We calculate the Casimir force between a perfect reflective wall and a semitransparent wall in the laser cavity. Using the Fox–Li quasimode theory to describe the electromagnetic field in the laser cavity, the vacuum...We calculate the Casimir force between a perfect reflective wall and a semitransparent wall in the laser cavity. Using the Fox–Li quasimode theory to describe the electromagnetic field in the laser cavity, the vacuum energy and the Casimir force are calculated. We compare our results to the force in the ideal situation and find it smaller in the dissipative cavity. We also find that the Casimir force decreases with the increase of the wall-wall distance and the decay rate of the quasimodes in the laser cavity.展开更多
采用非稳腔结构的激光器,当系统的菲涅耳数较大时,球面腔镜尺寸随之增大,尽管可以获得高输出功率,但由于不满足傍轴条件,球面腔镜的球差对输出模式的影响变大。采用Fox-Li迭代算法,分析了腔镜类型不同时谐振腔有效菲涅耳数为675的2 k W...采用非稳腔结构的激光器,当系统的菲涅耳数较大时,球面腔镜尺寸随之增大,尽管可以获得高输出功率,但由于不满足傍轴条件,球面腔镜的球差对输出模式的影响变大。采用Fox-Li迭代算法,分析了腔镜类型不同时谐振腔有效菲涅耳数为675的2 k W射频板条CO_2激光器的输出模式,并进行了实验研究。结果表明,当腔镜采用双球面镜时球差的影响显著,输出光束近似为球面波,输出平面上光束质量因子M!2=14.48,光束质量差,聚焦后光束偏离光轴,难以实现高功率、高光束质量的激光输出;当腔镜均采用抛物面镜时球差的影响得以消除,输出光束近似为平面波,此时输出平面上光束质量得到改善,M!2=3.96,实验结果与数值模拟结果一致。展开更多
基金Supported by the National Natural Science Foundation of China under Grant Nos.11175044,11105021,11347190,and 11204028the Natural Science Foundation of Jilin Province,China under Grant No.201115007
文摘We calculate the Casimir force between a perfect reflective wall and a semitransparent wall in the laser cavity. Using the Fox–Li quasimode theory to describe the electromagnetic field in the laser cavity, the vacuum energy and the Casimir force are calculated. We compare our results to the force in the ideal situation and find it smaller in the dissipative cavity. We also find that the Casimir force decreases with the increase of the wall-wall distance and the decay rate of the quasimodes in the laser cavity.
文摘采用非稳腔结构的激光器,当系统的菲涅耳数较大时,球面腔镜尺寸随之增大,尽管可以获得高输出功率,但由于不满足傍轴条件,球面腔镜的球差对输出模式的影响变大。采用Fox-Li迭代算法,分析了腔镜类型不同时谐振腔有效菲涅耳数为675的2 k W射频板条CO_2激光器的输出模式,并进行了实验研究。结果表明,当腔镜采用双球面镜时球差的影响显著,输出光束近似为球面波,输出平面上光束质量因子M!2=14.48,光束质量差,聚焦后光束偏离光轴,难以实现高功率、高光束质量的激光输出;当腔镜均采用抛物面镜时球差的影响得以消除,输出光束近似为平面波,此时输出平面上光束质量得到改善,M!2=3.96,实验结果与数值模拟结果一致。
