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Optical absorption and second harmonic generation in SiO_2:DR1 sol-gel films as function of poling time

机译:SiO_2:DR1溶胶-凝胶薄膜的光吸收和二次谐波的产生与极化时间的关系

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Amorphous and nanostructured SiO_2:DR1 sol-gel films were prepared by dip-coating. X-ray diffraction studies were performed to determine the long-order structure obtained in the films. The optical absorption (AO) measurements were done in three different nanostructures of the SiO_2 network: lamellar, hexagonal and mixed. The AO measurements and the second harmonic generation (SHG) intensity were carried out at different orientation steps of the chromophores embedded in the films. These chromophore orientation distributions were obtained by means of the corona technique, and they depend on the corona poling time. We physically model the optical absorption and the second harmonic generation experimental results as function of the corona poling time, employing only one fitting parameter related to the matrix-chromophore interactions. The physical model and the experimental results were in an excellent agreement The experimental results fitted by the model are shown in plots of order parameter against corona poling time and SHG intensity against corona poling time. The lamellar structure provides a larger order parameter values than those obtained for the other structures. A minimum value for the order parameter was detected by means of the optical absorption measurements at short poling times. For the SHG measurements, four different chromophore concentrations were used. As the concentration increases the measured SHG intensity increases too, but the increment is limited by the electrostatic interactions among the chromophores, which is also considered in our model.
机译:通过浸涂制备非晶和纳米结构的SiO_2:DR1溶胶-凝胶膜。进行X射线衍射研究以确定在膜中获得的长结构。在SiO_2网络的三种不同纳米结构中进行了光吸收(AO)测量:层状,六边形和混合。 AO测量和二次谐波生成(SHG)强度是在包埋在薄膜中的生色团的不同取向步骤下进行的。这些生色团取向分布是通过电晕技术获得的,它们取决于电晕极化时间。我们仅使用一个与基质-发色团相互作用有关的拟合参数,将光吸收和二次谐波产生实验结果作为电晕极化时间的函数进行物理建模。物理模型与实验结果吻合得很好。模型拟合的实验结果显示在订购参数对电晕极化时间和SHG强度对电晕极化时间的图中。层状结构提供的阶次参数值比其他结构获得的阶次参数值大。在短极化时间内通过光吸收测量来检测阶次参数的最小值。对于SHG测量,使用了四种不同的生色团浓度。随着浓度的增加,测得的SHG强度也会增加,但是这种增加受到发色团之间静电相互作用的限制,我们的模型也考虑了这一点。

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