准相位匹配周期极化钼酸钆制备及倍频效应  

Preparation of Periodically Poled Gadolinium Molybdate Crystal for Quasi-Phase-Matching and Its Second Harmonic Generation

作　　者：袁清习[1] 任铁未[2] 徐军[1] 潘守夔[1] 朱永元[2] 祝世宁[2] 

机构地区：[1]中国科学院上海光学精密机械研究所,上海201800 [2]南京大学固体微结构物理国家实验室,南京210008

出　　处：《光学学报》2003年第7期796-799,共4页Acta Optica Sinica

基　　金：国家自然科学基金 (698780 30 )资助课题

摘　　要：根据准相位匹配原理 ,对钼酸钆晶体用于准相位匹配倍频过程的周期性畴结构进行了设计 ,当入射基频光为 1 .0 64μm时 ,所需的钼酸钆晶体畴结构周期为 5 .54μm。利用外电场极化 ,当外电场为 2 .5kV/mm时 ,钼酸钆晶体的畴结构反转时间tc=50 0～ 60 0 μs。当外电场脉冲幅值为 2 .5kV/mm、脉冲延续时间t=0 .6～ 0 .8tc 时 ,在钼酸钆晶体中制备得到了周期畴结构。当Nd∶YAG纳秒激光器输出准连续功率为 7～ 1 0mW的 1 0 64μm激光通过具有周期畴结构的样品时 ,获得了 0 .532According to the theory of quasi-phase-matching (QPM), the periodical domain structure in gadolinium molybdate crystal for QPM second harmonic generation is designed. The designed domain period is 5.54 μm if the fundamental wavelength is 1.064 μm. The periodical domain structure is fabricated via poling the crystal with applied external pulse field. The switching time tc of the crystal is 500-600 μs when the external field is 2.5 kV/mm. The periodical domain structure has been obtained under the conditions that the voltage is 2.5 kV/mm and the duration of the applied pulse is 0.6-0.8 tc. Using the periodically poled sample, harmonic wave of 0.532 μm has been achieved when the power of the fundamental Nd:YAG laser is 7-10 W.

关 键 词：准相位匹配 周期极化 钼酸钆晶体 制备 倍频效应 

分 类 号：O734.1[理学—晶体学]