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二甲基萘异构体的静态和动态电子(超)极化率:通过密度分析表征空间贡献

Static and dynamic electronic (hyper)polarizabilities of dimethylnaphthalene isomers: characterization of spatial contributions by density analysis.

作者信息

Alparone Andrea

机构信息

Department of Chemistry, University of Catania, Viale A. Doria 6, 95125 Catania, Italy.

出版信息

ScientificWorldJournal. 2013 Oct 28;2013:832682. doi: 10.1155/2013/832682. eCollection 2013.

DOI:10.1155/2013/832682
PMID:24288508
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC3830888/
Abstract

Static and frequency-dependent electronic (hyper)polarizabilities of the dimethylnaphthalene (DMN) isomers were computed in vacuum using the Coulomb-attenuating Density Functional Theory method. The nonlinear optical Second Harmonic Generation (SHG) and Electro-Optical Pockels Effect (EOPE) were investigated at the characteristic Nd:YAG laser wavelength of 1064 nm. The response electric properties especially the longitudinal polarizability, polarizability anisotropy, and first-order hyperpolarizability are significantly affected by the position of the methyl groups. The SHG and EOPE techniques can be potentially useful to discriminate the α,α-DMN isomers (2,6-DMN < 2,7-DMN < 2,3-DMN) as well as the β,β-DMN isomers (1,5-DMN < 1,4-DMN < 1,8-DMN). The (hyper)polarizability differences among the investigated DMNs were elucidated through density analysis calculations. The predicted polarizabilities exhibit good linear relationships with the experimental first-order biomass-normalized rate coefficient, a physicochemical property connected to the rates of biodegradation processes of polycyclic aromatic hydrocarbons.

摘要

采用库仑衰减密度泛函理论方法,在真空中计算了二甲基萘(DMN)异构体的静态和频率相关的电子(超)极化率。在1064nm的特征钕:钇铝石榴石激光波长下,研究了非线性光学二次谐波产生(SHG)和电光普克尔效应(EOPE)。响应电性质,特别是纵向极化率、极化率各向异性和一阶超极化率,受甲基位置的显著影响。SHG和EOPE技术可能有助于区分α,α-DMN异构体(2,6-DMN < 2,7-DMN < 2,3-DMN)以及β,β-DMN异构体(1,5-DMN < 1,4-DMN < 1,8-DMN)。通过密度分析计算阐明了所研究的DMN之间的(超)极化率差异。预测的极化率与实验一阶生物质归一化速率系数呈现良好的线性关系,该系数是一种与多环芳烃生物降解过程速率相关的物理化学性质。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/e339e84d684d/TSWJ2013-832682.004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/4327eb1a4812/TSWJ2013-832682.001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/754351d46c1d/TSWJ2013-832682.002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/a424d3318038/TSWJ2013-832682.003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/e339e84d684d/TSWJ2013-832682.004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/4327eb1a4812/TSWJ2013-832682.001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/754351d46c1d/TSWJ2013-832682.002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/a424d3318038/TSWJ2013-832682.003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9c8/3830888/e339e84d684d/TSWJ2013-832682.004.jpg

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