The stopping power of heavy ions for energies below 0.2 MeV/nucleon measured by the semi-thick target method

Pasternak, A. A.; Sankowska, I.; Tucholski, A.; Srebrny, J.; Morek, T.; Droste, Ch.; Grodner, E.; Sałata, M.; Mierzejewski, J.; Kisieliński, M.; Kowalczyk, M.; Perkowski, J.; Nowicki, Ł.; Ratajczak, R.; Stonert, A.; Jagielski, J.; Gawlik, G.; Kownacki, J.; Kordyasz, A.; Korman, A.; Płóciennik, W.; Ruchowska, E.; Wolińska-Cichocka, M.

doi:10.1016/j.nima.2014.11.066

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Nuclear Stopping Power1

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2020

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“…The transfers of the energy are divided on two parts: (i) the inelastic collisions constitute the principal mode of energy loss; it acted of exchange of loads between the projectile and target atoms, of an ionization of the target atoms or excitation of the electrons [13][14][15][16] and (ii) the elastic collisions result primarily by displacements of the target atoms and thus in crystalline defects in the structure [7]. The stopping power of heavy charged particles at low energy using the semi-thick target method is described in detail in the literature [17].…”

Section: Nuclear Stopping Powermentioning

confidence: 99%

Nuclear Energy Loss and Range of Heavy Ions in SiO2, LiF and Kapton Polyatomic Targets: A Monte Carlo study

Asri¹,

Bounagui²,

Tahiri³

et al. 2020

International Journal of Engineering Research and Technology

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This paper is dedicated to study the nuclear energy loss in amorphous targets SiO2, LiF and Kapton for different charged incident particles at energy E > 0.01 keV, by using Monte Carlo simulations. The nuclear stopping power and mean range are investigated. However, the nuclear stopping power and its maximum increases with increasing the atomic number of charged particles. All results are compared with existing SRIM data, PSTAR and ASTAR values. Finally, using the Monte-Carlo simulation, a determination was also made of mean range of ions in amorphous targets at energies from 10 to 400 keV. Our results were compared with experimental data.

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