2017
DOI: 10.1142/s0217984917500373
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Ehrlich–Schwöbel barriers and adsorption of Au, Cu and Ag stepped (100) surfaces

Abstract: We use a combination of quenched molecular dynamics and embedded atom method to calculate the activation energy barriers for the hopping and exchange mechanisms of Au, Ag or Cu on Au(100), Ag(100) or Cu(100) stepped surfaces. Our findings show that the Ehrlich–Schwöbel (ES) barriers for an adatom to undergo jump or exchange at a step edge are found to be dependent of the nature of substrate stepped surfaces. We also find that the ES barriers for the hopping processes are too high, except for Cu/Au(100). While … Show more

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Cited by 7 publications
(5 citation statements)
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“…This behavior stems from the presence of a sizeable ES barrier at the step edge which hinders adatom diffusion across the steps 11 . In fact, the ES barrier corresponds to an additional energy needed for an adatom to jump across the terraces 23 , which characterize the (111)A vicinal surface, and decreases the diffusivity in the direction. Therefore, Ga adatoms at T > 400 °C predominantly migrate in the direction along steps in a strongly anisotropic way, this way approaching a quasi-one-dimensional diffusion behavior.
Figure 6( a ) AFM image of QDs grown on GaAs(111)A with 2° miscut towards at 300 °C (2 × 2 μm 2 , sample T1), corresponding ( c ) spatial dispersion of neighboring QDs (0.16 × 0.16 μm 2 ) and ( e ) CZD obtained from voronoi tessellation, fitted by GWD.
…”
Section: Resultsmentioning
confidence: 99%
“…This behavior stems from the presence of a sizeable ES barrier at the step edge which hinders adatom diffusion across the steps 11 . In fact, the ES barrier corresponds to an additional energy needed for an adatom to jump across the terraces 23 , which characterize the (111)A vicinal surface, and decreases the diffusivity in the direction. Therefore, Ga adatoms at T > 400 °C predominantly migrate in the direction along steps in a strongly anisotropic way, this way approaching a quasi-one-dimensional diffusion behavior.
Figure 6( a ) AFM image of QDs grown on GaAs(111)A with 2° miscut towards at 300 °C (2 × 2 μm 2 , sample T1), corresponding ( c ) spatial dispersion of neighboring QDs (0.16 × 0.16 μm 2 ) and ( e ) CZD obtained from voronoi tessellation, fitted by GWD.
…”
Section: Resultsmentioning
confidence: 99%
“…[ 38 ] In addition, EAM model is very accurate for highly symmetrical structures (such as fcc). [ 38,39 ] Daw and Baskes [ 37,40 ] developed this method for calculating the potential energy of each atom i as a sum of a pair contribution and an embedding term as given by the following equation: E i = 1 2 140%true j i j ϕ i j ( r i j ) + 140%true i F ( ρ i ) where ϕ i j is the pair potential and r i j is the distance between atom i and atom j ; F ( ρ i ) is the embedding energy function required to place atom i in an electron density ρ i characterizing the environment of that atom, ρ i = 140%true j i j ρ h ( r i j ) where ρ h ( r i j ) is the sum of the electron densities of all the other atoms j at the location of atom i . This potential is expressed essentially as a function of the separation distance r i j of the atoms in the form of different functions.…”
Section: Simulation Methods and Modelmentioning
confidence: 99%
“…[38] In addition, EAM model is very accurate for highly symmetrical structures (such as fcc). [38,39] Daw and Baskes [37,40] developed this method for calculating the potential energy of each atom i as a sum of a pair contribution and an embedding term as given by the following equation:…”
Section: Eammentioning
confidence: 99%
“…7a with the triangular dots. In this latter simulation, the recombination mechanism was artificially suppressed with the help of forbidding atom transfer from the middle to the lowerst terrace through the lower combinatory step by setting an infinitely high Schwöbel barrier [34].…”
Section: Resultsmentioning
confidence: 99%