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关于 sp 和 sp 杂化单空位缺陷[60]富勒烯的含时密度泛函理论研究:C59[9-4]和 C59[8-5]异构体的电子激发和非线性光学性质

TD-DFT Studies on sp- and sp-Hybridized Single Vacancy-Defected [60]Fullerene: Electronic Excitation and Nonlinear Optical Properties of C59 [9-4] and C59 [8-5] Isomers.

作者信息

Omri Nabil, Bu Yuxiang

机构信息

School of Chemistry and Chemical Engineering, Shandong University, Jinan 250100, People's Republic of China.

出版信息

J Phys Chem A. 2021 Jan 14;125(1):106-114. doi: 10.1021/acs.jpca.0c08533. Epub 2020 Dec 23.

DOI:10.1021/acs.jpca.0c08533
PMID:33355451
Abstract

By removing one carbon atom from [60]Fullerene (C60), two different isomers (C59 [9-4] and C59 [8-5]) are generated for the C59 cluster. Inspired by their structural and electronic properties, we, theoretically, studied the static and frequency-dependent electronic (hyper)polarizabilities of sp- and sp-hybridized isomers in vacuum by TD-DFT calculations. The simulated absorption spectra showed that all absorption bands of C59 [9-4] and C59 [8-5] are attributed to π → π* and n → π* transitions. Regarding their nonlinear optical properties, it is found that the frequency-dependent polarizability anisotropy α(λ = 1064.80 nm) of C59 [8-5] is 4 times larger than the static regime, revealing a notable polarization anisotropy, due to the delocalized π electrons around the vacancy defect. By decreasing the incident wavelengths from λ = 1908 nm to λ =589.08 nm, the dispersion of optical nonlinearity of C59 [8-5] has achieved the maximum at β (λ = 1064.8 nm) = 38.150 au and (γ (λ = 589.08 nm) -9.896 × 10 au), indicating that the resonance effect of the hyperpolarizability amplified with the decrease of incident wavelengths. Hyperpolarizability density analyses in and directions displayed that the conspicuous negative ρ() and -ρ() are more expanded on the C59 [8-5] cage when the main contributions stem from the π electrons instead to the sp-hybridized carbon.

摘要

通过从[60]富勒烯(C60)中去除一个碳原子,C59团簇会生成两种不同的异构体(C59[9-4]和C59[8-5])。受其结构和电子性质的启发,我们通过时域密度泛函理论(TD-DFT)计算,在理论上研究了真空条件下sp和sp杂化异构体的静态和频率相关电子(超)极化率。模拟吸收光谱表明,C59[9-4]和C59[8-5]的所有吸收带均归因于π→π和n→π跃迁。关于它们的非线性光学性质,发现C59[8-5]的频率相关极化率各向异性α(λ = 1064.80 nm)比静态状态下大4倍,这表明由于空位缺陷周围的离域π电子,存在显著的极化各向异性。通过将入射波长从λ = 1908 nm减小到λ = 589.08 nm,C59[8-5]的光学非线性色散在β(λ = 1064.8 nm) = 38.150 au和(γ(λ = 589.08 nm) = -9.896 × 10 au)时达到最大值,这表明超极化率的共振效应随着入射波长的减小而增强。在 和 方向上的超极化率密度分析表明,当主要贡献源于π电子而非sp杂化碳时,C59[8-5]笼上显著的负ρ()和-ρ()会更加扩展。

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