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1.
以电光调Q的Nd:YAG激光器为泵浦源,以磷酸氧钛钾(KTP)为非线性晶体,搭建了调谐范围为750~800 nm的光参量振荡器。信号光在中心波长780.2 nm处获得单脉冲能量113 mJ、脉宽15.43 ns、光斑直径5.5 mm的输出。用光栅单色仪测量信号光光谱宽度(FWHM)为0.38 nm。信号光通过120 ℃的铷蒸气池,观察到清晰的荧光轨迹。证明信号光能有效泵浦铷蒸气,可为铷激光器提供峰值功率7 MW的高强度脉冲泵浦源,进而研究铷激光器在高强度泵浦条件下的动力学过程和基础物理机制。  相似文献   

2.
用Raman散射研究了四方钽铌酸钾单晶的顺电 铁电结构相变,在相变时发现和分析了一个凝聚的软晶格振动模v5,它是产生于O2 O3键的对称弯曲振动。  相似文献   

3.
郭锐  杨文海  郭咏  姚慧 《光学学报》2023,(10):255-260
通过实验和理论研究连续变量高功率明亮压缩态光场制备实验中高功率种子光注入光学参量放大器引起的绿光诱导红外吸收效应。首先,通过优化实验系统工作参数,提升反馈控制回路的锁定稳定性,当种子光功率为500 mW、泵浦光功率为145 mW时,在分析频率为3 MHz处,获得光功率为200μW、压缩度为(-10.7±0.2) dB的明亮压缩态光场。然后,根据实验数据,定量分析高功率明亮压缩态光场与压缩真空态光场产生过程中周期极化磷酸氧钛钾晶体的吸收损耗,发现高功率明亮压缩态光场实验系统的总光学损耗为(9±0.05)%,其中由周期极化磷酸氧钛钾晶体吸收导致的内腔损耗为(5.8±0.05)%,占总光学损耗的(64.4±0.05)%。该条件下周期极化磷酸氧钛钾晶体对高功率明亮压缩态光场的吸收系数为(6.0±0.05)×10-2 cm-1。当泵浦光单独注入光学参量放大器时,周期极化磷酸氧钛钾晶体对压缩真空态光场的吸收系数约为2.1×10-4 cm-1。由此可知,当高功率种子光注入光学参量放大器时,绿光诱导红外吸收效应使周...  相似文献   

4.
对基于KTA(KTiOAsO4,砷酸钛氧钾)晶体的中红外2μm光参量振荡器的输入镜膜层损伤现象进行了初步分析及对比实验研究,表明薄膜缺陷导致的热效应是造成输入镜膜层损伤、抗损伤阈值低的主要原因,同时发现由于腔镜失调等原因造成的腔内残余1.06μm激光是造成膜层损伤的主要来源,这些结果对改进光参量振荡器系统设计、进一步提高2μm激光输出能量具有一定的指导作用。  相似文献   

5.
我们在实验中演示了520nm单频绿光泵浦的基于周期极化磷酸钛氧钾(PPKTP)晶体的780nm+1560nm双共振光参量振荡器,高效制备780nm+1 560nm连续可调谐双色下转换光场。该参量振荡器可输出93.3 mW的1 560nm单频激光和44.6mW的780nm单频激光。通过改变PPKTP晶体的温度所得到的波长粗调范围为:信号光1 529.81nm~1 573.83nm(~44nm),闲置光788.26nm~777.20nm(~11nm);通过连续调谐520nm泵浦激光频率初步得到的闲置光在780.24nm(铷原子D2线)处频率连续调谐范围约1.6GHz。  相似文献   

6.
本文利用周期极化磷酸氧钛钾晶体构成的光学参量振荡器实验制备了光通信波段1.34μm纯度为0.993的真空压缩态光场,压缩态光场的压缩度为2.98dB、反压缩度为3.04dB。高纯度的真空压缩态光场可为制备光通信波段高保真度的薛定谔猫态提供量子光源。  相似文献   

7.
频率稳定度是铷原子频标最重要的性能指标. 铷频标频率稳定度主要由原子鉴频信号的信噪比决定. 本文分析了微波腔的结构、铷光谱灯的光谱纯度和同位素滤光方案对信噪比的影响,指出采用模式优越、微波填充因子大的微波腔,光谱纯度高的铷光谱灯,用分离滤光方法进行同位素滤光,可以提高铷原子鉴频信号的信噪比,从而使铷频标的稳定度指标得到进一步改善.   相似文献   

8.
从理论上讨论了一阶和二阶斯托克斯与反斯托克斯拉曼散射截面的温度依赖关系;在293K至401K的温度范围内,测量了BaTiO3单晶斯托克斯和反斯托克斯过程的偏振拉曼光谱;通过对BaTiO3单晶斯托克斯和反斯托克斯拉曼光谱的综合分析,证实在X(ZZ)Y几何配置下测量到的位于275和514cm-1处的强峰为一阶拉曼光谱。此结果支持了BaTiO3铁电相变机制的有序—无序模型。  相似文献   

9.
周期极化KTP晶体光参量振荡特性研究   总被引:11,自引:6,他引:5  
桑梅  薛挺  于建  倪文俊  于云翔  李世忱 《光子学报》2003,32(11):1286-1290
基于较新的Sellmeier方程,研究了周期极化钛氧磷酸钾(KTiOPO4简称KTP)晶体光参量振荡的容差特性,给出了极化反转光栅周期、晶体温度及泵浦光波长的调谐曲线和带宽的容差特性曲线,并与PPLN晶体作了比较数值计算结果与已有实验数据吻合较好.  相似文献   

10.
KTP晶体—第二代光纤通信的重要材料   总被引:1,自引:0,他引:1  
黄朝恩 《物理》1991,20(5):270-273
磷酸氧钛钾(简称KTP)晶体是一种综合性能优异的非线性光学晶体.它的电光系数大,介电常数小,这就使它在集成光学中有着巨大的潜在用途.本文着重介绍KTP的电光及介电性能,其波导的制作方法,以及在光纤通信中的可能应用.  相似文献   

11.
Rudd JV  Law RJ  Luk TS  Cameron SM 《Optics letters》2005,30(15):1974-1976
We have designed and built a chirped-pulse parametric-amplifier system that utilizes a 10 Hz, 300 ps, Nd:YAG pump laser system; a 1.575 microm fiber oscillator and amplifier as the signal source; and rubidium titanyl phosphate and potassium titanyl arsenate nonlinear crystals. We obtained 260 fs, 30 mJ pulses centered at 1.550 microm, representing a gain of > 10(9) and a peak power of 100 GW. To our knowledge, these are the highest energy and peak power pulses ever produced in the 1.5-2.0 microm region  相似文献   

12.
13.
LD泵浦Nd:YVO4/KTP/BBO紫外激光器   总被引:3,自引:0,他引:3  
本文报道在国内首次实现的LD泵浦的四倍频连续紫外激光器的实验结果.首先研究了LD泵浦的Nd:YVO4激光器,在普通平-平腔结构下,得到斜效率55.68%,激光输出波长1064nm;利用KTP作为倍频晶体,实现腔内倍频,在泵浦功率11.85W时得到绿光(532nm)输出1.35W,光-光转换效率11%;用BBO晶体进行外腔谐振倍频,得到紫外光(266nm)输出.  相似文献   

14.
The molybdenum (Mo) and ferric (Fe) doped potassium titanyl phosphate (KTP) crystals were grown by high temperature solution growth (HTSG) technique. The concentration of Mo and Fe in grown crystals was measured by EDX analysis. The SHG efficiencies of the Mo and Fe doped KTP crystals were measured and it was found to be 1.77 and 1.38 times respectively higher than that of pure KTP crystal. The frequency dependence of dielectric constant, loss and ac conductivity was studied at room temperature. The phase matching measurements were made using a Q-switched Nd:YAG laser operating at 1064 nm and the measured phase matching angles are 44.2° and 87.88° for Mo and Fe doped KTP crystals respectively.  相似文献   

15.
We report what we believe to be the first use of a multilongitudinal-mode frequency-doubled microchip laser to pump a doubly resonant optical parametric oscillator (OPO). This compact OPO is based on potassium titanyl phosphate (KTP) and operates with a low pump power threshold of 35 mW. The OPO output consists of a single pair of signal and idler modes even though it is pumped with a multilongitudinal-mode pump laser. We achieved smooth tuning (1.7 GHz) of the output frequencies by temperature tuning of the pump laser.  相似文献   

16.
This paper presents the experimental results of degenerate optical parametric generation using a high gray track resistant potassium titanyl phosphate (HGTR KTP) optical parametric oscillator (OPO). An average output power of 7 W at 10 kHz has been achieved that includes both signal and idler powers near degeneracy using 20 W average power from a 1064 nm Nd:YVO4 pump source corresponding to an optical conversion efficiency of 35%.  相似文献   

17.
Frequency doubling and tripling of a Nd:YAG laser has been studied in a rubidium dihydrogen arsenate (RDA) crystal. An overall power conversion efficiency of 34% and 12% has been obtained for doubling and tripling, respectively. Some comparison with rubidium dihydrogen phosphate (RDP) crystal is reported for the generation of the third-harmonic radiation at 3547 Å.  相似文献   

18.

High-efficiency non-linear crystals suitable for the generation of coherent sources ranging from the deep ultraviolet to mid-infrared (0.16 to 5 µm) are explored. The key parameters for frequency conversion techniques (second-harmonic-generation, sumfrequency mixing, difference-frequency mixing, optical parametric oscillation (OPO) and stimulated Raman scattering) including tunability, beam quality, beam walk-off and the effective figure-of-merit are analysed. Materials selection rules for non-linear crystals (for wide transparency, high damage threshold, stability, low absorption and large figure-of-merit) are presented. Techniques using non-critical phase-matching, quasi-phase-matching, waveguided doubling and self-frequency doubling are explored. Features and applications of the new non-linear crystals ofβ-barium borate, lithium triborate (LBO), potassium titanyl phosphate (KTP), KNbO3 and MgO:LiNbO3 are presented and compared with other crystals. In addition to a critical review, this paper also presents some new results for the analysis of frequency-conversion efficiency, experimental data of OPO in KTP, LBO for frequency conversion using temperature-tuned non-critical phase-matching and green lasers from the diode-pumped self-frequency-doubling crystal of neodymium yttrium aluminium borate.

  相似文献   

19.
High-efficiency non-linear crystals suitable for the generation of coherent sources ranging from the deep ultraviolet to mid-infrared (0.16 to 5 µm) are explored. The key parameters for frequency conversion techniques (second-harmonic-generation, sumfrequency mixing, difference-frequency mixing, optical parametric oscillation (OPO) and stimulated Raman scattering) including tunability, beam quality, beam walk-off and the effective figure-of-merit are analysed. Materials selection rules for non-linear crystals (for wide transparency, high damage threshold, stability, low absorption and large figure-of-merit) are presented. Techniques using non-critical phase-matching, quasi-phase-matching, waveguided doubling and self-frequency doubling are explored. Features and applications of the new non-linear crystals of-barium borate, lithium triborate (LBO), potassium titanyl phosphate (KTP), KNbO3 and MgO:LiNbO3 are presented and compared with other crystals. In addition to a critical review, this paper also presents some new results for the analysis of frequency-conversion efficiency, experimental data of OPO in KTP, LBO for frequency conversion using temperature-tuned non-critical phase-matching and green lasers from the diode-pumped self-frequency-doubling crystal of neodymium yttrium aluminium borate.  相似文献   

20.
Chen YF 《Optics letters》2005,30(4):400-402
A potassium titanyl phosphate crystal is used to achieve efficient stimulated Raman scattering conversion with simultaneous self-sum frequency mixing and self-frequency doubling. Inside a diode-pumped Nd:YAG Q-switched laser cavity, 1.03 W of 1129-nm second Stokes average output power and 0.25 W of 548-nm sum-frequency average power are simultaneously generated with a diode input power of 10 W at a pulse repetition rate of 10 kHz.  相似文献   

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