latent track
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Author(s):  
A. Janse van Vuuren ◽  
M.M. Saifulin ◽  
V.A. Skuratov ◽  
J.H. O'Connell ◽  
G. Aralbayeva ◽  
...  

2018 ◽  
Author(s):  
Sanjeev Kumar ◽  
Jyoti Shakya ◽  
Tanmay Mahanta ◽  
Tanuja Mohanty

2016 ◽  
Vol 253 (11) ◽  
pp. 2144-2149 ◽  
Author(s):  
Jacques O'Connell ◽  
Vladimir Skuratov ◽  
Arno Janse van Vuuren ◽  
Maxim Saifulin ◽  
Abdirash Akilbekov
Keyword(s):  

Author(s):  
J.H. O’Connell ◽  
V.A. Skuratov ◽  
A. Akilbekov ◽  
A. Zhumazhanova ◽  
A. Janse van Vuuren
Keyword(s):  

Author(s):  
A. Al’zhanova ◽  
A. Dauletbekova ◽  
F. Komarov ◽  
L. Vlasukova ◽  
V. Yuvchenko ◽  
...  
Keyword(s):  

2016 ◽  
Vol 18 (36) ◽  
pp. 25421-25433 ◽  
Author(s):  
Pavel Y. Apel ◽  
Valery V. Bashevoy ◽  
Irina V. Blonskaya ◽  
Nikolay E. Lizunov ◽  
Oleg L. Orelovitch ◽  
...  

Asymmetric etching of ion tracks is strongly affected by osmotic flow which has a determinative effect on nanopore geometry. As a result, the narrowest part of the pore evolves through a variety of configurations.


Author(s):  
Stanislav Minárik

Abstract While passing swift heavy ion through a material structure, it produces a region of radiation affected material which is known as a "latent track". Scattering motions of electrons interacting with a swift heavy ion are dominant in the latent track region. These phenomena include the electron impurity and phonon scattering processes modified by the interaction with the ion projectile as well as the Coulomb scattering between two electrons. In this paper, we provide detailed derivation of a 3D Boltzmann scattering equation for the description of the relative scattering motion of such electrons. Phase-space distribution function for this non-equilibrioum system of scattering electrons can be found by the solution of mentioned equation.


2015 ◽  
Vol 12 (22) ◽  
pp. 20150771-20150771 ◽  
Author(s):  
Dongdong Zhao ◽  
Hongxia Liu ◽  
Shulong Wang ◽  
Qianqiong Wang ◽  
Chenxi Fei ◽  
...  

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