Thermal spike model for heavy ion induced desorption from surfaces

1987 ◽  
Vol 86 (1) ◽  
pp. 443-453 ◽  
Author(s):  
Robert R. Lucchese
1997 ◽  
Vol 248-249 ◽  
pp. 21-32 ◽  
Author(s):  
C. Dufour ◽  
S. Hemon ◽  
F. Gourbilleau ◽  
E. Paumier ◽  
E. Dooryhee

2006 ◽  
Vol 3 (5) ◽  
pp. 320-326
Author(s):  
I. V. Amirkhanov ◽  
A. Yu. Didyk ◽  
N. R. Sarker ◽  
I. Sarhadov ◽  
V. K. Semina ◽  
...  

RSC Advances ◽  
2016 ◽  
Vol 6 (64) ◽  
pp. 58950-58956 ◽  
Author(s):  
Vantari Siva ◽  
Abdelhak Chettah ◽  
Biswarup Satpati ◽  
S. Ojha ◽  
D. Kanjilal ◽  
...  

Enhanced surface and interface diffusion in Ni–Bi bilayers has been observed using 100 MeV Au ion irradiation. The experimental observations were demonstrated using thermal spike model calculations.


2019 ◽  
Vol 21 (30) ◽  
pp. 16634-16646
Author(s):  
Paramita Patra ◽  
S. A. Khan ◽  
M. Bala ◽  
D. K. Avasthi ◽  
S. K. Srivastava

A combination of density functional theory computations and swift heavy ion (SHI) mixing experiments is employed to assess the thermal spike model of SHI–matter interactions.


2020 ◽  
Vol 229 ◽  
pp. 05001
Author(s):  
Christelle Stodel ◽  
Marcel Toulemonde ◽  
Christoph Fransen ◽  
Bertrand Jacquot ◽  
Emmanuel Clément ◽  
...  

High electronic excitations in radiation of metallic targets with swift heavy ion beams at the coulomb barrier play a dominant role in the damaging processes of some metals. The inelastic thermal spike model was developed to describe tracks in materials and is applied in this paper to some systems beams/targets employed recently in some nuclear physics experiments. Taking into account the experimental conditions and the approved electron-phonon coupling factors, the results of the calculation enable to interpret the observation of the fast deformation of some targets.


1994 ◽  
Vol 373 ◽  
Author(s):  
G. Szenes

AbstractA model based on the assumption of a Gaussian temperature distribution in the thermal spike well accounts for the basic features of latent track formation. In good agreement with the observations it predicts a logarithmic variation of the track size for 2.7≥Se/Set≥1 and a linear variation for Se/Set≥2.7, where Se is the electronic stopping power and Set is a threshold value. The model also provides a quantitative relation between Set and the thermal properties of the target. A weak temperature dependence of track formation is predicted in agreement with the experiments.


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