Plasma and Fusion Research
Volume 13, 3403061 (2018)
Regular Articles
- 1)
- Department of Helical Plasma Research, National Institute for Fusion Science, National Institutes of Natural Sciences, 322-6 Oroshi-cho, Toki 509-5292, Japan
- 2)
- Department of Fusion Science, The Graduate University for Advanced Studies, 322-6 Oroshi-cho, Toki 509-5292, Japan
- 3)
- Department of Electrical Engineering, Graduate School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan
Abstract
To represent the formation of fuzzy nanostructures produced on a tungsten surface by exposure to a helium plasma, we have developed a hybrid simulation method that combines the binary collision approximation, molecular dynamics, and kinetic Monte Carlo calculations (BCA-MD-KMC). Since the MD code has been parallelized using the domain decomposition method (DDM) for execution in a multi-CPU environment, we developed the BCA code from scratch to mesh it efficiently with the DDM. The BCA-MD-KMC hybrid simulation code achieved a helium irradiation time of 0.1 seconds or longer, in spite of functioning at the level of atomic-scale models. In consequence, we have been able to observe the formation of concave and convex structures on a tungsten surface in the simulation.
Keywords
fuzz, helium plasma, hybrid simulation, binary collision, molecular dynamics, kinetic Monte Carlo, plasma-wall interaction
Full Text
References
- [1] S. Takamura, N. Ohno, D. Nishijima and S. Kajita, Plasma Fusion Res. 1, 051 (2006).
- [2] S. Kajita, W. Sakaguchi, N. Ohno, N. Yoshida and T. Saeki, Nucl. Fusion 49, 095005 (2009).
- [3] M. Tokitani, S. Masuzaki, H. Kasahara, Y. Yoshimura, R. Sakamoto, N. Yoshida, Y. Ueda, T. Mutoh, LHD Experiment Group and S. Nagata, Nucl. Mater. Energy 12, 1358 (2017).
- [4] S. Kajita, S. Takamura and N. Ohno, Nucl. Fusion 49, 032002 (2009).
- [5] H. Iwakiri, K. Morishita and N. Yoshida, J. Nucl. Mater. 307-311, 135 (2002).
- [6] S. Kajita, S. Takamura, N. Ohno, D. Nishijima, H. Iwakiri and N. Yoshida, Nucl. Fusion 47, 1358 (2007).
- [7] S. Takamura and Y. Uesugi, Appl. Surf. Sci. 356, 888 (2015).
- [8] K. Omori, A.M. Ito, K. Shiga, N. Yamashita, K. Ibano, H.T. Lee and Y. Ueda, J. Appl. Phys. 121, 155301 (2017).
- [9] S. Kajita, T. Nojima, Y. Tomita, N. Ohno, H. Tanaka, N. Yoshida, M. Yajima, T. Akiyama, M. Tokitani and T. Yagi, Surf. Coat. Technol. 340, 86 (2018).
- [10] K.O.E. Henriksson, K. Nordlund and J. Keinonen, Nucl. Instrum. Methods Phys. Res. B 244, 377 (2006).
- [11] K.O.E. Henriksson, K. Nordlund, A. Krasheninnikov and J. Keinonen, Fusion Sci. Technol. 50, 18 (2006).
- [12] F. Sefta, K.D. Hammond, N. Juslin and B.D. Wirth, Nucl. Fusion 53, 073015 (2013).
- [13] A. Lasa, K.O.E. Henriksson and K. Nordlund, Nucl. Instrum. Methods Phys. Res. B 303, 156 (2013).
- [14] R.D. Smirnov and S.I. Krasheninnikov, Nucl. Fusion 53 082002 (2013).
- [15] A.M. Ito, Y. Yoshimoto, S. Saito, A. Takayama and H. Nakamura, Phys. Scr. T159, 014062 (2014).
- [16] L. Hu, K.D. Hammond, B.D.Wirth and D. Maroudas, Surf. Sci. 626, L21 (2014).
- [17] X.-C. Li, X. Shu, P. Tao, Y. Yu, G.-J. Niu, Y. Xu, F. Gao and G.-N. Luo, J. Nucl. Mater. 445, 544 (2014).
- [18] Y.L. Zhou, J. Wang, Q. Hou and A.H. Deng, J. Nucl. Mater. 446, 43 (2014).
- [19] F. Ferroni, K.D. Hammond and B.D. Wirth, J. Nucl. Mater. 458, 419 (2015).
- [20] R. Kobayashi, T. Hattori, T. Tamura and S. Ogata, J. Nucl. Mater. 463, 1071 (2015).
- [21] T.P.C. Klaver, S. Zhang and K. Nordlund, J. Nucl. Mater. 492, 113 (2017).
- [22] G. Wei, F. Ren, W. Qin, W. Hu, H. Deng and C. Jiang, Comput. Mater. Sci. 148, 242 (2018).
- [23] L. Pentecoste, A.-L. Thomann, P. Brault, T. Lecas, P. Desgardin, T. Sauvage and M.-F. Barthe, Acta Mater. 141, 47 (2017).
- [24] H. Nakamura, S. Saito, A.M. Ito and A. Takayama, Plasma Fusion Res. 11, 2401080 (2016).
- [25] J. Drobny, A. Hayes, D. Curreli and D.N. Ruzic, J. Nucl. Mater. 494, 278 (2017).
- [26] S.I. Krasheninnikov, Phys. Scr. T145, 014040 (2011).
- [27] D. Trufanov, E. Marenkov and S. Krasheninnikov, Physics Procedia 71, 20 (2015).
- [28] B.D. Wirth, K.D. Hammond, S.I. Krasheninnikov and D. Maroudas, J. Nucl. Mater. 463, 30 (2015).
- [29] A.M. Ito, A. Takayama, Y. Oda, T. Tamura, R. Kobayashi, T. Hattori, S. Ogata, N. Ohno, S. Kajita, M. Yajima, Y. Noiri, Y. Yoshimoto, S. Saito, S. Takamura, T. Murashima, M. Miyamoto and H. Nakamura, J. Nucl. Mater. 463, 109 (2015).
- [30] A.M. Ito, A. Takayama, Y. Oda, T. Tamura, R. Kobayashi, T. Hattori, S. Ogata, N. Ohno, S. Kajita, M. Yajima, Y. Noiri, Y. Yoshimoto, S. Saito, S. Takamura, T. Murashima, M. Miyamoto and H. Nakamura, Nucl. Fusion 55, 073013 (2015).
- [31] K.D. Hammond, S. Blondel, L. Hu, D. Maroudas and B.D. Wirth, Acta Mater. 144, 561 (2018).
- [32] S. Saito, H. Nakamura, M. Tokitani, R. Sakaue and K. Yoshida, Jpn. J. Appl. Phys. 55, 01AH07 (2015).
- [33] Y. Yamamura and Y. Mizuno, Inst. Plasma Phys. Nagoya University, IPPJ-AM-40 (1985).
- [34] Y. Yamaura and W. Takeuchi, Nucl. Instrum. Methods B29, 461 (1987).
- [35] W. Eckstein, Computer Simulation of Ion-Solid Interactions (Springer-Verlag, Berlin, Heidelberg, 1991).
- [36] J.F. Ziegler, J. Biersack and U. Littmark, The Stopping and Range of Ions in Matter (Pergamon Press, New York, 1985).
- [37] A.M. Ito, S. Kato and H. Nakamura, IAEA Fusion Energy Conference 2016, Oct. 17-22, 2016, Kyoto, MPT/P5-23, proceedings.
- [38] R.P. Doerner, M.J. Baldwin, M. Simmonds, J.H. Yu, L. Buzi and T. Schwarz-Selinger, Nucl. Mater. Energy 12, 372 (2017).
- [39] H.T. Lee, A.A. Haasz, J.W. Davis, R.G. Macaulay-Newcombe, D.G. Whyte and G.M. Wright, J. Nucl. Mater. 363-365, 898 (2007).
- [40] P.E. Lhuillier, T. Belhabib, P. Desgardin, B. Courtois, T. Sauvage, M.F. Barthe, A.L. Thomann, P. Brault and Y. Tessier, J. Nucl. Mater. 433, 305 (2013).
- [41] M.T. Robinson, J. Nucl. Mater. 103, 525 (1981).
- [42] V. Borovikov, A.F. Voter and X-Z. Tang, J. Nucl. Mater. 447, 254 (2014).