偶氮基染料掺杂薄膜的双光子图象存储

研究了偶氮基染料掺杂薄膜ＭＯ－ＰＶＡ和ＥＯ－ＰＶＡ的双光子存储特性。在对薄膜用Ａｒ＾＋激光作预激发下实现了Ｈｅ－Ｎｅ激光的红光存储。获得了实时和短时存储照片。光电记录存储曲线，分析了双光四能级系统的存储机制。实现确定了最佳预激发功率约为０．２８Ｗ／ｃｍ＾２，最小Ｈｅ－Ｎｅ光可存储功率密度低于０．２Ｗ／ｃｍ＾２。     

强场作用下二能级原子双光子过程中的光子聚束与反聚束效应

本文采用数值计算方法研究了强场作用下二能级原子双光子过程中的光子聚束与反聚束效应.结果表明:辐射光子主要表现为反聚束性质,且随着n值的不断增大,场与原子的非线性耦合越来越强,重复地出现复苏收缩现象和短时的光子聚束效应.     

Four-State Model for Three-Branch Molecule＇s Two-Photon Absorption Properties

We present a four-state model for calculating the two-photon absorption of multi-branched molecules by using the time-depended function method, The numerical results indicate that the two-photon absorption cross section has a strong enhancement for three-branch molecules compared to two-branch structures, The maximal two-photon-absorption cross section is 2.358 × 10^-47 cm^4s/photon, At the same time, the charge-transfer process for the charge-transfer states is visualized in order to explain mechanism about the maximal TPA cross section.     

GaAs半导体材料中双光子吸收光限幅与偏振方向的关系

理论分析了线偏振光波的偏振方向对ＧａＡｓ半导体双光子吸收的影响，实现了ＧａＡｓ半导体材料中不同偏振方向的双光子吸收限幅，提高了双光子吸收光限幅的性能。     

钠5S态与基态钾原子的碰撞能量转移

在Ｎａ－Ｋ混合蒸汽中，利用染料激光器，将基态Ｎａ原子双光子激发到５Ｓ态。用荧光法测量了过程Ｎａ（５Ｓ）＋Ｋ（４Ｓ）→Ｎａ（３Ｓ）＋Ｋ（８Ｄ，１０Ｓ）的碰撞转移截面，Ｋ８Ｄ，１０Ｓ对Ｎａ５Ｓ的荧光比中，含有Ｋ８Ｄ１０Ｓ碰撞转移的影响。第２个实验可以消除这个影响，双光子激发Ｋ原子到８Ｄ（或１０Ｓ）探测８Ｄ（１０Ｓ）对１０Ｓ（８Ｄ）的荧光比，Ｎａ（５Ｓ）→Ｋ（８Ｄ，１０Ｓ）碰撞转移截面（１０－１５ｃｍ２）分别是１０．５±４．２和９．５±３．８     

压缩真空变态中二能级原子简并双光子过程的广义Bloch—Siegert频移

用密度算符主方程方法研究了一二能极原子与宽压缩真空态光场的简交双光子相互作用。我们发现原子偶极矩随时间的变化与压缩真空态光场的压缩参数│Ｍ│有关。│Ｍ│存在一个阈值Г／４ｇ。阈值之下，原子偶极矩以共振频率振荡。     

利用双光子J-C模制备三原子的W纠缠态

提出了利用双光子J-C模制备三原子W纠缠态的方案。阐明了通过控制原子腔场的相互作用时间便能获得所制备的态。还指出利用这个模型制备W态比制备GHZ态更优越。此外，就腔QED技术对方案的实验实现作了分析。     

温度对双光子独立明-暗空间屏蔽孤子对稳定性的影响

在忽略损耗和扩散的情况下,采用数值方法研究温度对串联双光子光折变晶体回路中独立明-暗屏蔽孤子对演化和稳定性的影响.结果表明:在给定温度下晶体回路中形成稳态明-暗孤子对,当一个晶体的温度改变且温度变化不大时,另一块晶体中支持的孤子将转变为另一个稳态孤子;当温度变化过大时,这个孤子将变得不稳或发生周期性的压缩或膨胀甚至崩溃.在独立屏蔽空间孤子对中,暗孤子对温度的敏感程度比明孤子强.     

双光子光折变介质中非相干耦合光伏孤子族

为了得到双光子非相干耦合光伏孤子族的结果,采用数值模拟方法,对稳态情况下多束互不相干的光束在双光子光伏光折变晶体中的传播进行了研究。结果表明:具有相同偏振和相同波长的多束互不相干的入射光束可在晶体中形成双光子非相干耦合光伏孤子族。当入射光束中仅包含两个分量时,孤子族就转化为光伏孤子对。并用双光子光伏光折变晶体Cu:KNSBN和LiNbO3进行了分析说明。研究结果可为空间光孤子理论的发展提供理论依据。     

Improving the precision of fluorescence lifetime measurement using a streak camera

Streak camera has high temporal resolution and high sensitivity, and is a powerful tool in biomedical study to measure fluorescence lifetime and perform fluorescence lifetime imaging. However, nonuniformity of the gain in the streak tube and nonlinearity of the sweeping speed limit the precision of fluorescence lifetime measurement, particularly when fluorescence lifetimes are short. We have constructed a two-photon excitation fluorescence lifetime measurement system that is based on a synchroscan streak camera and have developed accordingly a method to correct the effect of gain nonuniformity and nonlinearity of sweeping speed on the measurement precision. A continuous-wave laser of high stability is used to calibrate the gain of the streak camera, and a Fabry-Perot etalon is used to calibrate the nonlinearity of the sweeping speed. Fitting algorithms are used to correct the gain of the streak camera and nonlinearity of the sweeping speed respectively, which significantly improves the measurement precision of the system, as characterized through the fluorescence lifetime of the short-lived fluorescence dye, Rose Bengal. Experimental results show that the measurement fluctuation of the lifetime has been improved from more than 10% to 2% after correcting the effects of gain nonuniformity and sweeping speed nonlinearity.