Institute of Functional Material Chemistry, Faculty of Chemistry, Northeast Normal University, Changchun 130024, Jilin, People's Republic of China.
Institute of Functional Material Chemistry, Faculty of Chemistry, Northeast Normal University, Changchun 130024, Jilin, People's Republic of China.
J Mol Graph Model. 2014 Mar;48:28-35. doi: 10.1016/j.jmgm.2013.09.008. Epub 2013 Sep 23.
The unusual properties of Li-doped boron nitride nanomaterials have been paid further attention due to their wide applications in many promising fields. Here, density functional theory (DFT) calculations have been carried out to investigate the second-order nonlinear optical (NLO) properties of boron nitride nanocone (BNNC) and its Li-doped BNNC derivatives. The natural bond orbital charge, electron location function, localized orbital locator and frontier molecular orbital analysis offer further insights into the electron density of the Li-doped BNNC derivatives. The electron density is effectively bounded by the Li atom and its neighboring B atoms. The Li-doped BNNC molecules exhibit large static first hyperpolarizabilities (β(tot)) up to 1.19×10³ a.u. for Li@2N-BNNC, 5.05×10³ a.u. for Li@2B-BNNC, and 1.08×10³ a.u. for Li@BN-BNNC, which are significantly larger than that of the non-doped BNNC (1.07×10² a.u.). The further investigations show that there are clearly dependencies of the first hyperpolarizabilities on the transition energies and oscillator strengths. Moreover, time-dependent DFT results show that the charge transfer from BNNC to Li atom becomes more pronounced as doping the Li atom to BNNC. It is also found that the frequency-dependent effect on the first hyperpolarizabilities is weak, which may be beneficial to experimentalists for designing Li-doped BNNC molecules with large NLO responses.
由于掺锂氮化硼纳米材料在许多有前途的领域中的广泛应用,其独特的性质引起了人们的进一步关注。在这里,我们通过密度泛函理论(DFT)计算研究了氮化硼纳米角锥(BNNC)及其掺锂 BNNC 衍生物的二阶非线性光学(NLO)性质。自然键轨道电荷、电子位置函数、局域轨道定位器和前沿分子轨道分析进一步揭示了掺锂 BNNC 衍生物的电子密度。电子密度有效地被 Li 原子及其相邻的 B 原子束缚。掺锂 BNNC 分子表现出较大的静态第一超极化率(β(tot)),对于 Li@2N-BNNC 为 1.19×10³ a.u.,对于 Li@2B-BNNC 为 5.05×10³ a.u.,对于 Li@BN-BNNC 为 1.08×10³ a.u.,均显著大于未掺杂 BNNC 的 1.07×10² a.u.。进一步的研究表明,第一超极化率明显依赖于跃迁能量和振子强度。此外,含时密度泛函理论(TD-DFT)的计算结果表明,当向 BNNC 中掺杂 Li 原子时,BNNC 到 Li 原子的电荷转移变得更加明显。还发现,第一超极化率对频率的依赖性较弱,这可能有助于实验人员设计具有大 NLO 响应的掺 Li 氮化硼纳米角锥分子。