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Anisotropic Impact Sensitivity of Metal-Free Molecular Perovskite High-Energetic Material (C(6)H(14)N(2))(NH(2)NH(3))(ClO(4))(3) by First-Principles Study

[Image: see text] Density functional theory simulations were carried out to investigate energetic molecular perovskite (C(6)H(14)N(2))(NH(2)NH(3))(ClO(4))(3) which was a new type energetic material promising for future application. The electronic properties, surface energy, and hydrogen bonding of (...

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Detalles Bibliográficos
Autores principales: Li, Qiaoli, Li, Shenshen, Qu, Minghe, Xiao, Jijun
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9134386/
https://www.ncbi.nlm.nih.gov/pubmed/35647461
http://dx.doi.org/10.1021/acsomega.2c00878
Descripción
Sumario:[Image: see text] Density functional theory simulations were carried out to investigate energetic molecular perovskite (C(6)H(14)N(2))(NH(2)NH(3))(ClO(4))(3) which was a new type energetic material promising for future application. The electronic properties, surface energy, and hydrogen bonding of (100), (010), (011), (101), (111) surfaces were studied, and the anisotropic impact sensitivity of these surfaces were reported. By comparing the values of the band gaps for different surface structures, we found that the (100) surface has the lowest sensitivity, while the (101) surface was considered to be much more sensitive than the others. The results for the total density of states further validated the previous conclusion obtained from the band gap. Additionally, the calculated surface energy indicated that surface energy was positively correlated with impact sensitivity. Hydrogen bond content of the surface structures showed distinct variability according to the two-dimensional fingerprint plots. In particular, the hydrogen bond content of (100) surface was higher than that of other surfaces, indicating that the impact sensitivity of (100) surface is the lowest.