SiO2:DR1溶胶-凝胶膜中光吸收和二次谐波的产生与极化时间的关系

A. Franco, G. Valverde-Aguilar, J. García-Macedo
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引用次数: 1

摘要

采用浸涂法制备了无定形和纳米结构SiO2:DR1溶胶-凝胶膜。x射线衍射研究确定了在薄膜中获得的长阶结构。光学吸收(AO)测量在三种不同的纳米结构SiO2网络:片层,六边形和混合。在薄膜中嵌入的发色团的不同取向步长处进行了AO测量和二次谐波强度测量。这些发色团的取向分布是通过电晕技术得到的,它们与电晕极化时间有关。我们将光吸收和二次谐波产生的实验结果作为电晕极化时间的函数进行物理建模,只使用一个与基质-发色团相互作用相关的拟合参数。物理模型与实验结果非常吻合。模型拟合的实验结果显示为阶参量与日冕极化时间的关系图和SHG强度与日冕极化时间的关系图。与其他结构相比,层状结构提供了更大的阶参量值。通过在短极化时间内的光学吸收测量来检测阶参量的最小值。对于SHG测量,使用了四种不同的发色团浓度。随着浓度的增加,测量到的SHG强度也会增加,但增量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。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optical absorption and second harmonic generation in SiO2:DR1 sol-gel films as function of poling time
Amorphous and nanostructured SiO2: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 SiO2 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.
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