Matrix effect of bombardment-induced Gibbsian segregation on Cu depletion at a Cu x Ni100?x subsurface

Zheng, LP; Rs, Li; Xia, Xq; Li, MQ; My, Li

doi:10.1007/bf01540117

Cited by 2 publications

(5 citation statements)

References 18 publications

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“…Our MC simulation program series has been employed in investigating particle motions exclusively along a straight-line segment in amorphous and crystalline ,− materials. This MC simulation program , utilizes a binary collision model based on the Moliere potential for the ion−atom (or atom−atom) interactions and on the continuously slowing approximation for electronic stopping, at low temperatures.…”

Section: Simulation Program Seriesmentioning

confidence: 99%

Isotopic Mass Effects for Low-Energy Ion Channeling in Single-Wall Carbon Nanotubes

Zheng

Zhang

et al. 2008

J. Phys. Chem. C

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Monte Carlo (MC) simulation studies of isotopic mass effects have been conducted, for low-energy channeling of 12C and 13C ions in single-wall carbon nanotubes. It is found in MC simulations that (ΨC for 12C/ΨC for 13C) = (13/12)1/2, for the same incident energies. Here, ΨC for 12C is the critical angle for 12C channeling, andΨC for 13C is the critical angle for 13C channeling. This work shows the mass effect to be the incident momentum one, but a recent work (Moura, C. S.; Amaral, L. J. Phys. Chem. B 2005, 109, 13515) considered it to be the energy transfer effect. Our work disagrees with that of Moura and Amaral.

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Section: Simulation Program Seriesmentioning

confidence: 99%

Isotopic Mass Effects for Low-Energy Ion Channeling in Single-Wall Carbon Nanotubes

Zheng

Zhang

et al. 2008

J. Phys. Chem. C

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“…Our Monte Carlo (MC) simulation program series has been employed in investigating particle motions exclusively along a straight-line segment in amorphous and crystalline [12,19,20,22] materials. The present static MC simulation program utilizes a binary collision model [2,[12][13][14][15][16][17][18][19][20][21][22] based on the Moliere potential for the ion-atom (or atom-atom) interaction and on the continuously slowing approximation for electronic stopping, at low temperatures.…”

Section: Simulation Program Seriesmentioning

confidence: 99%

“…For binary interactions, transferred factor c(M, m, h i?1 ) is classical [2,[12][13][14][15][16][17][18][19][20][21][22], that is,…”

Section: Derivation Of Formulas Of the Ion-deposited Energiesmentioning

confidence: 99%

“…The present static MC simulation program utilizes a binary collision model [2,[12][13][14][15][16][17][18][19][20][21][22] based on the Moliere potential for the ion-atom (or atom-atom) interaction and on the continuously slowing approximation for electronic stopping, at low temperatures. Carbon nanotubes (the MWCNT) in a super-lattice are kept in a position of equilibrium by van der Waals forces, and the gap between the walls of neighboring nanotubes is usually *0.315 nm.…”

Section: Simulation Program Seriesmentioning

confidence: 99%

“…Therefore, for better understanding of these mechanisms [2,[7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22][23], it might be informative that we calculate the deposited energies of various energetic ions, especially at incident energies up to hundreds keV. This is the main goal of our present simulation works.…”

Section: Introductionmentioning

confidence: 99%

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Nuclear point mass effects in the interaction of energetic ion with carbon nanotubes

et al. 2016

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We have calculated deposited energies of various energetic ions in carbon nanotubes, to study nuclear point mass effects, with the help of a static Monte Carlo (MC) simulation program. As a result of nuclear point mass effects, we show that at the same incident energy, the iondeposited energy maximizes, while its mass has intermediate mass values, such as 11 B, 12 C and 14 N ion masses, under hundreds keV 4 He, 11 B, 12 C, 14 N, 20 Ne, 28 Si and 40 Ar ion irradiations of a thin-walled carbon nanotube. We also show that at the same incident energy, the coordination defect number maximizes, while its mass has an intermediate mass ( 20 Ne) value, under hundreds keV 4 He, 20 Ne and 40 Ar ion irradiations of the thin-walled nanotube. We derive an ion-deposited energy formula to analyze these maximum phenomena, and compare the MC simulation results with the MD (molecular dynamics) ones.

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Matrix effect of bombardment-induced Gibbsian segregation on Cu depletion at a Cu x Ni100?x subsurface

Cited by 2 publications

References 18 publications

Isotopic Mass Effects for Low-Energy Ion Channeling in Single-Wall Carbon Nanotubes

Isotopic Mass Effects for Low-Energy Ion Channeling in Single-Wall Carbon Nanotubes

Nuclear point mass effects in the interaction of energetic ion with carbon nanotubes

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