4.5 Article

Oxacarbon superalkali C3X3Y3 (X = O, S and Y = Li, Na, K) clusters as excess electron compounds for remarkable static and dynamic NLO response

期刊

出版社

ELSEVIER SCIENCE INC
DOI: 10.1016/j.jmgm.2021.107922

关键词

Superalkali clusters; Excess electrons; Nonlinear optical response; Refractive index; Dynamic nonlinear optical properties

资金

  1. Higher Education Commission of Pakistan
  2. COMSATS University, Abbottabad Campus

向作者/读者索取更多资源

A class of excess electron oxacarbon superalkali clusters with intriguing nonlinear optical response and remarkable electronic properties are explored. The clusters exhibit excellent thermodynamic and electronic stability, along with superior nonlinearity. The key factor controlling the first hyperpolarizability is found to be the excitation energy.
An intriguing class of excess electron oxacarbon superalkali clusters is explored for nonlinear optical response through density functional theory (DFT) methods at CAM-B3LYP/6-311++G(d,p). These superalkali clusters shows noticeable binding energies per atom (E-b) which reveals their thermodynamic stabilities (-86.45 similar to-119.44 kcal mol(-1)). The obtained significant VIPs values also suggest the electronic stability of these clusters. The VIP values range from 2.06 eV to 3.42 eV. These clusters show remarkable electronic properties and their HOMO-LUMO gaps (EH-L) are significantly reduced. The lowest H-L gap of 0.96 eV is obtained for C3O3K3 while the highest H-L gap of 2.07 eV is calculated for C3S3Li3. The obtained PDOS spectra further provide evidence for the superior electronic properties of these clusters. The clusters show excellent nonlinear optical properties as revealed from remarkable values (1.6 x 10(6) au) of static first hyperpolarizability. The controlling factors for hyperpolarizability are also explored by using conventional two-level model. The calculated values of beta(o) are correlated nicely with beta(tl). The crucial excitation energy is the key factor in controlling the first hyperpolarizability. In these excess electron clusters, the second hyperpolarizability (gamma(o)) response increases up to 4.3 x 10(9) au. Moreover, the calculated scattering hyperpolarizability (beta(HRS)) values are quite significant in these clusters and the highest value of 1.3 x 10(6) au is calculated for C3S3K3. Additionally, these clusters also possess larger dynamic nonlinearities. The dynamic second hyperpolarizability with dc-Kerr effect increases up to 1.0 x 10(11) au. The remarkable values for refractive index (n(2)) also suggest the excellent nonlinearity of these superalkali clusters. (C) 2021 Elsevier Inc. All rights reserved.

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