Muhammad Shabbir, Al-Sehemi Abdullah G, Su Zhongmin, Xu Hongliang, Irfan Ahmad, Chaudhry Aijaz Rasool
Institute of Functional Materials Chemistry, Faculty of Chemistry, Northeast Normal University, Changchun 130024, Jilin, People's Republic of China; Department of Physics, Faculty of Science, King Khalid University, Abha 61413, P.O. Box 9004, Saudi Arabia; Research Center for Advanced Materials Science (RCAMS), King Khalid University, Abha 61413, P.O. Box 9004, Saudi Arabia.
Research Center for Advanced Materials Science (RCAMS), King Khalid University, Abha 61413, P.O. Box 9004, Saudi Arabia; Department of Chemistry, Faculty of Science, King Khalid University, Abha 61413, P.O. Box 9004, Saudi Arabia.
J Mol Graph Model. 2017 Mar;72:58-69. doi: 10.1016/j.jmgm.2016.12.009. Epub 2016 Dec 14.
Using first-principle methods, several key electronic, optical and nonlinear optical properties are calculated for two recently synthesized chalcone derivatives i.e. (2E)-3-(4-methylphenyl)-1-(3-nitrophenyl)prop-2-en-1-one (comp.1) and (2E)-3-[4-(dimethylamino)phenyl]-1-(3-nitrophenyl)prop-2-en-1-one (comp.2). The calculation of dipole moment, polarizability <α>, anisotropy of polarizability as well as second hyperpolarizability (usually considered as a signature for two photon absorption phenomenon) are performed using density functional theory methods at PBE0/6-311G** level of theory. The linear average polarizability <α> for comp.1 and comp.2 are found to be 32.15×10 and 38.76×10esu, respectively. Similarly, the second hyperpolarizability <γ> amplitudes of comp.1 and comp.2 are found to be reasonably larger mounting to 79.31×10 and 181.36×10esu, respectively. The importance of donor end is determined by comparing p-methylphenyl group of comp.1 with that of N,N-dimethylaniline group of comp.2 that results a remarkable increase in its <γ> amplitude, which is ∼2 times larger as compared with that of comp.1 owing to the stronger donor-acceptor configuration of comp.2. Interestingly, a comparison of average static third-order nonlinear polarizabilities <γ> shows that <γ> amplitudes of comp.1 and comp.2 are ∼13 times and ∼29 times larger than that of para-nitroaniline (a typical standard push-pull NLO-phore) at the same PBE0/6-311G** level of theory, which indicates a real time NLO application of our titled compounds. Time dependent density functional theory (TD-DFT) calculations along with frontier molecular orbitals, density of states (DOS), second hyperpolarizability density analysis and molecular electrostatic potential (MEP) diagrams are used to trace the origin of electro-optical as well as structure property relationships.
采用第一性原理方法,计算了两种最近合成的查尔酮衍生物,即(2E)-3-(4-甲基苯基)-1-(3-硝基苯基)丙-2-烯-1-酮(化合物1)和(2E)-3-[4-(二甲基氨基)苯基]-1-(3-硝基苯基)丙-2-烯-1-酮(化合物2)的几个关键电子、光学和非线性光学性质。使用密度泛函理论方法在PBE0/6-311G理论水平上进行偶极矩、极化率<α>、极化率各向异性以及二阶超极化率(通常被视为双光子吸收现象的标志)的计算。化合物1和化合物2的线性平均极化率<α>分别为32.15×10和38.76×10 esu。同样,化合物1和化合物2的二阶超极化率<γ>幅值也相当大,分别为79.31×10和181.36×10 esu。通过比较化合物1的对甲基苯基与化合物2的N,N-二甲基苯胺基团,确定了供体端的重要性,这导致其<γ>幅值显著增加,由于化合物2更强的供体-受体构型,其比化合物1的<γ>幅值大约大2倍。有趣的是,在相同的PBE0/6-311G理论水平下,平均静态三阶非线性极化率<γ>的比较表明,化合物1和化合物2的<γ>幅值分别比对硝基苯胺(一种典型的标准推-拉型非线性光学发色团)大13倍和29倍,这表明我们标题化合物具有实际的非线性光学应用。含时密度泛函理论(TD-DFT)计算以及前沿分子轨道、态密度(DOS)、二阶超极化率密度分析和分子静电势(MEP)图被用于追踪电光以及结构-性质关系的起源。