲电压约500kV。实验研究了天鹅绒阴极在四脉冲条件下的发射能力、传导电流负载效应以及阴极等离子体运动对阴极电子发射和束能量的影响。利用空间电荷限制流模型推算出阴极等离子体膨胀速率在1 ~4cm/μs之间。     

基于组合模理论设计的激光二极管阵列外腔

针对激光二极管阵列提出了"组合模"概念,计算了组合模的远场分布.每个组合模在远场的空间分布呈双瓣结构.基于激光二极管阵列组合模的远场分布特征,设计了离轴外腔反馈的激光二极管阵列.运用此装置所获得激光二极管阵列的远场分布有了明显变化.与自由运转的激光二极管阵列相比,离轴外腔反馈的激光二极管阵列远场宽度减少了4.3倍.在抽运电流为16 A时,测得输出激光的功率1.82 W,这相当于相同电流下自由运转激光器输出功率的79%.组合模理论不仅可以用来指导设计一维离轴外腔反馈激光二极管阵列,而且也可以用于设计二维离轴外腔反馈激光二极管阵列.二维离轴外腔反馈激光二极管阵列可以产生高功率,高光束质量输出的激光.     

CW,single-mode,tunable GaAs laser system with good frequency stability

A cryostat has been designed for the refrigeration of a semiconductor diode laser (presently GaAs), using a flow of helium gas with controlled temperature. The possibility of independent adjustment of the injection current and of the temperature of the GaAs laser support allows cw emission over a wide wavelength range (～100 Å for a given diode) while maintaining single-mode operation. A long-term frequency stability of ±30 MHz of the free-running single-mode laser has been obtained. By varying the dc injection current, it was possible to achieve linear scanning of the mode frequency, step by step or continuously, over at least 20 GHz without hopping. Possible applications in optical pumping and high-resolution spectroscopy are discussed.     

Generation of tunable multi-wavelength optical short pulses using self-seeded Fabry-Perot laser diode and tilted multimode fiber Bragg grating

We experimentally demonstrate the simultaneous generation of tunable multi-wavelength picosecond laser pulses using a self-seeding configuration that consists of a gain-switched Fabry-Perot laser diode (FPLD) with an external cavity formed by a tilted multimode fiber Bragg grating.Dualand triple-wavelength pulses are obtained and tuned in a flexible manner by changing the temperature of the FPLD.The side mode suppression ratio larger than 25 dB is achieved at different dualand triple-wavelengths and the typical pulsewidth of the output pulses is ～70 ps.In the experiment,the wavelength separation can be narrowed to 0.57 nm.     

High-power pulse-periodic Nd3+-YAG laser with combined pumping by diode arrays

Output characteristics of the pulse-periodic solid-state laser pumped by diode arrays at a pump pulse repetition rate of 8...512 Hz were studied. Three pump types are used: longitudinal raster-lightguide, transverse, and combined ones. Diode arrays with a pulse power of ～800 W, emitting area sizes of 5 × 25 mm², and radiation divergence along two mutually perpendicular axes equal to 4° and 15°, respectively, were used as a pump source. The pump current pulse duration was varied within 100–350 µs. Three operating modes were studied: (i) free generation, (ii) passive Q-switch, and (iii) acousto-optic Q-switch ones. The lasing peak pulse power was (i) ～2 kW(free generation mode), (ii) ～1.5 MW (passive Q-switch mode), and (iii) ～100 kW (acousto-optic Q-switch mode). The highest average lasing power was 150 W at a pump pulse repetition rate of 512 Hz. The highest pulsed lasing energy was 0.65 J.     

Single-lobed Near Diffraction-limited Beam from 1W Laser Diode Array with an External Cavity

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Analysis of parameters of an electron beam from a plasma-filled diode

We analyze the properties of a high-current electron beam formed in an electron source based on a plasma-filled diode and a linear pulsed transformer. The beam parameters are determined by measuring bremsstrahlung X-rays and the beam current, as well as the photographs of the diode gap in the optical range, of the anode in X-rays, and beam autographs. A beam with a current of ～100 kA and a mean electron energy exceeding 0.7 MeV for an accelerating voltage amplitude of ～1 MV is obtained. The diameter of the generated beam is ～1 cm. The electron beam from the plasma-filled diode makes it possible to attain a high anode power density (>10¹⁰ W/cm²) for exciting shock waves, for obtaining high pressures, and for generating powerful X-rays.     

Single-lobed Near Diffraction-limited Beam from 1W Laser Diode Array with an External Cavity

Abstract　An external cavity for the laser diode array with a conventional mirror in what we call two-time self-injection operation is presented. The external cavity consists of two lenses, a flat external mirror(EM) in the image plane of the array and a prism that is used as an output coupler. The single-lobed near diffraction-limited far field beam of a 1 W 10-stripe gain-guided LD array lies at 6.4°～9° with the external cavity operation in two-time self-injection mode, whereas at 2.5°～3.0° for its normal feedback operation. The width of the far field beam (FWHM) is 0.43° and 0.63° at driving current of 2 and 3.2 ×Ithr, respectively, much narrower than that in normal feedback operation, but at the expense of lower output power. The output of the system is very stable and insensitive to the tilt and position of the EM.