Bitlis Eren University, Faculty of Arts & Science, Department of Physics, 13000 Bitlis, Turkey.
Spectrochim Acta A Mol Biomol Spectrosc. 2013 Feb;102:286-96. doi: 10.1016/j.saa.2012.10.018. Epub 2012 Oct 24.
The ground state (μ(g)) and excited state (μ(e)) dipole moments of 7-acetoxy-6-(2,3-dibromopropyl)-4,8-dimethylcoumarin (abbreviated as 7ADDC) are estimated from solvatochromic shifts of absorption and fluorescence spectra as a function of the dielectric constant (ε) and refractive index (n). While the ground state dipole moment is determined by using Bilot-Kawski method, the excited state dipole moment is calculated by using Bilot-Kawski, Lippert-Mataga, Bakhshiev, Kawski-Chamma-Viallet and Reichardt correlation methods. Excited state dipole moment is observed as larger than the ground state dipole moment due to substantial π-electron density redistribution. The ground state and excited state dipole moments are observed as parallel to each other with angle of 0°. Solute-solvent interactions are analyzed by means of linear solvation free energy relationships (LSER) using dielectric constant function (f(ε)), refractive index function (f(n)) and Kamlet-Taft parameters (α and β). Atomic charges, electron densities and molecular orbitals are calculated in vacuum and with solvent effect by using both DFT and TDDFT methods. Solvent accessible surface, molecular electrostatic potential (MEP) and electrostatic potential (ESP) are visualized as a result of DFT calculations.
7-乙氧基-6-(2,3-二溴丙基)-4,8-二甲基香豆素(简称 7ADDC)的基态(μ(g)) 和激发态(μ(e)) 偶极矩是通过吸收和荧光光谱的溶剂化位移随介电常数(ε) 和折射率(n) 的函数来估算的。虽然基态偶极矩是通过 Bilot-Kawski 方法确定的,但激发态偶极矩是通过 Bilot-Kawski、Lippert-Mataga、Bakhshiev、Kawski-Chamma-Viallet 和 Reichardt 相关方法计算的。由于π 电子密度的重新分布,激发态偶极矩大于基态偶极矩。基态和激发态偶极矩彼此平行,夹角为 0°。通过使用介电常数函数(f(ε))、折射率函数(f(n))和 Kamlet-Taft 参数(α 和 β),用线性溶剂化自由能关系 (LSER) 分析溶质-溶剂相互作用。通过使用 DFT 和 TDDFT 方法,在真空和溶剂效应下计算原子电荷、电子密度和分子轨道。作为 DFT 计算的结果,可视化了溶剂可及表面、分子静电势 (MEP) 和静电势 (ESP)。