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采用两波耦合非同时读出实验装置 ,测量了掺铈钾钠铌酸锶钡 (Ce∶KNSBN)晶体两波耦合过程中的信号光和抽运光非同时打开条件下两波耦合增益的时间变化规律 ,讨论了光扇的入射光强阈值及光扇效应对两波耦合动态过程的影响。结果表明 :6 32 .8nmHe Ne激光在Ce∶KNSBN晶体中写入体光栅时 ,光扇效应存在明显的写入光强阈值特性 ,当入射光强大于 30mW /cm2 时 ,才存在强烈的光扇效应。利用修正耦合波方程对Ce∶KNSBN晶体中的两波耦合动态过程、增益随着信号光和抽运光打开时间间隔Δt的变化进行了模拟计算 ,理论模拟结果与实验测量结果基本一致 相似文献
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Ce:KNSBN晶体两波耦合中的光扇效应 总被引:15,自引:2,他引:13
采用两波耦合非同时读出实验装置,测量了掺铈钾钠铌酸锶钡(Ce:KNSBN)晶体两波耦合过程中的信号光和抽运光非同时打开条件下两波耦合增益的时间变化规律,讨论了光扇的入射光强阈值及光扇效应对两波耦合动态过程的影响。结果表明:632.8 nm He-Ne激光在Ce:KNSBN晶体中写入体光栅时,光扇效应存在明显的写入光强阈值特性,当入射光强大于30mW/cm^2时才存在强烈的光扇效应。利用修正耦合波方程对Ce:KNSBN晶体中的两波耦合动态过程、增益随着信号光和抽运光打开时间间隔△t的变化进行了模拟计算,理论模拟结果与实验测量结果基本一致。 相似文献
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基于聚合物分散液晶全息光栅的可调增益均衡器 总被引:7,自引:4,他引:3
从理论和实验两方面分析研究了聚合物分散液晶全息光栅在632.8 nm光波的入射下的衍射谱特性和电压可调特性,实验结果与耦合波理论的计算结果具有很好的一致性,从实验上验证了用耦合波理论来描述聚合物分散液晶全息光栅的衍射特性是恰当的.并且提出了利用聚合物分散液晶全息光栅对掺饵光纤放大器增益谱进行平坦化的方法,利用聚合物分散液晶全息光栅的电压可调特性可实现动态增益均衡.运用该方法,可使掺饵光纤放大器在C波段1530~1560 nm内,温度在0℃~65℃范围内变化,掺饵光纤放大器自发辐射谱的不平坦度从3.3 dB降到0.2 dBp-p(峰-峰值). 相似文献
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采用非同时读出条件下晶体两波耦合实验装置,以单束光入射Ce:KNSBN光折变晶体,通过改变抽运光偏振方向和品体c轴的夹角φ.系统记录了不同φ角下的抽运光透射光强I',随时间的变化情况.实验结果表明,当φ≤30°时,基本没有光扇效应;实验研究了正交偏振光写入下Ce:KNSBN晶体的两波耦合动态过程,并与e光写入下两波耦合动态过程进行了比较,发现正交偏振光写入时光扇噪声得到了明显抑制,在相同的写入参量条件下光栅的衍射效率明显提高. 相似文献
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埋入式光栅双通道特性及其应用研究 总被引:1,自引:0,他引:1
利用严格耦合波理论分析了埋入式光栅在45°入射时,垂直和平行于光栅栅线的两个不同观察平面的零级共振反射衍射特性.在垂直于光栅栅线的平面内,TE、TM偏振下零级反射共振波长分别为432 am和420 am,在平行于光栅栅线的平面内,TE、TM偏振下零级反射共振主峰波长分别为623 nm和620 nm,在两个平面内,零级共振衍射光的共振波长差别较大,观察到的衍射光颜色差别明显,定义为双通道特性并用实验进行证明,制作了相应的光变色器件. 相似文献
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利用二维结构薄膜构建了具有偏振选择特性的新型相位光栅,借助严格耦合波分析(RCWA)方法计算了光栅各级衍射强度随入射光波长及入射角的变化,发现在垂直入射情况下,波长600—640 nm范围内,相位光栅对横向电学(TE)模主要产生0级衍射,而对横向磁学(TM)模产生±1级衍射,在波长633nm处,0级衍射光的偏振消光比为109.8,±1级衍射光的偏振消光比为334.6.利用时域有限差分方法对这种相位光栅的偏振分束现象进行了模拟,偏振分离角在玻璃基板内可以达到10°左右,最后模拟了入射角为23°时光栅对不同偏 相似文献
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光折变晶体中的体全息光栅光衍射的耦合波理论 总被引:1,自引:0,他引:1
本文考虑了晶体的各向异性特点,导出了光折变晶体中的体全息光栅光衍射的耦合波方程,给出了方程的解.用本文的公式还可以解释光线非对称入射时的实验结果. 相似文献
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Wave equations describing the non-linear two-beam coupling have been solved and expressions for the gain of the two beams in the photorefractive crystals have been derived. In case of the degenerate two-beam coupling, the gain depends upon the crystal thickness, coupling coefficient, absorption coefficient and the input intensity ratio. The effect of these parameters on the gain has been studied in details. In case of non-degenerate two-beam coupling the gain not only depends upon crystal thickness, coupling coefficient, absorption coefficient and the input intensity ratio but also on the response time of the photorefractive medium. This response time is the function of concentration ratio. The influence of oscillation frequency shift, concentration ratio on the gain for the non-degenerate two-beam coupling has also been studied. 相似文献
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We propose a simple method for measuring the gain coefficient of two-beam coupling for photorefractive polymer film. To measure the gain coefficient, we attached a phase grating onto the photorefractive polymer film and made an interference pattern between the transmitted and diffracted beams in the photorefractive film by using an illuminating single beam. The gain coefficient values measured at various external fields by our method showed good agreement with those measured by a standard two-beam coupling method. Compared to standard two-beam coupling, this method exhibited fairly improved stability of the output signal to external factors such as human sounds and airstreams. 相似文献
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The analytical solution of the optical field equations and the material equations for two-beam coupling in a medium with real excitation of quasiparticles is given. Transient energy transfer is analyzed throughout the range of the coherent overlapping of the excitation and probe pulses for a hypothetical medium with variable relation between the real part and the imaginary part of the nonlinear response. A detailed comparison between the theory and the model experiments for two-beam coupling in silicon is given. 相似文献
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We observe the photorefractivity without bias voltage or prepoling in a bifunctional photorefractive polymer. The maximum two-beam coupling gain is measured to be 126cm^-1 at zero bias voltage. The sample is considered to be poled by the photoinduced longitudinal electric field, which is formed due to the light intensity gradient along the light path. The expression of the electric field was deduced. The energy transfer direction between two writing beams and light intensity dependence of the two-beam coupling gain coefficient is predicted to be consistent with the experimental results. Furthermore, the dependence of the two-beam coupling gain coefficient on external applied electrical field is measured and this experiment verifies the existence of the photoinduced longitudinal electric field. 相似文献
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Photoconductive dependence of two-beam coupling between the pump beam and the signal beam in photorefractive materials have been analyzed in case of non-degenerate wave mixing under the undepleted pump approximation method. During the two-wave mixing in photorefractive materials, steady state amplification of the signal beam and oscillation characteristics of a single unidirectional ring resonator has been studied. The domination of the two-beam coupling gain over the combined absorption and resonator losses such as Fresnel reflections from the crystal and imperfect mirrors builds up unidirectional oscillation. The buildup of such an oscillation leads to a saturation of the gain, which can be explained in terms of the photorefractive phase-shift. The existence of this phase-shift between the photorefractive index grating and the illumination intensity pattern, which is of characteristic of the photorefractive effect, leads to an energy transfer between the two beams. For a single unidirectional ring resonators, the effects of photoconductivity of the materials, two-beam energy coupling coefficient, dielectric constant, crystal thickness, and material's absorption coefficient on amplification of the two-beam coupling gain and photorefractive phase-shifts of the signal beam have also been studied in detail. It has been found that amplification of the signal beam and phase-shift can be enhanced by taking the photorefractive crystal having higher photoconductivity and lower dielectric constant, which improves performance of the resonators. 相似文献
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Differentiation and subtraction of amplitude and phase images using a photorefractive novelty filter
M. Sedlatschek J. Trumpfheller J. Hartmann M. Müller C. Denz T. Tschudi 《Applied physics. B, Lasers and optics》1999,68(5):1047-1054
In this article, we demonstrate the capability of a two-beam coupling photorefractive optical novelty filter of detecting
changes in the amplitude or phase of optical images. These changes may either be continuous or discrete in time. The performance
of the two-beam coupling novelty filter is investigated and expressions for the output contrast corresponding to phase and
amplitude changes based on a novel, simple interference model of two-beam coupling are derived. These expressions are verified
by experimental results on the novelty contrast, revealing that the amplitude contrast is not described correctly by the commonly
accepted coupled-wave theory. The novelty filter was applied to the detection of temporally continuous phase changes provided
by a gas flow and moving microscopic objects. A novel scheme for image subtraction is also demonstrated, showing the novelty
filter’s ability to detect temporally discrete changes.
Received: 14 November 1998 / Revised version: 18 January 1999 / Published online: 12 April 1999 相似文献
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Dependence of two-beam coupling gain and phase-shift of the signal beams on the frequency detuning for a coupled unidirectional ring resonators based on non-degenerate two-wave mixing in the photorefractive crystals have been investigated in details. The effects of various parameters characterizing the photorefractive medium such as frequency detuning, absorption strength, two-beam energy coupling strength and pump intensity of the external laser beams, on the two-beam coupling gain and phase-shift of the signal beams for a coupled UPRR have also been studied in details. It has been found that the photorefractive gain of the signal beam in the primary cavity of the coupled UPRR can be enhanced to the higher order by taking the lower value of the frequency detuning of the primary cavity which could exist at much lower value of the absorption strength of the crystal B. This higher value of photorefractive gains in the cavities are responsible for the strong coupling between the modes of the oscillations of the coupled UPRR. 相似文献