First-Principles Study of Hydrogen Impact on the Formation and Migration of Helium Interstitial Defects in hcp Titanium
LU Yong-Fang1, SHI Li-Qun1**, DING Wei2, LONG Xing-Gui2
1Institute of Modern Physics, Fudan University, Shanghai 200433 2Institute of Nuclear Physics and Chemistry, China Academy of Engineering Physics, Mianyang 621900
First-Principles Study of Hydrogen Impact on the Formation and Migration of Helium Interstitial Defects in hcp Titanium
LU Yong-Fang1, SHI Li-Qun1**, DING Wei2, LONG Xing-Gui2
1Institute of Modern Physics, Fudan University, Shanghai 200433 2Institute of Nuclear Physics and Chemistry, China Academy of Engineering Physics, Mianyang 621900
摘要We present a first-principles study of the effects of hydrogen on helium behavior in hcp titanium. The calculation indicates that the dissolved H atoms in hcp Ti change the formation energy of the interstitial He atom, but they do not change the energetically favorable occupying site of the He atom, i.e., the tetrahedral site is more favorable than the octahedral site. The impacts of H on the formation of interstitial He defects are directly related to the atomic environment around H atoms and their positions relative to interstitial He atoms as well. For He diffusion, a tetrahedral interstitial He atom can more easily migrate along the indirect tetrahedron-octahedron-tetrahedron path than the direct path of tetrahedron-tetrahedron. When a H atom exists in the first neighbor octahedral site from the He, the activation energy for He atom diffusion is 0.46 eV, which is higher than that of the He atom diffusion in perfect crystal, 0.41 eV. Increasing the number of H atoms to two, He diffusion needs much higher activation energy. This suggests that the H atoms around interstitial He may impede the migration of interstitial He atom in hcp Ti.
Abstract:We present a first-principles study of the effects of hydrogen on helium behavior in hcp titanium. The calculation indicates that the dissolved H atoms in hcp Ti change the formation energy of the interstitial He atom, but they do not change the energetically favorable occupying site of the He atom, i.e., the tetrahedral site is more favorable than the octahedral site. The impacts of H on the formation of interstitial He defects are directly related to the atomic environment around H atoms and their positions relative to interstitial He atoms as well. For He diffusion, a tetrahedral interstitial He atom can more easily migrate along the indirect tetrahedron-octahedron-tetrahedron path than the direct path of tetrahedron-tetrahedron. When a H atom exists in the first neighbor octahedral site from the He, the activation energy for He atom diffusion is 0.46 eV, which is higher than that of the He atom diffusion in perfect crystal, 0.41 eV. Increasing the number of H atoms to two, He diffusion needs much higher activation energy. This suggests that the H atoms around interstitial He may impede the migration of interstitial He atom in hcp Ti.
(Surface states, band structure, electron density of states)
引用本文:
LU Yong-Fang;SHI Li-Qun**;DING Wei;LONG Xing-Gui. First-Principles Study of Hydrogen Impact on the Formation and Migration of Helium Interstitial Defects in hcp Titanium[J]. 中国物理快报, 2012, 29(1): 13102-013102.
LU Yong-Fang, SHI Li-Qun**, DING Wei, LONG Xing-Gui. First-Principles Study of Hydrogen Impact on the Formation and Migration of Helium Interstitial Defects in hcp Titanium. Chin. Phys. Lett., 2012, 29(1): 13102-013102.
[1] Kneff D W and Farrar H 1979 J. Nucl. Mater. 85 479 [2] Sawan M E et al 2002 Fusion Eng. Des. 61 561 [3] Gilliam S B et al 2005 J. Nucl. Mater. 347 289 [4] Vogelsang W F and Khater H Y 1987 Fusion Eng. Des. 5 367 [5] Nagata S and Takahiro K 2001 J. Nucl. Mater. 290 135 [6] Besenbacher F et al 1982 J. Appl. Phys. 53 3547 [7] Lee S R et al 1989 J. Appl. Phys. 66 1137 [8] Beavis L C and Kass W J 1977 J. Vac. Scl. Technol. 14 509 [9] Kass W J 1977 J. Vac. Technol. 16 518 [10] Seletskaia T et al 2005 Phys. Rev. L 94 046403 [11] Seletskaia T et al 2008 Phys. Rev. B 78 134103 [12] Zeng X L et al 2009 Nucl. Instrum. Methods B 267 3037 [13] Yang L et al 2008 Physica B 403 2719 [14] Thomas G J 1983 Radiat. Eff. 78 37 [15] Wu Y X et al 2010 J. Anhui University of Technology 27 57 [16] Segall M D et al 2002 J. Phys. Condens. Matter 14 2717 [17] Robinson P and Das S 2004 J. Eng. Fract. Mech. 71 345 [18] Vanderbilt D 1990 Phys. Rev. B 41 7892 [19] Perdew J P et al 1992 Phys. Rev. B 46 6671 [20] Monkhorst H J and Pack J D 1976 Phys. Rev. B 13 5188 [21] Song Y et al 2002 Philos. Mag. A 82 1345 [22] Wang Y L et al 2010 J. Nucl. Mater. 402 55