Javascript must be enabled to continue!
Growth of graphene on Al2O3 (0001) surface
View through CrossRef
At present, high quality graphene is synthesized mainly by chemical vapor deposition. It is crucial to decompose and adsorb methane (CH4) on the surface of substrate before CH4 grows into graphene. The graphene is grown mainly on metal substrate due to the catalytic effect of metal. It is difficult to grow graphene thin film on the surface of non-metallic substrate, especially on the surface of -Al2O3 (0001). In this paper, the density functional theory based generalized gradient approximation method is applied to simulating the nucleation of graphene on -Al2O3 (0001) surface, synthesized by chemical vapor deposition. First, we establish a scientific -Al2O3 (0001) surface model, then simulate the decomposition process of CH4 on -Al2O3 (0001) surface by calculating the adsorption sites and adsorption configurations of groups and atoms. Finally, we investigate the groups of CH4 decomposition and atom coupling process on -Al2O3 (0001) surface. The results show that the CH3 groups, C and H atoms are preferentially adsorbed at the top of the O atoms, and the adsorption energies are -2.428 eV,-4.903 eV, and -4.083 eV, respectively. The CH2 and CH groups are preferentially adsorbed on the bridge between O and Al atoms with the adsorption energies of -4.460 eV and -3.940 eV, respectively. The decomposition of CH4 on -Al2O3 (0001) surface is an endothermic process. It requires higher energy and cross reactive energy barrier for CH4 to be completely decomposed into C atom, which makes it difficult that the C atom stays on the substrate surface. The coupling process among CH groups on the surface of -Al2O3 (0001) is an exothermic process. When CH and CH groups are coupled, the energy of the system decreases by 4.283 eV. When (CH)2 and CH groups are coupled, the energy of the system decreases by 3.740 eV. The (CH)x can be obtained by continuous migration and coupling between the CH groups on the surface of the -Al2O3 (0001), and (CH)x group is a precursor of graphene growth. The energy of the system decreases in the process. The above results show that the activated atom or group of graphene nucleation is not C atom but CH group. The CH group migration and aggregation on the surface of -Al2O3 (0001) give priority to the formation of lower energy (CH)x structure. In order to better understand the microscopic growth process of graphene on sapphire, it is important to study the role of (CH)x in the surface of sapphire for revealing the nucleation mechanism of graphene.
Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
Title: Growth of graphene on Al2O3 (0001) surface
Description:
At present, high quality graphene is synthesized mainly by chemical vapor deposition.
It is crucial to decompose and adsorb methane (CH4) on the surface of substrate before CH4 grows into graphene.
The graphene is grown mainly on metal substrate due to the catalytic effect of metal.
It is difficult to grow graphene thin film on the surface of non-metallic substrate, especially on the surface of -Al2O3 (0001).
In this paper, the density functional theory based generalized gradient approximation method is applied to simulating the nucleation of graphene on -Al2O3 (0001) surface, synthesized by chemical vapor deposition.
First, we establish a scientific -Al2O3 (0001) surface model, then simulate the decomposition process of CH4 on -Al2O3 (0001) surface by calculating the adsorption sites and adsorption configurations of groups and atoms.
Finally, we investigate the groups of CH4 decomposition and atom coupling process on -Al2O3 (0001) surface.
The results show that the CH3 groups, C and H atoms are preferentially adsorbed at the top of the O atoms, and the adsorption energies are -2.
428 eV,-4.
903 eV, and -4.
083 eV, respectively.
The CH2 and CH groups are preferentially adsorbed on the bridge between O and Al atoms with the adsorption energies of -4.
460 eV and -3.
940 eV, respectively.
The decomposition of CH4 on -Al2O3 (0001) surface is an endothermic process.
It requires higher energy and cross reactive energy barrier for CH4 to be completely decomposed into C atom, which makes it difficult that the C atom stays on the substrate surface.
The coupling process among CH groups on the surface of -Al2O3 (0001) is an exothermic process.
When CH and CH groups are coupled, the energy of the system decreases by 4.
283 eV.
When (CH)2 and CH groups are coupled, the energy of the system decreases by 3.
740 eV.
The (CH)x can be obtained by continuous migration and coupling between the CH groups on the surface of the -Al2O3 (0001), and (CH)x group is a precursor of graphene growth.
The energy of the system decreases in the process.
The above results show that the activated atom or group of graphene nucleation is not C atom but CH group.
The CH group migration and aggregation on the surface of -Al2O3 (0001) give priority to the formation of lower energy (CH)x structure.
In order to better understand the microscopic growth process of graphene on sapphire, it is important to study the role of (CH)x in the surface of sapphire for revealing the nucleation mechanism of graphene.
Related Results
Characterization and preliminary application of top-gated graphene ion-sensitive field effect transistors
Characterization and preliminary application of top-gated graphene ion-sensitive field effect transistors
Graphene, a 2-dimensional material, has received increasing attention due to its unique physicochemical properties (high surface area, excellent conductivity, and high mechanical s...
Preparation of Graphene Fibers
Preparation of Graphene Fibers
Graphene owns intriguing properties in electronic, thermal, and mechanic with unique two-dimension (2D) monolayer structure. The new member of carbon family has not only attracted ...
(Invited) Excellent Wetting Behavior of Yttria on 2D Materials
(Invited) Excellent Wetting Behavior of Yttria on 2D Materials
A high quality yttrium oxide (yttria, Y2O3) dielectric has been grown on different carbon derivatives materials (carbon nanotubes, exfoliated graphene, chemical vapor deposition gr...
In-Situ Hydrogen-Induced Defects on the Single Layer CVD Growth Graphene
In-Situ Hydrogen-Induced Defects on the Single Layer CVD Growth Graphene
In this paper we present in-situ hydrogen-induced defects on the single layer CVD growth graphene sheets with reactive terminated edges and holes within the graphene matrix. The sa...
Exploring defects and induced magnetism in epitaxial graphene films
Exploring defects and induced magnetism in epitaxial graphene films
Graphene has been demonstrated to have unique properties not only in its virgin state but also by altering its environment through rotations in bilayer graphene, doping, and creati...
Inadekvát, aránytalan sinuscsomó-tachycardia: egy régi szívritmuszavar új megvilágításban (II.)
Inadekvát, aránytalan sinuscsomó-tachycardia: egy régi szívritmuszavar új megvilágításban (II.)
Összefoglaló.
Bevezetés: Az inadekvát, aránytalan sinuscsomó-tachycardia a
szív nomotop ingerképzési zavarával járó, nem ritka klinikai szin...
Karakterisasi Sensor Liquefied Petroleum Gas (LPG) dari Bahan SnO2 Didoping dengan Al2O3
Karakterisasi Sensor Liquefied Petroleum Gas (LPG) dari Bahan SnO2 Didoping dengan Al2O3
Karakterisasi terhadap sensor gas LPG dari bahan SnO2 didoping dengan Al2O3 telah dilakukan. Sampel dibuat dengan persentase doping 0%, 2%, 4%, 6%, 8% dan 10% mol terhadap bahan da...
Impact on Wrinkled Graphene
Impact on Wrinkled Graphene
Abstract
We investigated wrinkle-free single layer graphene and graphene with various wrinkles to examine their fracture toughness during an impact with a silver nan...

