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KDP晶体高效二倍频理论计算 总被引:2,自引:0,他引:2
根据三波耦合方程研究了基波功率密度晶体长度,相位匹配类型,相位失配角,离散角等因素对KDP晶体倍频转换效率的影响。给出了不同长度KDP晶体Ⅱ类相位匹配的理论计算曲线,由此选择最佳条件进行实验,获得了80%的倍频转换效率。 相似文献
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本文报导了一种具有精密恒温的角相位匹配KDP二倍频、三倍频系统,其特点是温度恒温控制在40℃,稳定度0,1℃。在大功率输出的Nd:YAG激光器中,实现0.53μm和0.355μm波长的连续稳定运转,其光脉冲能量涨落<±2%。 相似文献
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利用Ⅱ类相位匹配实现稳定倍频输出 总被引:2,自引:0,他引:2
提出利用Ⅱ类相位匹配方法实现稳定倍频输出,并对该方法进行了理论分析和数值模拟。数值模拟是对KTP晶体xy平面内的Ⅱ类相位匹配倍频过程进行的。数值计算结果表明,Ⅱ类相位匹配倍频过程中,当基频光以除最佳入射偏振角之外的偏振方向入射时,倍频强度曲线随倍频晶体长度增加而呈周期性变化;由于这种周期性变化的存在,当基频光起伏变化时,倍频强度曲线会交叉汇聚,出现倍频稳定区;当偏离角(入射偏振角与最佳入射偏振角差值)一定时,随着基频光入射强度的增大,实现稳定倍频输出所需的倍频晶体长度减小,稳定输出时倍频效率不变;当基频光强度一定时,随着偏离角的增大,倍频输出稳定性提高,倍频效率稍有下降。 相似文献
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在对描述Ⅰ类相位匹配倍频过程的耦合波进行分析的基础上,发现不同初始条件下倍频过程中基频光和倍频光强度变化情况不相同。当注入倍频光能量不为零,且初始相位满足一定条件时,能量会在基频光和倍频光中循环交换。利用倍频过程中的这个循环过程,提出在倍频过程中注入倍频种子光(简称倍频注入)以实现稳定的倍频能量输出,并用数值模拟计算结果证明了倍频注入方法的有效性。进一步的数值模拟研究结果表明:倍频注入方法中可以通过改变注入的倍频种子光强和倍频种子光与基频光之间的相对相位来调节实现稳定倍频输出所需的倍频晶体长度。 相似文献
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大功率CO2激光器倍频晶体综述 总被引:1,自引:0,他引:1
介绍了中红外激光的产生方式以及各种中红外激光器的特点。结合CO2激光器倍频产生中红外的优点,重点讨论了CO2激光器倍频晶体的性能。对常用的双折射相位匹配(BPM)倍频晶体和准相位匹配(QPM)倍频晶体性能进行了比较分析。展望了高功率CO2倍频激光器的发展需要解决的问题及可能的技术途径。 相似文献
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1 Introduction In recent years short wavelength coherent radiation lying in th blue and UV range has attracted wide attention for a variety o applications, including laser printing, undersea communicatio etc. In view of this, several studies of nonlinear-… 相似文献
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双轴晶体LiB3O5和KTiOPO4的和频特性 总被引:1,自引:1,他引:0
本文综述了非线性晶体的和频(SFM)特性。对LiB3O5和KTiOPO4中的二次谐波产生(SHG)和SFM进行了数值计算并分析了相位匹配范围,主要的相位匹配参数,最佳相位匹配角θ和Х,有效非线性系数deff,走离角α和允许角△θ和△Х。还讨论了在3个主平面内SFM的偏振特性。 相似文献
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-A discussion of second harmonic generation with imperfect phase matching in the high conversion limit is presented. Phase modulation of the fundamental pulse, dispersion, central frequency wavevector mismatch, and fundamental depletion are included. The results show that even small amounts of phase modulation or central frequency wavevector mismatch can limit harmonic generation and must be considered at high conversion efficiency. Both spatial and temporal phase matching parameters are more restrictive at high conversion efficiency because of the narrowing of the central phase matching peak. If the harmonic conversion process is overdriven, severe distortion of the harmonic and transmitted fundamental pulses can result. Cascade harmonic generation of neodymium laser radiation to 266 nm is presented as an example. 相似文献
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Studies of second harmonic conversion of the 5145-Å line of the Ar II ion laser spectrum into the near UV at 2573 Å are presented. Close to optimum conditions were achieved by utilizing 90° phase matching in ADP and KDP crystals in a low loss focusing cavity. Small absorption losses in the cavity at the second harmonic frequency are presently preventing the realization of the expected theoretical efficiency. 相似文献
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Effect of group velocity mismatch on the measurement of ultrashort optical pulses via second harmonic generation 总被引:2,自引:0,他引:2
The use of second harmonic generation as a technique for optical pulse width measurements is analyzed to determine the effects of both phase velocity and group velocity mismatch between fundamental and second harmonic fields. An expression for the time average second harmonic energy, which except for special cases differs from the intensity autocorrelation function, is derived. For Type I phase matching, the measurement yields an apparent correlation width which can be either shorter or longer than the actual intensity correlation width, depending on the specific pulse shape. When the group velocity mismatch is nonzero, the measurement becomes sensitive to the phase matching condition. Two special pulse shapes for which the measurement is independent of group and phase velocity mismatch are the Gaussian and the single-sided exponential. 相似文献