Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Structure of BP3S monolayer on Au(111)

View through CrossRef
The first-principle technique is employed to determine the structure of the BP3S monomer, the structures of the molecular chains and monolayers on virtual Au(111), and the atomic structure of BP3S/Au(111) adsorption system. The results show that the BP3S monomer presents a symmetric structure, and the angle between two benzene rings is 3510. At first, many BP3S monomers are assembled into one stable molecular chain in the virtual Au(111), the distance between the neighbor monmers is 0.516 nm, and the bind energy between the monmer and the molecular chain is 0.071 eV. It is a self-assembly system. Then many molecular chains are assembled into two stable monolayers in the virtual Au(111)-(37) and Au(111)-(313), and their coverages are 0.20 ML and 0.14 ML, respectively. In the virtual Au(111)-(37) and Au(111)-(313), the angles between the molecular chains and the virtual surface are 60 and 30, respectively, and the binding energies between the monmer and two monolayers are 0.101 eV and 0.125 eV, respectively. They are both the self-assembly systems. Finally, two monolayers are adsorbed on the Au(111)-(37) and Au(111)-(313) at four adsorption sites. The S atom is easy to obtain two electrons and turn into S2- ion, and the Au atom is easy to lose one electron and become Au+ ion, so the bridge site(two Au+ ions) is more stable than the top site(one Au+ ion), while the hcp and fcc hollow sites(three Au+ ions) are both unstable. In the Au(111)-(37), the chemisorption energy of the bridge site(-1.879 eV) is lower than that of the top site(-1.511 eV). And in the Au(111)-(313), the chemisorption energy of the bridge site(-1.691 eV) is lower than that of the top site(-1.492 eV). The results are confirmed in the other S-Au adsorption systems, such as the C6H13S/Au(111). A comparison between the structures of the BP3S monolayer before and after being adsorbed on Au(111) clearly shows that the structural parameters of the adsorption system depend mainly on the interaction in the monolayer, and that the contribution of Au(111) to the structure of the monolayer is weak. These results are confirmed in the other self-assembly adsorption systems.
Acta Physica Sinica, Chinese Physical Society and Institute of Physics, Chinese Academy of Sciences
Title: Structure of BP3S monolayer on Au(111)
Description:
The first-principle technique is employed to determine the structure of the BP3S monomer, the structures of the molecular chains and monolayers on virtual Au(111), and the atomic structure of BP3S/Au(111) adsorption system.
The results show that the BP3S monomer presents a symmetric structure, and the angle between two benzene rings is 3510.
At first, many BP3S monomers are assembled into one stable molecular chain in the virtual Au(111), the distance between the neighbor monmers is 0.
516 nm, and the bind energy between the monmer and the molecular chain is 0.
071 eV.
It is a self-assembly system.
Then many molecular chains are assembled into two stable monolayers in the virtual Au(111)-(37) and Au(111)-(313), and their coverages are 0.
20 ML and 0.
14 ML, respectively.
In the virtual Au(111)-(37) and Au(111)-(313), the angles between the molecular chains and the virtual surface are 60 and 30, respectively, and the binding energies between the monmer and two monolayers are 0.
101 eV and 0.
125 eV, respectively.
They are both the self-assembly systems.
Finally, two monolayers are adsorbed on the Au(111)-(37) and Au(111)-(313) at four adsorption sites.
The S atom is easy to obtain two electrons and turn into S2- ion, and the Au atom is easy to lose one electron and become Au+ ion, so the bridge site(two Au+ ions) is more stable than the top site(one Au+ ion), while the hcp and fcc hollow sites(three Au+ ions) are both unstable.
In the Au(111)-(37), the chemisorption energy of the bridge site(-1.
879 eV) is lower than that of the top site(-1.
511 eV).
And in the Au(111)-(313), the chemisorption energy of the bridge site(-1.
691 eV) is lower than that of the top site(-1.
492 eV).
The results are confirmed in the other S-Au adsorption systems, such as the C6H13S/Au(111).
A comparison between the structures of the BP3S monolayer before and after being adsorbed on Au(111) clearly shows that the structural parameters of the adsorption system depend mainly on the interaction in the monolayer, and that the contribution of Au(111) to the structure of the monolayer is weak.
These results are confirmed in the other self-assembly adsorption systems.

Related Results

Driving Biomineralisation Using Soft Templation
Driving Biomineralisation Using Soft Templation
<p>Sea shells, bones and teeth are three examples of Nature's unrivalled ability to produce complex hierarchical structures from simple inorganic materials. Unlike the synthe...
First-principles study of electronic structure and optical properties of monolayer defective tellurene
First-principles study of electronic structure and optical properties of monolayer defective tellurene
Monolayer tellurene is a novel two-dimensional semiconductor with excellent intrinsic properties. It is helpful in understanding doping and scattering mechanism to study the electr...
Cyclic Control of the Surface Properties of a Monolayer‐Functionalized Electrode by the Electrochemical Generation of Hg Nanoclusters
Cyclic Control of the Surface Properties of a Monolayer‐Functionalized Electrode by the Electrochemical Generation of Hg Nanoclusters
AbstractHg2+ ions are bound to a 1,4‐benzenedimethanethiol (BDMT) monolayer assembled on a Au electrode. Electrochemical reduction of the Hg2+–BDMT monolayer to Hg+–BDMT (at E°=0.4...
Extraction of Synovial Fluid from the Non-Effusive Pathologic Knee with Pneumatic Compression
Extraction of Synovial Fluid from the Non-Effusive Pathologic Knee with Pneumatic Compression
Objectives – Aspiration of synovial fluid from non-effusive joints is undertaken for the diagnosis of crystal-associated arthritis, biomarker analysis, and to con...
Physical Review B. Condensed Matter and Materials Physics
Physical Review B. Condensed Matter and Materials Physics
The atomic and electronic structure of the lattice-mismatched h-BN/Pt(111) and h-BN/Rh(111) interfaces formed by pyrolitic reactions with vaporized borazine has been studied by l...
MBE Growth and Characterization of Graphene on Well-Defined Cobalt Oxide Surfaces: Graphene Spintronics without Spin Injection
MBE Growth and Characterization of Graphene on Well-Defined Cobalt Oxide Surfaces: Graphene Spintronics without Spin Injection
The direct growth of graphene by scalable methods on magnetic insulators is important for industrial development of graphene-based spintronic devices, and a route towards substrate...
Interlayer molecular diffusion and thermodynamic equilibrium in organic heterostructures on a metal electrode
Interlayer molecular diffusion and thermodynamic equilibrium in organic heterostructures on a metal electrode
In this paper, we investigate by photoemission the electronic properties of an organic/organic interface consisting in a strong electron acceptor hexaazatriphenylene-hexacarbonitri...
Assessment of 18F-PBR-111 in the Cuprizone Mouse Model of Multiple Sclerosis
Assessment of 18F-PBR-111 in the Cuprizone Mouse Model of Multiple Sclerosis
The study aims to assess site assessment of the performance of 18F-PBR-111 as a neuroinflammation marker in the cuprizone mouse model of multiple sclerosis (MS). 18F-PBR-111 PET im...

Back to Top