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高β值非线性光学发色团-聚合物客体-主体材料中的近红外光吸收行为。II. 非晶态聚碳酸酯共聚物主体中的染料间隔基长度效应。

Near-infrared optical-absorption behavior in high-beta nonlinear optical chromophore-polymer guest-host materials. II. Dye spacer length effects in an amorphous polycarbonate copolymer host.

作者信息

Barto Richard R, Frank Curtis W, Bedworth Peter V, Ermer Susan, Taylor Rebecca E

机构信息

Department of Materials Science and Engineering, Stanford University and Lockheed Martin Space Systems Company, Palo Alto, California 94304, USA.

出版信息

J Chem Phys. 2005 Jun 15;122(23):234907. doi: 10.1063/1.1929742.

Abstract

In the second of a three-part series, spectral absorption behavior of nonlinear optical (NLO) dyes incorporated into amorphous polycarbonate, comprised of a homologous series of dialkyl spacer groups extending from the midsection of the dye molecule, is characterized by UV-Vis and photothermal deflection spectroscopy. The dyes are structural analogs of the NLO dye FTC [2-(3-cyano-4-{2-[5-(2-{4-[ethyl-(2-methoxyethyl)amino]phenyl}vinyl)-3,4-diethylthiophen-2-yl]vinyl}-5,5-dimethyl-5H-furan-2-ylidene)malononitrile]. Previous Monte Carlo calculations [B. H. Robinson and L. R. Dalton, J. Phys. Chem. A 104, 4785 (2000)] predict a strong dependence of the macroscopic nonlinear optical susceptibility on the chromophore waist: length aspect ratio in electric-field-poled films arising from interactions between chromophores. It is expected that these interactions will play a role in the absorption characteristics of unpoled films, as well. The spacer groups range in length from diethyl to dihexyl, and each dye is studied over a wide range of concentrations. Among the four dyes studied, a universal dependence of near-IR loss on inhomogeneous broadening of the dye main absorption peak is found. The inhomogeneous width and its concentration dependence are seen to vary with spacer length in a manner characteristic of the near-IR loss-concentration slope at transmission wavelengths of 1.06 and 1.3 mum, but not at 1.55 mum. The lower wavelength loss behavior is assigned to purely Gaussian broadening, and is described by classical mixing thermodynamic quantities based on the Marcus theory of inhomogeneous broadening [R. A. Marcus, J. Chem. Phys. 43, 1261 (1965)], modeled as a convolution of dye-dye dipole broadening and dye-polymer van der Waals broadening. The Gaussian dipole interactions follow a Loring dipole-broadening description [R. F. Loring, J. Phys. Chem. 94, 513 (1990)] dominated by the excited-state dipole moment, and have a correlated homogeneous broadening contribution. The long-wavelength loss behavior has a non-Gaussian dye-dye dipole contribution which follows Kador's broadening analysis [L. Kador, J. Chem. Phys. 95, 5574 (1991)], with a net broadening described by a convolution of this term with a Gaussian van der Waals interaction given by Obata et al. [M. Obata, S. Machida, and K. Horie, J. Polym. Sci. B 37, 2173 (1999)], with each term governed by the dye spacer length. A minimum in broadening and loss-concentration slope at a spacer length of four carbons per alkyl at all wavelengths has important consequences for practical waveguide devices, and is of higher aspect ratio than the spherical limit shown by Robinson and Dalton to minimize dipole interactions under a poling field.

摘要

在这个分为三部分的系列文章的第二篇中,通过紫外 - 可见光谱和光热偏转光谱对掺入非晶态聚碳酸酯中的非线性光学(NLO)染料的光谱吸收行为进行了表征,这些染料由从染料分子中部延伸出的一系列同系二烷基间隔基团组成。这些染料是NLO染料FTC [2 - (3 - 氰基 - 4 - {2 - [5 - (2 - {4 - [乙基 - (2 - 甲氧基乙基)氨基]苯基}乙烯基) - 3,4 - 二乙基噻吩 - 2 - 基]乙烯基} - 5,5 - 二甲基 - 5H - 呋喃 - 2 - 基亚甲基)丙二腈]的结构类似物。先前的蒙特卡罗计算[B. H. 罗宾逊和L. R. 道尔顿,《物理化学杂志A》104, 4785 (2000)]预测,在电场极化薄膜中,由于发色团之间的相互作用,宏观非线性光学极化率强烈依赖于发色团腰长与长度的纵横比。预计这些相互作用在未极化薄膜的吸收特性中也将起作用。间隔基团的长度范围从二乙基到二己基,并且对每种染料在很宽的浓度范围内进行了研究。在所研究的四种染料中,发现近红外损耗对染料主吸收峰的非均匀展宽具有普遍依赖性。在1.06和1.3μm的传输波长处,非均匀宽度及其浓度依赖性随间隔长度而变化,其方式与近红外损耗 - 浓度斜率的特征一致,但在1.55μm处并非如此。较低波长的损耗行为归因于纯粹的高斯展宽,并由基于马库斯非均匀展宽理论[R. A. 马库斯,《化学物理杂志》43, 1261 (1965)]的经典混合热力学量来描述,该理论被建模为染料 - 染料偶极展宽和染料 - 聚合物范德华展宽的卷积。高斯偶极相互作用遵循由激发态偶极矩主导的洛林偶极展宽描述[R. F. 洛林,《物理化学杂志》94, 513 (1990)],并且具有相关的均匀展宽贡献。长波长损耗行为具有非高斯的染料 - 染料偶极贡献,并遵循卡多尔的展宽分析[L. 卡多尔,《化学物理杂志》95, 5574 (1991)],其净展宽由该术语与小畑等人给出的高斯范德华相互作用[M. 小畑、S. 町田和K. 堀江,《聚合物科学杂志B》37, 2173 (1999)]的卷积来描述,每个术语都由染料间隔长度决定。在所有波长下,当每个烷基的间隔长度为四个碳原子时,展宽和损耗 - 浓度斜率出现最小值,这对实际的波导器件具有重要影响,并且其纵横比比罗宾逊和道尔顿所示的球形极限更高,以便在极化场下最小化偶极相互作用。

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