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First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties

[Image: see text] This work examines six structures (P4̅3m, P4(2)nm, R3m, P2(1)/c, R3̅m, and C2/m) of alkaline earth metal cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba) using first-principles calculations. The symmetries of P4̅3m, P4(2)nm, and R3m reflect a variation of Pn3̅m, previously reported as...

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Autores principales: Leong, Pak Kin, Sekine, Toshimori, Tam, Kuan Vai, Tam, Sok I., Tang, Chi Pui
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9878677/
https://www.ncbi.nlm.nih.gov/pubmed/36713722
http://dx.doi.org/10.1021/acsomega.2c05667
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author Leong, Pak Kin
Sekine, Toshimori
Tam, Kuan Vai
Tam, Sok I.
Tang, Chi Pui
author_facet Leong, Pak Kin
Sekine, Toshimori
Tam, Kuan Vai
Tam, Sok I.
Tang, Chi Pui
author_sort Leong, Pak Kin
collection PubMed
description [Image: see text] This work examines six structures (P4̅3m, P4(2)nm, R3m, P2(1)/c, R3̅m, and C2/m) of alkaline earth metal cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba) using first-principles calculations. The symmetries of P4̅3m, P4(2)nm, and R3m reflect a variation of Pn3̅m, previously reported as occurring on Be(CN)(2) and Mg(CN)(2) in X-ray diffraction studies, while the symmetries of P2(1)/c, R3̅m, and C2/m were selected from the P3̅m1 symmetry found using Mg(OH)(2) as the initial structures, with −OH being replaced by −CN. The band structure, density of states, and phonon properties of all A(CN)(2) structures were then investigated using density functional theory (DFT), with a generalized gradient approximation (GGA) applied for the exchange and correlation energy values. The simulation results for the phonon spectra indicate that the stable structures are Be(CN)(2) (P4̅3m, P4(2)nm, and C2/m), Mg(CN)(2) (P4̅3m, P4(2)nm, and C2/m), Ca(CN)(2) (P2(1)/c), Sr(CN)(2) (P2(1)/c and R3̅m), and Ba(CN)(2) (R3̅m) at 0 GPa. For the effects of high pressure, Ca(CN)(2) and Sr(CN)(2) were thus found to be stable as C2/m at pressures above 10 and 3 GPa, respectively, while Ca(CN)(2) is as stable as R3̅m above 15 GPa. In the calculated band structures, all of the compounds with the C2/m structure demonstrated good conductivity, while the other structures have a band gap range of 2.83–6.33 eV.
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spelling pubmed-98786772023-01-27 First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties Leong, Pak Kin Sekine, Toshimori Tam, Kuan Vai Tam, Sok I. Tang, Chi Pui ACS Omega [Image: see text] This work examines six structures (P4̅3m, P4(2)nm, R3m, P2(1)/c, R3̅m, and C2/m) of alkaline earth metal cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba) using first-principles calculations. The symmetries of P4̅3m, P4(2)nm, and R3m reflect a variation of Pn3̅m, previously reported as occurring on Be(CN)(2) and Mg(CN)(2) in X-ray diffraction studies, while the symmetries of P2(1)/c, R3̅m, and C2/m were selected from the P3̅m1 symmetry found using Mg(OH)(2) as the initial structures, with −OH being replaced by −CN. The band structure, density of states, and phonon properties of all A(CN)(2) structures were then investigated using density functional theory (DFT), with a generalized gradient approximation (GGA) applied for the exchange and correlation energy values. The simulation results for the phonon spectra indicate that the stable structures are Be(CN)(2) (P4̅3m, P4(2)nm, and C2/m), Mg(CN)(2) (P4̅3m, P4(2)nm, and C2/m), Ca(CN)(2) (P2(1)/c), Sr(CN)(2) (P2(1)/c and R3̅m), and Ba(CN)(2) (R3̅m) at 0 GPa. For the effects of high pressure, Ca(CN)(2) and Sr(CN)(2) were thus found to be stable as C2/m at pressures above 10 and 3 GPa, respectively, while Ca(CN)(2) is as stable as R3̅m above 15 GPa. In the calculated band structures, all of the compounds with the C2/m structure demonstrated good conductivity, while the other structures have a band gap range of 2.83–6.33 eV. American Chemical Society 2023-01-11 /pmc/articles/PMC9878677/ /pubmed/36713722 http://dx.doi.org/10.1021/acsomega.2c05667 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Leong, Pak Kin
Sekine, Toshimori
Tam, Kuan Vai
Tam, Sok I.
Tang, Chi Pui
First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title_full First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title_fullStr First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title_full_unstemmed First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title_short First-Principles Calculations with Six Structures of Alkaline Earth Metal Cyanide A(CN)(2) (A = Be, Mg, Ca, Sr, and Ba): Structural, Electrical, and Phonon Properties
title_sort first-principles calculations with six structures of alkaline earth metal cyanide a(cn)(2) (a = be, mg, ca, sr, and ba): structural, electrical, and phonon properties
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9878677/
https://www.ncbi.nlm.nih.gov/pubmed/36713722
http://dx.doi.org/10.1021/acsomega.2c05667
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