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1.
Third-order harmonic mode locking of a diode-laser pumped bulk Er:Yb:glass laser by frequency modulation with a lithium niobate modulator is reported. Stable pulses at a repetition rate of 2.5 and 5 GHz with a pulse duration down to 9.6 ps are obtained. The average output power is 3 mW, the pulse peak power is 120 mW at 2.5 GHz repetition rate, and the pulses are approximately 1.4 times transform limited. The pulse duration can be increased up to 30 ps by decreasing the mode-locker drive power  相似文献   

2.
为了实现铜蒸气激光器电源的小型化,采用高压大功率脉冲变压器对储能电容进行开关脉冲充电的电路拓扑,通过建立设计和输出模型,采用铁基超微晶材料,研制了高压大功率脉冲变压器,在14kHz下实现了13kV的充电电压,传输功率超过2.3kW。通过控制IGBT的触发脉宽,可实现输出电压和功率的调节。  相似文献   

3.
激光二极管抽运声光调Q高重复频率473nm激光器   总被引:3,自引:2,他引:3  
冯立春  霍玉晶  何淑芳 《中国激光》2005,32(8):027-1030
实现了重复频率高达100kHz,紧凑的全固态激光二极管抽运的声光调Q473nm腔内倍频蓝光激光器。使用5mm长的Nd∶YAG作为激光介质,倍频采用了10mm长的I类非临界匹配LBO晶体,激光器外形尺寸为11cm×6cm×3cm。使用2W的激光二极管抽运,20kHz重复频率下,得到平均功率为64.8mW的473nm稳定输出,总光光转换效率为3.2%。在1kHz重复频率下,得到脉冲宽度为23ns,峰值功率接近700W,单脉冲能量达到16μJ的稳定的473nm激光脉冲。推导了准三能级系统的储能公式。此公式与以前的结果不同,认为有效储能时间不等于上能级寿命。通过实验结果的分析验证了这个结论。  相似文献   

4.
电光调Q射频激励波导CO2激光器   总被引:6,自引:3,他引:6  
报道了电光调Q射频波导CO2激光器,其中波导长度400mm,在插入电光调Q晶体但不加调制电压情况下,激光器的连续输出功率为3.5W。调Q脉冲重复频率1Hz~10kHz可调,在10kHz重复频率时,获得了脉冲峰值功率为200W,脉冲宽度为400ns的输出。  相似文献   

5.
激光二极管(LD)泵浦的Q调制高频率、窄脉宽、高峰值功率的固体激光器在激光雷达、激光加工等领域日益得到广泛的应用,而更高调制频率的固体激光器在将来会更受青睐。分析了泵浦功率和输出透过率两个因素在10~100 kHz调制频率下对脉宽的影响程度。研制了LD单端泵浦Nd:GdVO4声光调Q 激光器,实现了重频100 kHz下窄脉宽激光输出。在重频为80 kHz时,获得脉宽17.7 ns,平均输出功率3.49 W,峰值功率2.46 kW和在重复频率为100 kHz时,获得脉宽19.6 ns,平均输出功率3.52 W,峰值功率1.79 kW的效果。  相似文献   

6.
激光二极管(LD)抽运的固体激光器(DPSSL)的调Q器件是获得高重复频率、高峰值功率的有效手段之一,随着激光雷达、激光加工业的发展,要求调Q器件向着更高重复频率的方向发展。Nd∶GdVO4以其优异的物理和激光特性,使得它在激光二极管端面抽运固体激光器的声-光(A-O)调Q器件中,即使在很高的调制重复频率下,仍可获得窄脉宽、高峰值功率的脉冲激光输出。理论分析了影响脉冲激光的输出能量和脉宽大小的决定因素,研究了脉宽、平均输出功率及峰值功率随调Q重复频率的变化关系。利用双激光二极管双端抽运Nd∶GdVO4晶体棒,实现了声-光调Q高重复频率窄脉宽1063 nm激光输出。在晶体入射端面总抽运功率约43 W条件下,当重复频率f=10 kHz时,获得脉宽Δt=10.2 ns,单脉冲能量E=0.95 mJ,峰值功率PM=93.1 kW的输出;在重复频率f=100 kHz时,获得Δt=28.1 ns,E=0.10 mJ,PM=3.6 kW的结果。  相似文献   

7.
为了获得高功率、高重频半导体激光脉冲,设计了一种体积小、重量轻、造价低的纳米级大功率半导体激光器驱动电源。采用改进的单稳态触发器产生窄脉冲,经放大后驱动快速开关MOSFET获得大电流窄脉冲;电源脉冲电流驱动能力0A~80A,脉冲上升时间2.8ns,下降时间3.8ns,脉冲宽度5ns~500ns范围内可调,最小5.2ns,重复频率可达200kHz。用该电源实验测试了激光波长为905nm的半导体激光器,在重复频率为10kHz时,激光脉冲峰值功率达到70W以上。结果表明,采用窄脉冲驱动MOSFET可以得到高重复频率10ns以内的大电流窄脉冲,可以驱动大功率半导体激光器,若驱动100A以上的激光器需进一步研究。  相似文献   

8.
A highly efficient and high power green laser generated by intracavity frequency doubling of a diode-sidepumped Q-switched Nd:YAG laser has been demonstrated. In the simple L-shaped cavity geometry,the maximum green output power of 28.5 W was obtained with a pulse width of 95 ns at a pulse repetition rate of 10 kHz by using a LBO crystal for frequency doubling,corresponding to a conversion efficiency of 11% from diode pump power to pulse green power. At a pulse repetition rate of 1 kHz,6.9 mJ of pulse energy,25 ns of pulse duration and 276 kW of peak power were obtained.  相似文献   

9.
为了满足激光推进、光电对抗等应用领域的需要,研制了一台高单脉冲能量高重复频率新型TEA CO2激光器。采用紫外(UV)预电离双路Ernst石墨电极串并联放电结构、超薄水冷不变形镜折叠腔、双回路直冷式封闭循环流动系统和高压大电流快脉冲开关电源等技术,解决了高功率高压电容充电、高气压大体积均匀辉光放电、高气压高速均匀流场、激光谐振腔和高脉冲能量、高重复频率脉冲激光输出等技术难题。成功研制了一台最大脉冲激光能量92 J,重复频率35 Hz,激光输出发散角1.4 mrad,脉冲能量稳定性0.8%,平均功率大于3000 W的脉冲激光器。  相似文献   

10.
By coupling the active laser cavity to a passive low-finesse Fabry-Perot resonator, supermode stabilization of mode-locked Ti:Er:LiNbO3 waveguide lasers for 5- and 10-GHz pulse repetition rates with side mode suppression ratios of 60 and 55 dB has been achieved. The 10-GHz source emits pulses with a pulsewidth of 5.7 ps and a time-bandwidth product lower than 0.52 within an RF frequency tuning range of 3.2 MHz. The 5-GHz source has been used in a 2×5 Gbit/s soliton transmitter. In a back-to-back measurement, a Q-factor of 25.1 dB has been obtained. In soliton transmission experiments over 160 km on a step-index fiber, an extrapolated bit error rate of 6·10 -17 has been measured. The passive cavity can serve also as a pulse repetition rate multiplier. Pulse repetition rate multiplication from 2.5 to 10 GHz has been demonstrated  相似文献   

11.
A power supply specifically designed for capacitor-charging applications that uses a series-resonant circuit topology, a constant on-time/variable frequency control scheme, and zero-current switching techniques has been developed. The performance of this capacitor-charging power supply (CCPS) has been evaluated in the laboratory by charging several values of load capacitance at various repetition rates. The CCPS has charged a 1 μF capacitor from 0 to 1500 V DC in 750 μs, exhibiting a charging power of 1500 J/s. This operation has been repeated at a rate of 800 charges per second, which corresponds to an average power output of 900 W. A 10 μF capacitor has been charged from 0-1500 V DC in 8 ms. These results indicate that this design is feasible for use in capacitor-charging applications  相似文献   

12.
设计了适应于迫弹激光近炸引信的小体积、低电压、窄脉宽、高功率的脉冲半导体激光电源.采用电容充放电的模式,选用高速大功率MOSFET管作为开关,设计了相应的高速开关控制电路.激光电源模块的重复频率高达50kHz,常规热电池供电电压条件下的输出脉冲激光峰值功率为9W,光脉冲上升沿为4.2 ns,光脉宽为10 ns,为有效提...  相似文献   

13.
受激布里渊散射主被动混合调Q光纤激光器   总被引:2,自引:0,他引:2  
邢磊  冯雪  张磊  刘小明 《中国激光》2008,35(3):338-342
基于瑞利散射和受激布里渊散射(RS-SBS)的被动调Q掺铒光纤(EDF)激光器的输出脉冲序列具有重复频率低、脉宽窄、功率高的特点,适合光时域反射(OTDR)系统对脉冲光源的基本要求,但是输出的脉冲序列不够稳定。提出在被动调Q激光腔中插入声光调制器(AOM)构成主被动混合调Q激光器。实验结果证明,这种混合调Q的方法既保持了声光调制器主动调Q激光器输出脉冲序列重复频率低而且稳定的特点,又发挥了瑞利散射和受激布里渊散射被动调Q机制动态速度快、输出脉冲宽度窄的优势。在120~200 mW的抽运功率条件下,得到的脉冲序列重复频率从30 Hz~90 kHz连续可调,脉冲宽度最小可达20 ns,峰值功率最高可达200 W,脉冲重复频率稳定度优于5%,脉冲幅度起伏不大于10%。脉冲峰值功率和脉冲宽度受抽运功率的影响不大,但随着调制频率增加,脉冲峰值功率降低而脉冲宽度加宽。  相似文献   

14.
An output of 1.5 W of average power at 3371 Å is obtained from a pulsed nitrogen laser operating at a repetition rate of 1200 Hz. Pulse powers up to 300 kW are observed, with 10-ns pulse duration. The high repetition rate is made possible through the use of a closed-cycle transverse gas flow system to supply fresh ion-free gas to the laser for each pulse.  相似文献   

15.
为压缩激光声信号的带宽,基于热膨胀激光致声理论提出了一种采用高重频激光脉冲串产生窄带声信号的方法(重频法),推导了最优重复频率的计算过程,并通过实验测量对重频法进行了验证。以声信号在中心频率处的功率谱密度为参考标准,将重频法与长脉冲法产生窄带声信号的性能进行了比较。理论分析与实验结果表明,激光器在最优重复频率下产生的声信号窄带特性最好;最优重复频率与激光波长、光束半径以及观测角有关;激光脉冲数大于10时,重频法的性能优于长脉冲法;脉冲数为100时,在中心频率处重频法的功率谱密度比长脉冲法高9.3dB。  相似文献   

16.
Power and life extension of battery-ultracapacitor hybrids   总被引:1,自引:0,他引:1  
The performance of a battery-ultracapacitor hybrid power source under pulsed load conditions is analytically described using simplified models. We show that peak power can be greatly enhanced, internal losses can be considerably reduced, and that discharge life of the battery is extended. Greatest benefits are seen when the load pulse rate is higher than the system eigenfrequency and when the pulse duty is small. Actual benefits are substantial; adding a 23 F ultracapacitor bank (3 × 7 PC10 ultracapacitors) in parallel with a typical Li-ion battery of 7.2 V and 1.35 A hr capacity can boost the peak power capacity by 5 times and reduce the power loss by 74%, while minimally impacting system volume and weight, for pulsed loads of 5 A, 1 Hz repetition rate, and 10% duty  相似文献   

17.
高重复率窄脉宽Nd:YVO4板条激光器   总被引:4,自引:1,他引:3  
部分端面抽运的混合腔板条激光器是一种新型的全固态激光器,采用这种结构,实现了高重复率调Q运转.在脉冲抽运情况下,1 kHz运转时,得到脉宽4.6 ns,单脉冲能量4.5 mJ的激光输出.在连续抽运调Q输出情况下,5 kHz高重复率运转时,获得了脉宽6 ns,单脉冲能量3.1 mJ的脉冲序列输出,平均功率超过15 W;当重复率高达25 kHz时,得到脉宽9.5 ns,单脉冲能量1.2 mJ的激光输出,平均功率达30 W.实验结果表明,输出水平还有很大的提升空间.  相似文献   

18.
A 1.0 cm long, two contact, monolithic extended-cavity laser has been fabricated and actively mode-locked at a repetition rate of 4.4 GHz to produce 9.0 ps optical pulses. Doubling of the optical pulse repetition rate of 8.8 GHz without changing the sinusoidal drive frequency is achieved by synchronously modulating two separate active regions.<>  相似文献   

19.
CdTe电光调频晶体用于电光调Q研究   总被引:3,自引:0,他引:3  
本文研究了CdTe电光调Q晶体及电光调频晶体的调制特性,报道了采用 CdTe电光调频晶体进行电光调 Q的光栅选支射频激励波导 CO2激光器,调 Q激光脉冲重复频率 1Hz~10 kHz可调,在 10 kHz重复频率时,获得激光脉冲峰值功率为 300 W,脉冲宽度为 150 ns.  相似文献   

20.
We demonstrate a compact and efficient diode-end-pumped TEM00 laser with output power of 25.2 W for 52 W of incident pump power by use of a single YVO4 crystal with a Nd concentration of 0.3 at.%. In Q-switched operation 21-W of average power at a pulse repetition rate of 100 kHz and ~1.1-mT pulse energy at a pulse repetition rate of 10 kHz were produced. At 10 kHz, the pulse width is around 10 ns and the peak power is higher than 100 kW  相似文献   

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