Graphenyldiene: A new sp2-graphene-like nanosheet

The race and the discovery of novel two-dimensional (2D) carbon-based materials have been intensified because many are suitable for energy storage systems, thermoelectric devices, and catalysis applications. Therefore, this study introduces to the scientific community a novel 2D nanosheet named grap...

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Main Authors: José A.S. Laranjeira, Nicolas F. Martins, Pablo A. Denis, Julio R. Sambrano
Format: Article
Language:English
Published: Elsevier 2024-03-01
Series:Carbon Trends
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2667056924000026
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author José A.S. Laranjeira
Nicolas F. Martins
Pablo A. Denis
Julio R. Sambrano
author_facet José A.S. Laranjeira
Nicolas F. Martins
Pablo A. Denis
Julio R. Sambrano
author_sort José A.S. Laranjeira
collection DOAJ
description The race and the discovery of novel two-dimensional (2D) carbon-based materials have been intensified because many are suitable for energy storage systems, thermoelectric devices, and catalysis applications. Therefore, this study introduces to the scientific community a novel 2D nanosheet named graphenyldiene (GPD), which is formed by arranging cyclobutadiene and bi-phenyl groups to create a monolayer with octadecagonal, hexagonal and tetragonal rings. The cohesive energy of GPD is only 1.37 and 0.65 eV/atom higher than graphene and biphenylene, respectively. Molecular dynamics simulations confirmed its structural and thermal stability. The GPD monolayer remains stable, with no significant deformations at around 1000 K, and the disintegration of the geometry occurs only at a temperature of 1500 K, which is characterized by the formation of an amorphous graphdiyne. The GPD electronic structure shows a direct band gap transition, 1.26 eV, at the Γ point. GPD is a promising alternative to electronic devices due to its carrier mobility of around 103.cm2/V.s. Also, the GPD satisfies the Born-Huang criterion for mechanical stability with elastic constants C11 = 157.62 N/m, C12 = 53.66 N/m and C66 = 51.98 N/m. The Bader's topological analysis indicated that all bonds have strong shared shell characteristics. Finally, the vibrational analysis identified 54 modes, where 21 are Raman active, with A1g and E2g modes dominating the spectrum at 1347, 1685 and 1697 cm−1.
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spelling doaj.art-cefd508ab1b94ab78ff0d8820265a0712024-03-16T05:09:50ZengElsevierCarbon Trends2667-05692024-03-0114100321Graphenyldiene: A new sp2-graphene-like nanosheetJosé A.S. Laranjeira0Nicolas F. Martins1Pablo A. Denis2Julio R. Sambrano3Modeling and Molecular Simulation Group, São Paulo State University, Bauru, SP, BrazilModeling and Molecular Simulation Group, São Paulo State University, Bauru, SP, BrazilComputational Nanotechnology, DETEMA, Facultad de Química, UDELAR, CC 1157, 11800 Montevideo, UruguayModeling and Molecular Simulation Group, São Paulo State University, Bauru, SP, Brazil; Corresponding author.The race and the discovery of novel two-dimensional (2D) carbon-based materials have been intensified because many are suitable for energy storage systems, thermoelectric devices, and catalysis applications. Therefore, this study introduces to the scientific community a novel 2D nanosheet named graphenyldiene (GPD), which is formed by arranging cyclobutadiene and bi-phenyl groups to create a monolayer with octadecagonal, hexagonal and tetragonal rings. The cohesive energy of GPD is only 1.37 and 0.65 eV/atom higher than graphene and biphenylene, respectively. Molecular dynamics simulations confirmed its structural and thermal stability. The GPD monolayer remains stable, with no significant deformations at around 1000 K, and the disintegration of the geometry occurs only at a temperature of 1500 K, which is characterized by the formation of an amorphous graphdiyne. The GPD electronic structure shows a direct band gap transition, 1.26 eV, at the Γ point. GPD is a promising alternative to electronic devices due to its carrier mobility of around 103.cm2/V.s. Also, the GPD satisfies the Born-Huang criterion for mechanical stability with elastic constants C11 = 157.62 N/m, C12 = 53.66 N/m and C66 = 51.98 N/m. The Bader's topological analysis indicated that all bonds have strong shared shell characteristics. Finally, the vibrational analysis identified 54 modes, where 21 are Raman active, with A1g and E2g modes dominating the spectrum at 1347, 1685 and 1697 cm−1.http://www.sciencedirect.com/science/article/pii/S2667056924000026GrapheneCarbon allotropeBiphenyldieneBiphenyleneGraphenyldiene
spellingShingle José A.S. Laranjeira
Nicolas F. Martins
Pablo A. Denis
Julio R. Sambrano
Graphenyldiene: A new sp2-graphene-like nanosheet
Carbon Trends
Graphene
Carbon allotrope
Biphenyldiene
Biphenylene
Graphenyldiene
title Graphenyldiene: A new sp2-graphene-like nanosheet
title_full Graphenyldiene: A new sp2-graphene-like nanosheet
title_fullStr Graphenyldiene: A new sp2-graphene-like nanosheet
title_full_unstemmed Graphenyldiene: A new sp2-graphene-like nanosheet
title_short Graphenyldiene: A new sp2-graphene-like nanosheet
title_sort graphenyldiene a new sp2 graphene like nanosheet
topic Graphene
Carbon allotrope
Biphenyldiene
Biphenylene
Graphenyldiene
url http://www.sciencedirect.com/science/article/pii/S2667056924000026
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AT juliorsambrano graphenyldieneanewsp2graphenelikenanosheet