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 共查询到19条相似文献,搜索用时 109 毫秒
1.
可调谐钛宝石激光抽运的KTP单谐振光学参量振荡器的研究   总被引:2,自引:0,他引:2  
介绍了 70 0nm~ 980nm的脉冲可调谐钛宝石激光抽运的KTP单谐振光学参量振荡器。通过改变抽运光波长作为光学参量振荡器输出参量光的调谐方式 ,确定了KTP晶体最佳切割角度 (θ=6 2 .5°,φ =0°) ,实验上获得了 12 5 1nm~ 2 5 32nm的连续参量光输出 ,最大输出能量约为 2 7 2mJ,最大转换效率为 35 7% (1311nm处 )。  相似文献   

2.
田宏宾  王丽 《光子学报》2007,36(8):1495-1499
基于周期极化晶体的Sellmeier方程和准相位匹配理论,对准相位匹配光参变振荡器的调谐特性进行了理论分析.通过数值模拟计算,得到了PPRTA晶体光参变振荡的调谐特性与极化反转光栅周期、晶体温度和抽运光波长等参量的关系曲线.并且与PPKTP晶体和PPLN晶体光参变振荡器的调谐特性进行了比较,研究了三者的不同之处,得出了PPRTA晶体的参量调谐特性优于PPKTP晶体和PPLN晶体的结论,与国外已报道的实验数据相吻合.证实了PPRTA晶体是一种可以产生可调谐近中红外光的理想准相位匹配非线性光学晶体.  相似文献   

3.
脉冲内腔光学参变振荡器的研究   总被引:4,自引:0,他引:4  
柳强  王月珠  姚宝权  王骐 《光学学报》2001,21(10):228-1233
对于腔内含有KTP光学参变振荡器的调Q Nd:YAG激光振荡器,利用简单的内腔光学参变振荡器动力学模型,用瞬态耦合波方程求解了抽运激光介质反转粒子数,抽运动率和信号光功率的时间演变特性,结果显示对于不同的抽运水平和光学参变振荡谐振腔结构,内腔光学参变振荡器可以产生一个或者多个信号光脉冲,实验中,通过改变谐振腔输出镜的反射率,得到了单个和多个信号光脉冲,实验结果与理论分析相吻合,最后还分析了内腔光学参变振荡器输出的能量和调谐特性。  相似文献   

4.
朱雅琛  兰戈  李彤  牛瑞华  任钢 《光学学报》2007,27(11):2059-2063
为了验证KTiOAsO4(KTA)晶体用于光参变振荡产生2μm激光的可行性,设计了脉冲式2μm KTA光参变振荡器,采用θ=49°切割的KTA晶体作为光参变振荡晶体,实现了2μm激光的输出;计算了该系统在双谐振情况下的起振阈值,在实验中测得输出的信号光、闲频光波长在2.16μm和2.09μm附近,与理论计算基本吻合,并测量了脉冲宽度。同时选用了对信闲光透过率分别为60%、70%、90%的镜片作为光参变振荡器(OPO)输出镜,测得了三种情况下的输出能量及电光效率的数值;测得了在380 V电压下,输出镜透过率一定时输出能量与光参变振荡器腔长之间的关系曲线,从而验证了KTA晶体用于光参变振荡产生2μm激光的可行性,为下一步的研究工作打下了基础。  相似文献   

5.
郭靖  何广源  焦中兴  王彪 《物理学报》2015,64(8):84207-084207
报道了一种高效率的2 μm光学参量振荡器. 利用1.064 μm声光调Q Nd:YVO4激光器抽运基于氧化镁掺杂周期性极化铌酸锂的内腔式光学参量振荡器, 在简并状态实现了稳定高效的2 μm激光输出. 当808 nm激光二极管抽运功率为20 W, Q开关工作频率为15 kHz时, 产生了平均功率为3.5 W、脉冲宽度为1.4 ns的2 μm激光, 光-光转换效率为17.5%, 斜效率为25%. 据我们所知, 该转换效率在2 μm波段内腔式光学参量振荡器中是最高的.  相似文献   

6.
采用电光调Q脉冲Nd∶YAG激光的二次谐波 (5 32nm)抽运温度调谐的MgO∶LiNbO3晶体光学参量振荡器 ,调谐范围达 80 0nm~ 175 0nm。在单谐振运转条件下 ,抽运阈值为 2 1.5mJ/ pulse ,最大抽运能量为 5 8mJ时输出为 6 .45mJ ,在大信号情况下的能量转换效率达 11% ,输出线宽 1nm左右。  相似文献   

7.
高性能85mm短腔光学参变振荡器的THz电磁波输出特性分析   总被引:5,自引:0,他引:5  
报道了以MgO∶LiNbO3为非线性光学介质,采用85 mm长的法布里珀罗单谐振腔结构形式的光学参变振荡器,产生THz电磁波的实验结果。使用波长为1064 nm的Nd∶YAGQ开关脉冲激光器作为抽运光源,通过改变入射角度使参变振荡器的相位匹配条件发生变化。采用Si真空量热器,并利用THz波干涉测量仪;或通过测量闲频光的频率对产生的THz波频率进行了测量。实验表明该参变振荡器输出频率调谐范围为0.9~3.0 THz。在抽运光能量为20 mJ/pulse,脉冲宽度16 ns,重复频率50 Hz条件下得到输出峰值位于1.2 THz,能量为102.5 PJ/pulse的THz波输出。通过引入Si棱镜阵列减小了THz波在晶体中的全反射,从而提高THz波的能量输出。使用金属缝隙探测器,对辐射的THz波的波束水平方向空间分布进行了测量,分析了Si棱镜阵列的衍射效应对THz波束空间分布的影响。  相似文献   

8.
BiB_3O_6纳秒光参变振荡器   总被引:2,自引:1,他引:1  
采用电光调Q脉冲Nd:YAG固体激光器的532 nm绿光作为抽运光源(10~13 ns,0~20 mJ),以Ⅱ类相位匹配(θ=57.5°Φ=0°)、尺寸为4 mmX 4 mm×12 mm的三硼酸铋晶体(BiB3O6)与一对1215 nm单谐振波长的平镜组成腔长为40 mm的谐振腔,构建了光参变振荡器的整个实验系统.系统将入射抽运光振荡产生1215 nm的信号光及946 nm的闲频光,结果显示,抽运阈值为9 mJ,最高耦合输出为2.57 mJ,抽运脉冲能量与信号脉冲能量的最高转换效率为14.59%.  相似文献   

9.
宽波段温度调谐MgO:LiNbO3光学参量振荡器   总被引:1,自引:1,他引:0  
吕卫  于意仲等 《光学学报》2001,21(4):40-443
采用电光调Q脉冲Nd:YAG激光的二次谐波(532nm)抽运温度调谐的MgO:LiNbO3晶体光学参量振荡器,调谐范围达800nm-1750nm.在单谐振运转条件下,抽运阈值为21.5mJ/pulse,最大抽运能量为58mJ时输出为6.45mJ,在大信号情况下的能量转换效率达11%,输出线宽1nm左右。  相似文献   

10.
基于周期性极化铌酸锂晶体(PPLN)的准相位匹配光参变放大过程,通过倾斜周期极化铌酸锂晶体中极化域(极化光栅)一定角度,实现了介于共线匹配方式和非共线匹配方式之间的一种半非共线型准相位匹配方式,并以该匹配方式下的各光矢量几何关系得出相位匹配曲线,找到在特定抽运光和信号光波长下能获得宽带增益放大的周期极化长度。并研究其极化倾斜角度与温度特性。模拟计算表明,在合适的角度与温度条件下,该方式可以532 nm抽运光抽运的信号光在800 nm和1064 nm处均获得宽带光参变放大。  相似文献   

11.
We report a continuous-wave optical parametric oscillator (OPO) based on periodically poled RbTiOAsO(4) (PPRTA). The singly resonant OPO, which is located within a Ti:sapphire laser, has a high-finesse signal cavity and delivers a maximum output power of 270 mW to the nonresonant idler wave at 2.92mum , through a 4.5-mm PPRTA crystal. For room-temperature operation and a crystal with a 30-mu;m grating period, pump tuning over 838-848 nm results in OPO tuning over 1.13-1.27mum (signal) and 2.53-3.26mum (idler), limited by the bandwidth of optical coatings. PPRTA exhibits thermal properties superior to those of periodically poled LiNbO(3) .  相似文献   

12.
We demonstrate that the threshold for a mid-IR optical parametric oscillator based on periodically poled LiNbO3 is significantly reduced by the introduction of an optical amplifier inside the cavity. Thresholds as low as 8 mW and a tuning range of 3.0-4.2 microm were attained for stable single-mode operation.  相似文献   

13.
We describe a synchronously pumped femtosecond optical parametric oscillator based on periodically poled LiNbO(3) that is broadly tunable in the mid infrared. A transmission window of periodically poled lithium niobate beyond the conventionally accepted infrared absorption edge of 5.4 mum has been exploited to produce idler pulses that are tunable across a wavelength range of 4 mum , with milliwatt-level output powers at wavelengths as long as 6.8 mum . We also present experimental tuning results that are in good agreement with the theoretical phase matching predicted from published infrared-corrected Sellmeier equations for LiNbO(3) .  相似文献   

14.
郑雄桦  张宝夫  焦中兴  王彪 《中国物理 B》2016,25(1):14208-014208
We present a continuous-wave singly-resonant optical parametric oscillator with 1.5% output coupling of the resonant signal wave, based on an angle-polished Mg O-doped periodically poled lithium niobate(Mg O:PPLN), pumped by a commercial Nd:YVO4laser at 1064 nm. The output-coupled optical parametric oscillator delivers a maximum total output power of 4.19 W with 42.8% extraction efficiency, across a tuning range of 1717 nm in the near- and mid-infrared region.This indicates improvements of 1.87 W in output power, 19.1% in extraction efficiency and 213 nm in tuning range extension in comparison with the optical parametric oscillator with no output coupling, while at the expense of increasing the oscillation threshold by a factor of ~ 2. Moreover, it is confirmed that the finite output coupling also contributes to the reduction of the thermal effects in crystal.  相似文献   

15.
We present a cw, Nd:YAG-pumped singly resonant single-frequency narrow-linewidth high-power optical parametric oscillator with idler tuning from 3.7 to 4.7 microm. In this spectral range the absorption of the idler wave in the LiNbO3 crystal is significant, causing the oscillation threshold to increase with a subsequent decrease in output power from 1.2 W at 3.9 microm to 120 mW at 4.7 microm. The optical parametric oscillator's cavity was stabilized and mode-hop tuned with a rotatable solid etalon but with a subsequent reduction in idler power of as much as 50%. We demonstrated the usefulness for spectroscopy by recording the photoacoustic spectrum of a strong CO2 absorption, using a 24-GHz continuous idler scan.  相似文献   

16.
本文首先阐述光参量振荡器的调谐原理及其温度调谐的计算.接着讨论研制光参量振荡器的若干技术问题.最后给出信号单谐光参量振荡的实验结果.波长谐范围为1.3—2.0μm.当波长调谐到1.9μm且工作重复率为10PPS时,输出能量为0.37mJ/脉冲.  相似文献   

17.
We describe a compact all-solid-state continuous-wave singly resonant optical parametric oscillator (SRO) with a minimal pump-power requirement. The SRO is based on periodically poled LiNbO(3) as the nonlinear material and is pumped by a 1-W diode-pumped Nd:YVO(4) minilaser at 1.064 microm . By exploiting the intracavity pumping technique in a 50-mm crystal, we have achieved SRO operation threshold at a diode pump power of only 310 mW.At 1 W of input diode power, the SRO delivers 70 mW of output power in the nonresonant idler at 3.66 microm , at a photon conversion efficiency of 55%. Multiparameter tuning of the SRO yields a signal wavelength range from 1.45 to 1.60 microm and an idler wavelength range from 3.16 to 4.02 microm in the mid infrared. The device is characterized by robust turnkey operation and long-term amplitude-stable performance.  相似文献   

18.
微微秒自动调谐参量激光的研究   总被引:3,自引:3,他引:0  
何慧娟  陆雨田 《光学学报》1991,11(6):25-530
采用一对MgO:LiNbO_3角度调谐覆盖了红近外波段0.7~2.2μm,并配以自动波长扫描。文中分析了影响脉冲宽度与线宽的因素,与实验结果相吻合。脉宽<30ps,线宽~1nm(简并波长附近~10nm),单脉冲峰功率达MW级,参量光总能量转换效率达5.4%。  相似文献   

19.
We demonstrate an optical parametric chirped-pulse amplifier producing infrared 20 fs (3-optical-cycle) pulses with a stable carrier-envelope phase. The amplifier is seeded with self-phase-stabilized pulses obtained by optical rectification of the output of an ultrabroadband Ti:sapphire oscillator. Energies of -80 microJ with a well-suppressed background of parametric superfluorescence and up to 400 microJ with a superfluorescence background are obtained from a two-stage parametric amplifier based on periodically poled LiNbO3 and LiTaO3 crystals. The parametric amplifier is pumped by an optically synchronized 1 kHz, 30 ps, 1053 nm Nd:YLF amplifier seeded by the same Ti:sapphire oscillator.  相似文献   

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