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为解决四波混频法测量光纤非线性系数未考虑泵浦消耗而导致结果不准确的问题,提出了一种在简并四波混频情况下测量非线性系数的方法.根据光纤中简并的四波混频理论,推导出了考虑泵浦消耗和光纤损耗的椭圆方程.通过设定数值计算所需的各个参量并利用简单的数学方法分析了计入泵浦消耗、光纤损耗的必要性,得到被测光纤的非线性系数,与Optisystem的仿真结果一致.研究表明,这种改进的测量方法不但适用于小信号情形下的四波混频过程,还可以应用于出现参量饱和现象的场合,为进一步设计光纤2R再生器件提供了重要依据. 相似文献
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为解决四波混频法测量光纤非线性系数未考虑泵浦消耗而导致结果不准确的问题,提出了一种在简并四波混频情况下测量非线性系数的方法.根据光纤中简并的四波混频理论,推导出了考虑泵浦消耗和光纤损耗的椭圆方程.通过设定数值计算所需的各个参量并利用简单的数学方法分析了计入泵浦消耗、光纤损耗的必要性,得到被测光纤的非线性系数,与Optisystem的仿真结果一致.研究表明,这种改进的测量方法不但适用于小信号情形下的四波混频过程,还可以应用于出现参量饱和现象的场合,为进一步设计光纤2R再生器件提供了重要依据. 相似文献
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本文研究了近共振增强的四能级系统有机染料溶液中简并的四波混频后向波和前向波的位相复共轭特性。用有效长度为5毫米、浓度为2.5×10-5克分子的叶绿素A甲醇溶液作介质,当调QNd:YAG倍频抽运光能量为8毫焦耳时,非线性反射率为22%。研究了若丹明6G酒精溶液双光子共振增强的简并的四波混频作用。测量了非线性反射率与介质浓度及抽运波和物波强度的关系曲线。理论分析了四波混频前向波的位相复共轭特性,实验证实了理论的预言。另外,把四重简并的四波混频推广到二重简并。用9740有机染料二氯乙烷饱和吸收溶液作介质,实现了1.06微米到5320埃的象转换。介质长度为5毫米,抽运光能量为5毫焦耳时,转换效率达25%。理论分析表明,用对红外近共振吸收而对可见辐射是透明的介质可实现高效率红外象转换。
关键词: 相似文献
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研究了近共振增强的四能级系统有机染料溶液中简并的四波混频后向反射波及前向波的位相复共轭特性。用有效长度为5mm,浓度为2.5×10~(-5)mol的叶录素A甲醇溶液作介质,当调QNd:YAG倍频泵浦光的能量为8mj时,非线性反射率为22%。 对于若丹明6G酒精溶液,在相同条件下的反射率为10%。用象差板检证了位相复共轭特性。用调QNd:YAG激光辐射作泵浦源,研究了若丹明6G酒精溶液双光子共振增强的简并的四波混频作用。当介质浓度为10~(-4)克分子,有效长度为5mm,泵浦光能量为70mj时,非线性反射率达14%。测量了非线性反射率与介质浓度及入射物波与后向反射波的强度的关系曲线。理论分析了四波混频前向波的位相复共轭特性,用调QNd:YAG倍频激光作泵浦源,若丹明6G酒精溶液作介质,实验上证实了理论的预言。另外,把四重简并的四波混频推广到二重简并的情况。用若丹明6G酒精溶液作介质,实现了由6300A到5320A的象转换。用9740有机染料二氯乙烷饱和吸收溶液作介质,实现了1.06μm到5320A的象转换。当介质长度为5mm,泵浦光束的能量为5mj时,后者的转换效率为25%。理论分析表明,用对红外近共振吸收,而对可见辐射是透明的介质可以实现高效率的红外象转换。这种红外象转换的方法还具有实时、快响应等优点。 相似文献
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本文由光学Bloch方程和密度矩阵方程出发,研究了二能级系统共振型简并四波混频(DFWM)的饱和效应,给出了DFWM信号强度与泵浦光强度的函数关系.饱和泵浦光强的大小取决于纵向弛豫时间T1和横向弛豫时T2.对理论结果与相应实验进行了比较,表明二者符合得很好. 相似文献
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对特定介质中的光学稳态简并四波混频过程进行了数学描述,并对四波混频耦合波方程组作了数学推导,指出四波混频中有关参量之间的关系和特性。 相似文献
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The relaxation oscillation in triply resonant optical parametric oscillators (TROs) is studied theoretically. With constant pumping, the intensity noise spectra of the signal wave consist of a zero frequency and a relaxation oscillation frequency. An accurate relation between the relaxation oscillation frequency and the pump power is obtained. The square of the inherent relaxation oscillation frequency in TROs is linear in the square root of the pump power under high-power pumping. Also, the decay rate varies rapidly with low-power pumping and slowly with high-power pumping. Significantly, when there is a relaxation oscillation in the pumping, the undulation of the signal photon density in TROs also contains the relaxation oscillation frequency of the pumping besides its inherent noise. When those two frequencies are close, a resonance will appear, which should be avoided in practice. PACS 42.65.Yj; 42.65.Sf; 42.60.Rn 相似文献
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G. A. Melkov A. A. Serga A. N. Slavin V. S. Tiberkevich A. N. Oleinik A. V. Bagada 《Journal of Experimental and Theoretical Physics》1999,89(6):1189-1199
A solution is obtained for the general problem of the nonstationary interaction of backward volume magnetostatic waves in
films of yttrium-iron garnet with local parametric pumping. In the case of a large pump region, l≫λ, where λ is the wavelength of the backward volume magnetostatic waves, the problem reduces to a system of truncated equations for
two packets of counter propagating waves. In the opposite case, l<λ, the exact problem of parametric interactions of the eigenmodes of a ferrite film (both counterpropagating and in the same
direction) is solved numerically. Both cases are studied experimentally and good qualitative and quantitative agreement is
obtained with the theory. For the first time, the reversal of a wave front and the time reversal of the shape of backward
volume magnetostatic wave pulses are observed and a change in the propagation time for the peak of the signal pulse and a
reduction in its width owing to pumping are recorded. Two operating regimes are identified for a nonstationary parametric
backward volume magnetostatic wave amplifier with local pumping, which differ in the ratio of the duration of the pump pulse
to the transit time for the wave through the local pump region, and the effect of the parametric excitation of two-dimensional
spin waves on the interaction of backward volume magnetostatic waves with a local nonstationary parametric pump is determined.
Zh. éksp. Teor. Fiz. 116, 2192–2211 (December 1999) 相似文献
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泵浦光强对激光相位共轭波非线性效应的影响 总被引:2,自引:0,他引:2
分析了泵浦光强对激光相位共轭谐振腔中探测光场的作用。基于稳定性定理,通过确定系统的Lyapunov指数,数值计算了在不同泵浦光强下的激光相位共轭波的非线性效应。结果显示,泵浦光强是系统的控制参量。调节泵浦光强的数值,系统的动力学性质发生了改变,可以呈现一周期、二周期、四周期以及倍周期分岔、周期并缩和混沌现象。 相似文献
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在本文中,我们从磁-弹性耦合的宏观表达式,通过经典场论的方法,求得弹性振动和磁振璗的耦合方程,用来分析了伴随波长约等于铁氧体样品的线度的声振动而存在的磁振璗(磁声模)。文中指出,Spencer和LeCraw所发现的磁声效应是磁声模和静磁模在注入场的激发下产生的参量振璗现象(也可以说是热声子的电磁讯号的放大)。我们引用Berk等人在讨论一种半静磁操作放大器的文章中给出的公式,算出Spencer-LeCraw实验所需要的功率,其结果与记录的数据相接近。我们提出了使任一静磁模配合磁声模产生振璗的调谐条件以及降低激发功率和观测几十到几百兆赫的声频的办法。通过磁声模和静磁模的交变场向量的空间对称性的分析,我们推导出磁声参量振璗的选择定则:对于球体三个主要弹性振动模(旋转模、向径模和椭球模),(1)静磁模(n,m,r)的Walker指标n是偶数者不产生磁声效应;(2)指标m是奇数者不与旋转模产生磁声效应,m是偶数者不与向径模或椭球模产生磁声效应。我们也举出第一类本征振动中有只可能和n是偶数、m是奇数的静磁模产生参量振璗的例子。Spencer-LeCraw局限于使静磁场调谐在(110)模上,所观察到的现象仅仅是本文所给出理论预见的一个特殊情况。他们发现了椭球模和向径模的频率显著地出现,但并无旋转模的频率,这是上述的选择定则的具体验证。最后,我们指出,热声子的参量放大可形成铁氧体微波放大器的噪声的来源。 相似文献
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分析了泵浦光为光强在时空上不均匀和高度有限性分布的高斯光波时,对光学参量发生过程的不利影响,提出了解决这种不利影响,以获得高质量,高效率参量光的方案。 相似文献
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针对光学参量振荡产生太赫兹波转换效率低的缺点, 提出了级联参量振荡产生太赫兹波的新机理以提高转换效率. 以周期极化铌酸锂晶体为例, 对级联参量振荡产生太赫兹波的原理和过程进行了理论研究. 分析了抽运光波长、周期极化铌酸锂晶体极化周期和工作温度对产生一阶、二阶闲频光频率的影响. 推导了三波共线相互作用条件下太赫兹波的增益特性和吸收特性. 计算结果表明, 通过级联参量振荡可以有效提高太赫兹波的转换效率, 并可以得到宽调谐的太赫兹波输出. 基于分析结果, 设计了周期极化铌酸锂晶体级联参量振荡产生高效率、宽调谐、窄线宽、连续太赫兹波的实验.
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太赫兹波
太赫兹波参量振荡
级联参量振荡 相似文献
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Second-order nonlinear optical materials for efficient generation and amplification of temporally-coherent and narrow-linewidth terahertz waves 总被引:1,自引:0,他引:1
We have considered forward and backward optical parametric oscillation and amplification, and difference-frequency generation for efficiently generating and amplifying terahertz waves in several second-order nonlinear optical materials. We have used a single crystal of CdSe as an example. We have also investigated GaSe, periodically-poled LiNbO3 and LiTaO3, and diffusion-bonded-stacked GaAs and GaP plates. The advantage of using birefringence in CdSe and GaSe is tunability of the output terahertz frequency. Furthermore, both CdSe and GaSe can be used to achieve the backward parametric oscillation without any cavity. On the other hand, in periodically-poled LiNbO3 and LiTaO3, one can take advantage of large diagonal elements of second-order nonlinear susceptibility tensor. In the diffusion-bonded-stacked GaAs and GaP plates, quasi-phase matching can be achieved by alternatively rotating the plates. We have shown that it is feasible to achieve forward optical parametric oscillation in the THz domain using these plates. The advantage of using coherent parametric processes is possibility of efficiently generating and amplifying temporally-coherent and narrow-linewidth terahertz waves. Compared with a noncollinear configuration, by using the parallel wave propagation configurations, the conversion efficiency can be higher because of longer effective interaction length among all the waves. 相似文献
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Optical parametric amplification controlled by the auxiliary electromagnetic field enables transparency, amplification, and oscillation with no cavity in strongly absorbing negative-index metamaterials. The opposite directions of the wave vector and the Poynting vector in such materials result in extraordinary optical properties, including "backward" phase matching and the generation of entangled pairs of left- and right-handed counterpropagating photons. 相似文献
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Second harmonic generation and optical parametric amplification in negative-index metamaterials (NIMs) are studied. The opposite
directions of the wave vector and the Poynting vector in NIMs results in a “backward” phase-matching condition, causing significant
changes in the Manley–Rowe relations and spatial distributions of the coupled field intensities. It is shown that absorption
in NIMs can be compensated by backward optical parametric amplification. The possibility of distributed-feedback parametric
oscillation with no cavity has been demonstrated. The feasibility of the generation of entangled pairs of left- and right-handed
counter-propagating photons is discussed.
PACS 78.67.-n; 42.65.Ky; 42.65.Lm 相似文献