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用溶剂变色法估算 1,4-二取代蒽醌染料的基态和第一激发单线态偶极矩。

Estimation of the ground and the first excited singlet-state dipole moments of 1,4-disubstituted anthraquinone dyes by the solvatochromic method.

机构信息

Department of Physics, Gulbarga University, Jnana Ganga, Gulbarga 585106, Karnataka, India.

出版信息

Spectrochim Acta A Mol Biomol Spectrosc. 2010 Apr;75(4):1203-10. doi: 10.1016/j.saa.2009.12.007. Epub 2009 Dec 6.

DOI:10.1016/j.saa.2009.12.007
PMID:20138571
Abstract

The both, ground-state (mu(g)) and the excited-state (mu(e)) dipole moments of three 1,4-disubstituted anthraquinones, namely 1,4-diaminoanthracene-9,10-dione (1,4-DAAQ), 1-amino-4-hydroxyanthracene-9,10-dione (1,4-AHAQ), and 1,4-dihydroxyanthracene-9,10-dione (1,4-DHAQ) were estimated in binary solvent mixtures (methylcyclohexane-ethyl acetate and ethyl acetate-acetonitrile). The dipole moments (mu(g) and mu(e)) were estimated from Lippert-Mataga, Bakhshiev, Kawski-Chamma-Viallet, McRae, and Suppan equations by using the variation of Stokes shift with the solvent's relative permittivity and refractive index. The ground-state dipole moments were also calculated theoretically by Gaussian 03 software using B3LYP/6-31 G* level of theory. Further, the change in dipole moment values Deltamu were also calculated by using the variation of Stokes shift with the molecular-microscopic empirical solvent polarity parameter (E(T)(N)). The excited-state dipole moments observed are larger than their ground-state counterparts, indicating a substantial redistribution of the pi-electron densities in a more polar excited state for all the molecules investigated.

摘要

三种 1,4-取代蒽醌的基态(μ(g))和激发态(μ(e))偶极矩,即 1,4-二氨基蒽醌-9,10-二酮(1,4-DAAQ)、1-氨基-4-羟基蒽醌-9,10-二酮(1,4-AHAQ)和 1,4-二羟基蒽醌-9,10-二酮(1,4-DHAQ),在二元溶剂混合物(甲基环己烷-乙酸乙酯和乙酸乙酯-乙腈)中进行了估算。偶极矩(μ(g)和μ(e))是通过 Lippert-Mataga、Bakhshiev、Kawski-Chamma-Viallet、McRae 和 Suppan 方程,利用斯托克斯位移随溶剂相对介电常数和折射率的变化来估算的。基态偶极矩也通过 Gaussian 03 软件使用 B3LYP/6-31 G*理论水平进行了理论计算。此外,还通过斯托克斯位移随分子微观经验溶剂极性参数(E(T)(N))的变化来计算偶极矩值的变化Δμ。观察到的激发态偶极矩大于其基态偶极矩,表明在所有研究的分子中,在更极性的激发态下,π电子密度发生了实质性的重新分布。

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