准相位匹配周期极化高掺镁铌酸锂532 nm倍频准连续输出研究

对周期性极化高掺镁铌酸锂倍频过程进行了准相位匹配倍频理论研究。在室温下通过外加电场极化法,用较低的极化开关电场～5．5kV／mm,在厚为1mm、长为10mm、宽为10mm的掺镁铌酸锂基片上成功地制备了周期为5．8～7．3pm(间隔0．3pm)的一阶准相位匹配倍频周期性极化光学微结构。将温度控制在70℃左右,以波长为1．060μm的Nd：YAG激光为基频光源,对所研制的光学微结构样品进行倍频通光实验验证。当入射基频光为920mW时,可以获得约15mW的532nm准连续倍频蓝光输出．其归一化转换效率高达1．77％／W。     

准相位匹配PPKTP晶体连续倍频13 mW绿光输出

采用高压脉冲电场极化,通过电光效应实时监控、倍频通光二维监控等手段的应用,制备出周期为9μm、长为8 mm、宽为3 mm、厚为1 mm的周期极化KTiOPO4晶体(PPKTP);倍频通光实验中,当波长1064 nm的基频光功率为1 W时,得到了功率为13.5 mW的532 nm连续倍频绿光输出,单通倍频转换效率为1.35%,归一化转换效率为1.69%/(W.cm),接近理论最大值。     

基于单块周期极化铌酸锂晶体级联三倍频的440 nm蓝光固体激光器

阐述了一种基于单块周期极化铌酸锂晶体级联三倍频实现440 nm蓝光输出的实验方案。根据周期极化铌酸锂晶体的Sellmeier方程以及倍频与和频的相位匹配条件,在一块周期极化铌酸锂晶体上设计了两段不同的极化周期,使其在同一工作温度下能分别实现倍频与和频,在先后经过倍频与和频后,实现级联三倍频输出。实验采用Nd: YAG产生的1319 nm光作为基频光,重频400 Hz,脉宽110 ns,横向和纵向光束质量因子分别为1.81和2.65。耦合进周期极化铌酸锂晶体后,出射光中检测到660 nm的红光和440 nm的蓝光。通过调整工作温度和入射基频光功率,得到2.4 mW的最大蓝光输出,此时工作温度55.5 ℃,基频光功率530 mW。实验结果验证了单块晶体实现级联三倍频440 nm蓝光输出的可行性。     

低阈值温度调谐PPMgLN红外光参量振荡

研究了温度调谐下周期极化镁掺杂铌酸锂晶体的红外光参量振荡特性。采用外电场短脉冲极化技术,在大小为7.0mm×50.0mm×1.0mm的Z切高镁掺杂(摩尔分数0.05)铌酸锂上制备出了准相位匹配光学微结构器件,极化周期为30.0μm。以输出波长为1064nm的声光调QNd:YAG固体激光器作为基频泵浦光开展了光参量振荡研究。实验表明:泵浦该PPMgLN晶体,实现了室温下低阈值红外光参量振荡产生,阈值功率仅为45mW(重复频率1kHz)。在泵浦输入功率为225mW时,有36mW信号光输出,转换效率达到16.0%,通过调谐晶体温度(20~180℃),获得了调谐范围为1503~1550nm波段的OPO信号光,实现了低阈值可调谐红外光的稳定输出。     

分段小信号近似方法研究准相位匹配倍频效率

从PPLN波导微结构出发分析准相位匹配倍频过程中的相位补偿机理,以极化畴为单元,通过耦合波方程计算极化畴内产生的二次谐波电场,通过电场相干叠加计算倍频效率。分别在小信号近似和基频光高消耗情况下计算准相位匹配倍频效率,结果显示：倍频效率小于5％时,两种情况下的计算结果吻合得很好;随着转换效率增大,小信号近似不再适用,需要在基频光高消耗情形下计算倍频效率。研究了基频光功率密度与准相位匹配倍频效率的关系,定性分析了极化周期存在误差时,误差对倍频效率的影响。     

基于周期极化化学计量比掺氧化镁钽酸锂晶体的高效率、单程、连续外腔倍频

利用长度为20mm的周期极化化学计量比掺氧化镁钽酸锂晶体（PP-MgO: SLT），实现了转换效率为11.8%的单程连续外腔准相位匹配（QPM）倍频，此时1064nm基频光的输入功率为7.69W，获得的532nm倍频光的输出功率为905mW。实验中可以发现，在不同的基频光聚焦条件和输入功率下，对应最大倍频输出的晶体温控炉的设定温度也要随之改变。此外，对允许角和允许温度也进行了研究，实验结果和理论结果符合的很好。     

准相位匹配扇形光栅铌酸锂光波导倍频绿光输出

采用外加电场极化方式对具有扇形光栅的 0 .5mm厚Z切铌酸锂晶体进行极化反转 ,制成了退火质子交换光波导。极化反转周期为 5 .8μm～ 6 .2 μm ,采用Nd∶YAG激光器输出的 1.0 6 4 μm连续激光为基频光波 ,实现了0 .5 32 μm倍频绿光输出 ,相互作用长度为 4mm ,耦入波导的基频光波功率为 10mW ,获得了 2 0 μW的绿色倍频光输出 ,归一化转换效率为 12 5 % (W·cm2 )。     

基于半整块谐振腔的426nm高效倍频光的产生

通过内置周期极化磷酸氧钛钾晶体的半整块谐振腔,采用铯原子D2线的抽运光实现了426nm的蓝光倍频输出。实验采用了相对松散的聚焦,明显改善了基频光和倍频光吸收诱发的热效应。采用305 mW的模式匹配基频光,获得了117.2mW的倍频蓝光,倍频过程中最高光-光转化效率达到42%;84.5mW蓝光在约1h内的功率起伏为0.48%。结果表明,所提方法可实现倍频光的稳定输出,在量子光学、光与物质相互作用等领域具有广阔的应用前景。     

PPLT倍频宽线宽掺镱双包层光纤放大激光

分别通过理论和实验研究了周期性极化的钽酸锂（PPLT）倍频宽线宽准连续掺镱双包层光纤放大激光.PPLT样品长为40 mm,极化周期为7.67 μm.基频光的中心波长为1064 nm,线宽约为6 nm.从基频光的光谱特性出发,利用超晶格倍频理论,解释了实验中获得的倍频温度与二次谐波功率之间的关系.在基频光的功率为2.2 W时,获得的宽线宽光纤激光倍频效率为1.8%.     

周期极化KTiOPO4晶体连续倍频绿光输出

采用外加电场极化方法，在Z切1mm厚的KTiOPO4晶体中实现了周期性极化反转。晶体的极化反转周期为9．0／μm，相互作用长度为3mm。波长为1．064μm的基频光功率为900mW，晶体中心温度为32℃时，获得0．532μm、22μW的倍频绿光输出，二次谐波转换效率为0．0024％。     

低电场周期极化化学比掺镁铌酸锂绿光倍频器

对气相平衡扩散输运工艺制备的化学比掺镁铌酸锂晶体进行周期极化,实验中发现化学比掺镁铌酸锂晶体的矫顽场为12kV/mm,只有常用的同成分铌酸锂晶体的矫顽场的1/20,用低电场就可以制备出结构均匀周期为62～64μm的周期性极化结构.在室温下对此周期极化结构进行二次谐波倍频实验,其归一化倍频转换效率为48%/W。     

Room-temperature, continuous-wave 1-W green power by single-pass frequency doubling in a bulk periodically poled MgO:LiNbO3 crystal

Continuous-wave high-power green light generation at room temperature is reported in a single-pass frequency-doubling configuration with bulk periodically poled MgO:LiNbO3 crystal placed outside a diode end-pumped Nd:GdVO4 laser. The MgO:LiNbO3 samples of 6.95-microm domain period, uniform periodicity, and 50% duty cycle along the entire crystal length are fabricated by use of a high-voltage multipulse poling method. A maximum power of 1.18 W at 531 nm with 16.8% conversion efficiency is obtained from a 2-mm-thick, 25-mm-long MgO:LiNbO3 crystal; the corresponding internal green power and conversion efficiency are 1.38 W and 19.6%, respectively, whereas the normalized conversion efficiency is 3.3%/W.     

基于耦合场量子受激拉曼散射的太赫兹波辐射

使用两块长度各为65 mm的MgO:LiNbO3和无掺杂LiNbO3晶体,以1064nm的Q开关Nd:YAG激光器作为抽运光源,在12 mJ/pulse的抽运光能量下得到频率范围为0.34～2.90 THz的电磁辐射.分析表明,激光入射使LiNbO3晶体中具有电磁特性的横光学声子可以和入射光子形成耦合场量子.作为一种电磁特性的元激发,LINbO3晶体的耦合场量子的辐射场频率覆盖部分太赫兹频段范围,并可通过耦合场量子受激拉曼散射过程辐射THz波.根据耦合场量子辐射理论,通过分析晶体的耦合场量子色散特性曲线,可以确定该晶体能否辐射THz波及其带宽范围.     

600 mW optical output power at 488 nm by use of a high-power hybrid laser diode system and a periodically poled MgO:LiNbO3 bulk crystal

600 mW second-harmonic blue light at 488 nm has been generated by use of a master-oscillator power amplifier diode laser system as a pump source with a maximum optical output power of 4 W in continuous-wave operation. For frequency doubling, a periodically poled MgO:LiNbO3 bulk crystal was used in a single-pass configuration. A conversion efficiency of 15% and an overall wall-plug efficiency of 4% were achieved.     

Generation of 520 mW pulsed blue light by frequency doubling of an all-fiberized 978 nm Yb-doped fiber laser source

Pulsed blue light at 489 nm has been generated by second-harmonic-generation of a nanosecond pulsed master-oscillator power amplifier system based on a short Yb(3+) doped single-mode fiber amplifier at 978 nm and an external-cavity diode laser as seed source. The Yb(3+)-doped fiber was core-pumped by a W type Nd(3+) doped double-clad fiber laser operating on the transition near 930 nm ((4)F(3/2)→(4)I(9/2)). 520 mW of average power was generated at 489 nm using a periodically poled MgO:LiNbO(3), corresponding to a conversion efficiency of 34%.     

Efficient green-light generation by proton-exchanged periodically poled MgO:LiNbO3 ridge waveguide

Efficient cw 532?nm green-light generation is demonstrated using a periodically poled MgO:LiNbO3 ridge waveguide prepared by a process that combines annealed proton exchange and precise dicing. Performance of waveguides with different widths has been investigated. The 6-μm-wide, 1.6-cm-long uncoated ridge waveguide has achieved a green output power of 127?mW under a coupled fundamental light power of 250?mW. The highest conversion efficiency achieved is 53%.     

Generation of 360-nm ultraviolet light in first-order periodically poled bulk MgO:LiNbO3

Ultraviolet second-harmonic generation in first-order periodically poled MgO:LiNbO3 is presented. Using a high-voltage multipulse application method, we fabricated a first-order nonlinear grating with a period of 1.8 microm and depth of approximately 150 microm over 10-mm interaction length in a 1-mm-thick MgO:LiNbO3 substrate. In a single-pass configuration, continuous-wave 30-mW UV light at 362.5 nm was generated for a fundamental power of 522 mW, corresponding to a normalized conversion efficiency of 11%/W.