Comment on "Temporally resolved electro-optic effect"

We comment on the recent Letter by S. P. Jamison et al. [Opt. Lett.31, 1753 (2006)] where the analysis of a chirped probe pulse that is electro-optically modulated by a terahertz pulse reportedly results in a new expression for the electric field. While in principle the derived expressions for the total field after the crystal are correct, in their treatment the authors implicitly assumed that the derived total field is identical to the measured field, without regard to the residual birefringence of a typical electro-optic crystal or a crossed analyzer. Based on this analysis neglecting birefringence, they report that earlier expressions of the temporal field are incorrect. Here we show, on the contrary, that for chirped single-shot terahertz measurement schemes that include residual birefringence, the temporally resolved electro-optic effect is described correctly by the commonly used expression in the literature. We verify this result with our experimental data.     

Temporally and spectrally resolved imaging of laser-induced plasmas

We report a hybrid imaging technique capable of performing measurements of the spatial, temporal, and spectral emission characteristics of laser-induced plasmas by use of a single detection system. We apply this technique to study the plasma produced by laser ablation of LiNbO3 and observe phenomena not seen in such detail with standard instruments. These include extreme line broadening up to a few nanometers accompanied by self-absorption near the target surface, and expansion dynamics that differ strongly between the different species. Overall, the wealth of quantitative information provided by this novel technique sheds new light on processes occurring during plasma expansion.     

Temporally and spectrally resolved sampling imaging with a specially designed streak camera

We present a novel sampling imaging technique capable of performing simultaneous two-dimensional measurements of the temporal and spectral characteristics of light-emission processes by use of a specially designed streak camera. A proof-of-principle experiment was performed with a homemade multifocal multiphoton fluorescence microscope. The system was calibrated with a Fabry-Perot etalon and a standard fluorophore solution (rhodamine 6G in ethanol) and was shown to have temporal and spectral resolution of 6.5 ps and 3 nm, respectively, as well as high accuracy and reproducibility in lifetime and spectrum measurement. Temporally and spectrally resolved images of 4 x 4 foci on the sample can be obtained with a snapshot.     

The electro-optic effect in proustite

The low-frequency unclamped electro-optic coefficients of proustite have been measured at an optical wavelength of 0.6328m. The results show thatr ₂₂ is comparable to that of lithium niobate,r ₁₃ andr ₃₃ are considerably lower. The maximum theoretical value is calculated at 10.8×10^–12 m/V about three times the largest measured coefficient value.     

LB薄膜的线性电光效应

本文用电光微分表面等离子激元光谱研究芪盐单分子层LB薄膜在不同光波长处(488nm,633nm和832nm)的电光响应.指出这是一种十分有效,简便的评估厚度小于100nm超薄膜非线性光学特性的实验技术.     

A semiclassical approach for electro-optic effect

In this article, we present a semiclassical approach for modeling of electro-optic (EO) effect. We calculate phase retardation between x and y polarizations of optical electric field when a transverse external electric field is applied. Our results are well agreed with experimental measurements. Moreover, we show when wavelength of optical signal decreases, the phase retardation increases.     

Temporally and spectrally resolved analysis of a copper plasma plume produced by ultrafast laser ablation

We report an experimental analysis of the plasma plume produced during ultrafast laser ablation of a copper target, in high vacuum. The plasma plume optical emission is studied by using a hybrid time-gated imaging technique which allows obtaining simultaneous information on the spectral and spatial characteristics of the emitting species. We used both single and double pulse ablation scheme, observing their influence on the characteristics of the ablated atomic species.     

电光晶体研究究进进展及其对称性性研研究

由电场引起的晶体折射率的变化称为晶体的电光效应,具有电光效应的晶体称为电光晶体。利用电光效应可以制作电光Q开关等重要光电器件。晶体的电光效应及其有效利用,均与其对称性密切相关。本文在综述电光晶体研究进展的基础上,推导了不同晶系中各晶类电光效应类型及其特点,并以电光Q开关的要求为例讨论了晶体的电光效应及其对称性之间的关系。从讨论结果得出:立方晶系Td-ˉ43m,三方晶系C3v-3m,四方晶系D2d-4ˉ2m,D4v-4mm和六方晶系D3h-6ˉm2,C6v-6mm点群中相应电光系数的横向或纵向效应可能有实用价值。在考虑旋光性影响后,立方晶系T-23,三方晶系D3-32,四方晶系中S4-4ˉ,六方晶系中C3h-6ˉ等也有可能应用。但是,电光晶体的应用与许多因素相关,对称性只是其中一个基本条件。     

基于电光效应的光子频移研究

系统分析了如何通过电光调制的方式来消除量子点纠缠光源中不同偏振模式光子之间的频率差异,并实际设计了一套泡克耳斯盒电光调制方案,通过给其加载约8 V/ns的上升沿或下降沿电压,实现了18 MHz带宽的光子频率的移动.表明只需增大调制电压斜率,便可以有效实现GHz以上的频率移动,为未来实现确定性完美的量子点纠缠光源提供了切实可行的依据.     

Photonic switching nodes based on self electro-optic effect devices

Photonic switching nodes based on self electro-optic devices are described. These nodes are proposed for use in extended generalized shuffle networks with free space digital optical interconnections between nodes. Several experiments are described demonstrating both individual switching nodes and arrays of switching nodes operating concurrently. Node complexity, optical system complexity, and tolerance issues associated with different types of nodes are also discussed.     

偏振态对准相位匹配线性电光效应的影响

系统研究入射光为不同偏振态时的准相位匹配线性电光效应。在准相位匹配条件满足时,若入射光为线偏振光,则o光与e光能够彻底耦合,出射光仍为线偏振光,且其偏振方向可以通过外加电场调节到任意角度;若入射光为椭圆偏振光,则o光与e光不能彻底耦合,输出光为与输入光同椭圆率的椭圆偏振光,其椭圆方位角可以通过调节外加电场旋转到任意角度;若入射光为圆偏振光,则o光与e光之间没有能量耦合,输出光仍为圆偏振光。准相位匹配条件满足的线性电光效应在保偏的偏振旋转器中有重要应用。在准相位匹配条件不满足时,o光与e光由于相位失配而没有能量耦合,输出光的偏振态取决于o光与e光的初始相位差和双折射(自然双折射和电光双折射)引起的附加相位差,特别是极化占空比为0.5时,电光效应引起的双折射总效果为零。     

Quadratic electro-optic effect and electro-absorption process in CdSe-ZnS-CdSe structure

The third order nonlinearity susceptibility is obtained as a function of wavelength for CdSe-ZnS-CdSe structure. Numerical calculations show that the quadratic electro-optic and electro absorption effects of this structure depend on the parameters such as structure size, relaxation time and pump photon energy. By changing shells thickness, these structures can be designed with the susceptibility peak from the visible to infrared regions of the spectrum. The intensity and position of the third order nonlinearity susceptibility peaks depend on outer shell thickness and radius of the core.     

First-principles study of the electro-optic effect in ferroelectric oxides

We first present a method to compute the electro-optic tensor from first principles, explicitly taking into account the electronic, ionic and piezoelectric contributions. We then study the nonlinear optic behavior of three paradigmatic ferroelectric oxides. Our calculations reveal the dominant contribution of the soft mode to the electro-optic coefficients in LiNbO3 and BaTiO3 and its minor role in PbTiO3. We identify the coupling between the electric field and the polar atomic displacements along the B-O chains as the origin of the large electro-optic response in perovskite ABO3 compounds.     

旋光性与电光效应交互作用及其对旋光晶体电光Q开关的影响

研究了晶体的旋光性与电光效应的交互作用、以及此交互作用对 旋光晶体电光Q开关的影响. 关键词： 旋光性 电光效应 电光Q开关 3Ga₅SiO₁₄晶体')" href="#">La₃Ga₅SiO₁₄晶体     

Wave-coupling theory of linear electro-optic effect for ultrashort laser pulses

A wave-coupling theory of linear electro-optic (EO) effect for ultrashort laser pulses has been developed. As one of its applications, the linear EO effect of ultrashort Gaussian pulses propagating in LiNbO₃ crystal is demonstrated, with the intensity lower than the damage threshold. It is found that the EO effect is sensitive to both the azimuth angle and the polar angle of wave vector of light. And the larger the applied electric field, the shorter the crystal used for optimization of EO coupling is. The numerical results show that, with the duration of input pulse changing from 150 fs to 5 fs, the durations of output pulses are broadened due to the group-velocity dispersion, as well as the first- and second-order refractive dispersion. In addition, when input pulse duration is larger than 20 fs, in contrast with zero chirp, the output durations can be slightly compressed if a positive chirp input pulse is used. The validities of slowly varying amplitude approximation and continuous wave approximation are also discussed. The influence of self-phase modulation and cross-phase modulation on the EO effect is also discussed briefly.