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Calculations of Stopping Power, Straggling and Range Projected of FeKr+

Received: 6 March 2024    Accepted: 27 March 2024    Published: 17 May 2024
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Abstract

The present work consists of the simulation of the interaction of a beam of Kr+ ions with a solid iron target by the software SRIM (Stopping and Range of Ions In Matter). Our goal is to calculate different parameters related to sputtering and ion implantation in a target, such as the spatial distribution of implanted ions, the distributions of electronic and nuclear energy losses as a function of penetration depth and sputtering efficiency, as well as the damage created inside the target. The sputter induced photon spectroscopy technique was used to study the luminescence spectra of the species sputtered from Iron powder, during 5 keV Kr+ ions bombardment in vacuum better than 107 torr. The optical spectra recorded between 350 and 470 nm exhibit discrete lines which are attributed to neutral excited atoms of Iron (Fe). The experiments are also performed under 105 torr ultra-pure oxygen partial pressure. To ensure the maximum efficiency of molecular modification process, energy of irradiation was decided by using of SRIM software. Based on SRIM simulation of Iron ions interaction with Krypton, the areas on which effect of high energy ions will maximum were predicted. A comparative analysis of molecular before and after irradiation was carried out by scanning electron microscopy. The maximum change in Krypton morphology, in the form of destruction of walls, was appeared at a distance of about μm from the start point of Fe+ ions track inside the molecular. A substantiation of reason of wall degradation in this area was proposed.

Published in Engineering Physics (Volume 7, Issue 1)
DOI 10.11648/j.ep.20240701.11
Page(s) 1-9
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

SRIM 2013 Software, Stopping Power, Range Projected

References
[1] J. F. Ziegler at el, SRIM - The stopping and range of ions in matter, Nuclear Instruments and Methods in Physics Research B, 2010, 268, page 1818-1823.
[2] Berger, M. J, ESTAR, PSTAR, ASTAR, A PC package for calculating stopping powers and ranges of electrons, protons and helium ions, Version 2, International Atomic Energy Agency, nuclear data services, documentation series of the IAEA nuclear data section, 1993.
[3] National Research Council, Committee on the Biological Effects of Ionizing Radiation, Health Effects of Exposure to Low Levels of Ionizing Radiation, BEIR V, National Academy Press, Washington, D. C., 1990.
[4] Fred A. Mettler, Jr., M. D. and Arthur C. Upton, M. D. Medical Effects of Ionizing Radiation, Grune & Stratton, Inc., Orlando, Florida, 1995.
[5] Ahmed, S. N., physics and Engineering of Radiation Detection, Queen’s University, Kingston, Ontario, 2007 118-120.
[6] Y. H. Song, and Y. N. Wang, "Effect of ion-nucleus sizes on the electric stopping power for heavy ions in solids", Nucl. Instr. and Meth. in Phys. Res. B, 1998, 135, 124-127.
[7] W. Brandt, and M. Kitagawa, "Effective stopping-power charges of swift ions in condensed matter", Phys. Rev. B, 1982, 25, (9), 5631-5637.
[8] L. E. Porter, "Further observations of projectile-z dependence in target parameters of modified Bethe-Bloch theory", Int. J. Quantum Chem. 2003, 95, (4-5), 504-511.
[9] P. M. Echenique, R. M. Nieminen, J. C. Ashley, and R. Ritchie, "Nonlinear stopping power of an electron gas for slow ions", Phys. Rev. A, 1986, 33, (2), 897-904.
[10] J. F. Ziegler, Nucl. Instr. Meth. B, 2004, 1027, 219-220.
[11] J. F. Ziegler, "SRIM - the stopping and range of ions in matter",
[12] A. Jablonski, C. J. Powell, and S. Tanuma, Surf. Interface Anal. 37, 861 (2005).
[13] A. Jablonski, Prog. Surf. Sci, 2005, 79, (3).
[14] A. Jablonski, F. Salvat, and C. J. Powell, J. Phys. Chem. Ref. Data, 2004, (33), 409.
[15] F. Salvat, A. Jablonski, and C. J. Powell, Comput. Phys. Commun, 2005, 165, 157.
[16] ESTAR, PSTAR and ASTAR: Computer Codes for Calculating Stopping-Power and Range Tables for Electrons, Protons, and Helium Ions, Martin J. Berger* Ionizing Radiation Division National Institute of Standards and Technology Gaitherburg.
[17] Hunt, J. G., Dantas B. M., Azeredo, A. M. G. F. Visual Monte Carlo in-vivo in the CONRAD and IAEA Whole Body Counter Intercomparisons. In. Workshop on Uncertainty Assessment in Computational Dosimetry, Bologna, 2007
[18] J. C. Hsiao and K. Fong. Nature. 2004, 428 (6979), 218-220.
[19] T. Ozel, G. R. Bourret and C. a Mirkin. Nat Nanotechnol, 2015, 10 (4), 319-324.
[20] S. V. Trukhanov, A. V. Trukhanov, V. A. Turchenko, A. V. Trukhanov, E. L. Trukhanova, D. I. Tishkevich, V. M. Ivanov, T. I. Zubar, M. Salem, V. G. Kostishyn, L. V. Panina, D. A. Vinnik and S. A. Gudkova. Ceram Int, 2018, 44, (1), 290-300.
[21] C. R. Martin. Science, 1994, 266, (80), 1961-1966.
[22] E. Y. Kaniukov, A. L. Kozlovsky, D. I. Shlimas, M. V. Zdorovets, D. V. Yakimchuk, E. E. Shumskaya and K. K. Kadyrzhanov. J Surf Investig X-ray, Synchrotron Neutron Tech, 2017, 11, (1), 270-275.
[23] S. Y. Chou, P. R. Krauss and P. J. Renstrom. Science, 1996, 272, (5), (80), 85-87.
[24] D. I. Tishkevich, S. S. Grabchikov, L. S. Tsybulskaya, V. S. Shendyukov, S. S. Perevoznikov, S. V. Trukhanov, E. L. Trukhanova, A. V. Trukhanov and D. A. Vinnik. J Alloys Compd, 2018, 735, 1943-1948.
[25] S. E. Demyanov, E. Y. Kaniukov, A. V. Petrov, E. K. Belonogov, E. A. Streltsov, D. K. Ivanov, Y. A. Ivanova, C. Trautmann, H. Terryn, M. Petrova, J. Ustarroz and V. Sivakov. J Surf Investig X-ray, Synchrotron Neutron Tech, 2014, 8, (4), 805-813.
[26] E. Kaniukov, A. Kozlovsky, D. Shlimas, D. Yakimchuk, M. Zdorovets and K. Kadyrzhanov. IOP Conf Ser Mater Sci Eng, 2016, 110, 12013.
[27] N. A. Kalanda, G. G. Gorokh, M. V. Yarmolich, A. A. Lozovenko and E. Y. Kanyukov. Phys Solid State, 2016, 58, (2), 351-359.
[28] A. Cultrera, L. Boarino, G. Amato and C. Lamberti. J Phys D Appl Phys, 2014, 47, 015102, 1-8.
[29] E. Kaniukov, A. Shumskaya, D. Yakimchuk, A. Kozlovskiy, A. Ibrayeva and M. Zdorovets. NANO 2016 Nanophysics, Nanomater Interface Stud Appl. 2017 (2017) 79-91.
[30] J. Liu, B. Liu, Z. Ni, Y. Deng, C. Zhong and W. Hu. Electrochim Acta, 2014, 150, 146-150.
[31] M. P. Proenca, C. T. Sousa, J. Ventura and J. P. Araújo. Magn Nano- Microwires Des Synth Prop Appl. 2015 (2015) Electrochemical Synthesis and Magnetism of Magnetic Nanotubes.; 2015.
[32] W. Li, L. Liao, X. Xiao, X. Zhao, Z. Dai, S. Guo, W. Wu, Y. Shi, J. Xu, F. Ren and C. Jiang. Nano Res., 2014, 7, (11), 1691-1698.
[33] A. Solanki, S. Choudhary, V. R. Satsangi, R. Shrivastav and S. Dass. J Alloys Compd, 2013, 561, 114-120.
[34] I. P. Jain and G. Agarwal. Surf Sci Rep, 2011, 66, (3-4), 77-172.
[35] S. Dhara. Crit Rev Solid State Mater Sci, 2007, 32, (1-2), 1-50.
[36] S. Panchal and R. P. Chauhan. Phys E Low-Dimensional Syst Nanostructures, (November 2016) (2017), 87, 37-43.
[37] R. P. Chauhan and P. Rana. Radiat Meas, 2015, 83, 43-46.
[38] Computer simulation of atomic-displacement cascades in solids in the binary-collisions approximation, Mark T. Robinson, lan M. Torrens, PHYSICAL Review B, 15 june 1974 (9) 12.
[39] J. F. Ziegler, J. Biersack, and U. Littmark, “The stopping and range of ions in matter, 1985, vol. 1”, 1, Pergamon Press, New York.
[40] J. Ziegler, J. Biersack, and M. Ziegler, “Srim” the stopping and range of ions in matter, ion implantation press, 2008.
[41] J. Lindhard, M. Schar, and H. E. Schiøtt, Range concepts and heavy ion ranges, Munks-gaard Copenhagen, 1963.
[42] Junichiro Sameshima, Aya Takenaka, Yuichi Muraji, Shingo Ogawa, Masanobu Yoshikawa, Katsuaki Suganuma, Optimization of the depth resolution for profiling SiO/SiC interfaces by dual-beam TOF-SIMS combined with etching, Surf. Interface Anal, 2019, 51, 743.
[43] Pavel Andreevich Yunin, Yurii Nikolaevich Drozdov, Mikhail Nikolaevich Drozdov, A new approach to express ToF SIMS depth profiling, Surf. Interface Anal, 2015, 47, 771.
[44] Atsushi Murase, Takuya Mitsuoka, Mitsuhiro Tomita, Hisataka Takenaka, Hiromi Morita, An effect of measurement conditions on the depth resolution for low-energy dual-beam depth profiling using TOF-SIMS, Surf. Interface Anal, 2013, 45, 1261.
[45] H. Faik-Etienne, Étude de l'implantation ionique dans les miroirs multicouches Mo/Si: application aux optiques diffractives, Thèse de doctorat, Institut National des Sciences Appliquées de Toulouse, 2005.
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    Farjallah, M. (2024). Calculations of Stopping Power, Straggling and Range Projected of FeKr+. Engineering Physics, 7(1), 1-9. https://doi.org/10.11648/j.ep.20240701.11

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    ACS Style

    Farjallah, M. Calculations of Stopping Power, Straggling and Range Projected of FeKr+. Eng. Phys. 2024, 7(1), 1-9. doi: 10.11648/j.ep.20240701.11

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    AMA Style

    Farjallah M. Calculations of Stopping Power, Straggling and Range Projected of FeKr+. Eng Phys. 2024;7(1):1-9. doi: 10.11648/j.ep.20240701.11

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  • @article{10.11648/j.ep.20240701.11,
      author = {Mohamed Farjallah},
      title = {Calculations of Stopping Power, Straggling and Range Projected of FeKr+
    },
      journal = {Engineering Physics},
      volume = {7},
      number = {1},
      pages = {1-9},
      doi = {10.11648/j.ep.20240701.11},
      url = {https://doi.org/10.11648/j.ep.20240701.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ep.20240701.11},
      abstract = {The present work consists of the simulation of the interaction of a beam of Kr+ ions with a solid iron target by the software SRIM (Stopping and Range of Ions In Matter). Our goal is to calculate different parameters related to sputtering and ion implantation in a target, such as the spatial distribution of implanted ions, the distributions of electronic and nuclear energy losses as a function of penetration depth and sputtering efficiency, as well as the damage created inside the target. The sputter induced photon spectroscopy technique was used to study the luminescence spectra of the species sputtered from Iron powder, during 5 keV Kr+ ions bombardment in vacuum better than 107 torr. The optical spectra recorded between 350 and 470 nm exhibit discrete lines which are attributed to neutral excited atoms of Iron (Fe). The experiments are also performed under 105 torr ultra-pure oxygen partial pressure. To ensure the maximum efficiency of molecular modification process, energy of irradiation was decided by using of SRIM software. Based on SRIM simulation of Iron ions interaction with Krypton, the areas on which effect of high energy ions will maximum were predicted. A comparative analysis of molecular before and after irradiation was carried out by scanning electron microscopy. The maximum change in Krypton morphology, in the form of destruction of walls, was appeared at a distance of about μm from the start point of Fe+ ions track inside the molecular. A substantiation of reason of wall degradation in this area was proposed.
    },
     year = {2024}
    }
    

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  • TY  - JOUR
    T1  - Calculations of Stopping Power, Straggling and Range Projected of FeKr+
    
    AU  - Mohamed Farjallah
    Y1  - 2024/05/17
    PY  - 2024
    N1  - https://doi.org/10.11648/j.ep.20240701.11
    DO  - 10.11648/j.ep.20240701.11
    T2  - Engineering Physics
    JF  - Engineering Physics
    JO  - Engineering Physics
    SP  - 1
    EP  - 9
    PB  - Science Publishing Group
    SN  - 2640-1029
    UR  - https://doi.org/10.11648/j.ep.20240701.11
    AB  - The present work consists of the simulation of the interaction of a beam of Kr+ ions with a solid iron target by the software SRIM (Stopping and Range of Ions In Matter). Our goal is to calculate different parameters related to sputtering and ion implantation in a target, such as the spatial distribution of implanted ions, the distributions of electronic and nuclear energy losses as a function of penetration depth and sputtering efficiency, as well as the damage created inside the target. The sputter induced photon spectroscopy technique was used to study the luminescence spectra of the species sputtered from Iron powder, during 5 keV Kr+ ions bombardment in vacuum better than 107 torr. The optical spectra recorded between 350 and 470 nm exhibit discrete lines which are attributed to neutral excited atoms of Iron (Fe). The experiments are also performed under 105 torr ultra-pure oxygen partial pressure. To ensure the maximum efficiency of molecular modification process, energy of irradiation was decided by using of SRIM software. Based on SRIM simulation of Iron ions interaction with Krypton, the areas on which effect of high energy ions will maximum were predicted. A comparative analysis of molecular before and after irradiation was carried out by scanning electron microscopy. The maximum change in Krypton morphology, in the form of destruction of walls, was appeared at a distance of about μm from the start point of Fe+ ions track inside the molecular. A substantiation of reason of wall degradation in this area was proposed.
    
    VL  - 7
    IS  - 1
    ER  - 

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