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Theoretical study of optical pockels and Kerr coefficients of polyenes

机译:聚烯酶光袋和克尔系数的理论研究

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We report here the numerically exact Pockels' and Kerr's coefficients of polyenes within the Pariser-Parr Pople Model. We have computed the model exact polarizability of polyenes of chain length, N $EQ 6, 8 and 10 at various static electric fields and excitation frequencies. From a 3rd degree polynomial fit of the model exact polarizability ($beta@(approximately ega@; approximately ega@,O) (linear term) and $tau@(approximately ega@; approximately ega@,O,O) (2nd order term) are obtained. The Pockels and Kerr coefficients are calculated from $beta and $tau@. In polyenes the Pockels coefficients are small and the Kerr coefficients dominate and are the largest when the field is applied along the chain axis. The coefficients, $alpha@(approximately ega@; approximately ega@), $beta@(approximately ega@; approximately ega@,O) and $tau@(approximately ega@; approximately ega@,O,O) all increase with chain length. $alpha@(approximately ega@; approximately ega@) and $tau@(approximately ega@; approximately ega@,O,O) have the usual power law dependence and have exponent values at 1.54 and 3.78 respectively which are in agreement with the values reported in the literature. The coefficients $alpha@(approximately ega@; approximately ega@), $beta@(approximately ega@; approximately ega@,O) and $tau@(approximately ega@; approximately ega@,O,O) increases with increase in the excitation frequency, for frequencies below the two photon resonance value.
机译:我们在这里报道了在巴黎 - Parr Pople模型中的数值精确的Pockels和Kerr的聚烯部分系数。我们计算了各种静电场和励磁频率的链长,N $ EQ 6,8和10的聚烯部分的模型精确极化性。从模型精确的极化性($测试的第三阶多项式拟合@(约EGA @;约EGA @,O)(线性项)和$ tau蛋白@(约EGA @;约EGA @,O,O)(2阶获得术语。袋子和kerr系数由$ beta和$ tau @计算。在聚合物中,孔径系数小,kerr系数占据沿链轴施加的磁场。系数,$ alpha @(大约是ega @;大约是ega @),$ beta @(大约是ega @;大约是ega @,o)和$ tau @(大约ega @;大约是ega @,o,o)所有增加链长。$ Alpha @(大约是ega @;大约是ega @)和$ tau @(大约是ega @;大约是ega @,o,o)具有通常的权力法依赖性,并且分别在1.54和3.78处具有指数值,这与价值观一致在文献中报道。系数$ alpha @(大约是ega @; ega @),$ beta @(大约是ega @;近似ega @,o)和$ tau @(大约是ega @;大致EGA @,O,O)随着激励频率的增加而增加,用于两个光子谐振值以下的频率。

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