Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects
Despite the low solubility of hydrogen isotopes (HIs) in tungsten (W), their concentration can reach up to ∼10 at.% after low-energy plasma irradiation. This is generally attributed to the vacancies that may accommodate excessive HIs. However, the kinetic energy of incident HIs transferred to W is f...
| Published in: | Nuclear Fusion |
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| Main Authors: | , , , , , , , |
| Format: | Article |
| Language: | English |
| Published: |
IOP Publishing
2024-01-01
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| Subjects: | |
| Online Access: | https://doi.org/10.1088/1741-4326/ad3091 |
| _version_ | 1850361470520393728 |
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| author | Hao-Xuan Huang Yu-Hao Li Jin-Liang Li Fang-Fei Ma Qing-Yuan Ren Li-Min Liu Hong-Bo Zhou Guang-Hong Lu |
| author_facet | Hao-Xuan Huang Yu-Hao Li Jin-Liang Li Fang-Fei Ma Qing-Yuan Ren Li-Min Liu Hong-Bo Zhou Guang-Hong Lu |
| author_sort | Hao-Xuan Huang |
| collection | DOAJ |
| container_title | Nuclear Fusion |
| description | Despite the low solubility of hydrogen isotopes (HIs) in tungsten (W), their concentration can reach up to ∼10 at.% after low-energy plasma irradiation. This is generally attributed to the vacancies that may accommodate excessive HIs. However, the kinetic energy of incident HIs transferred to W is far below the energy threshold to create a Frenkel pair, the underlying mechanism of defect production is still unclear. Here, we investigate the influence of H on the defect production in W using the molecular dynamic (MD) simulations. It is found that the threshold displacement energy (TDE) in bulk W slight decreases with the increasing of H concentration. This is due to the formation of H-vacancy complexes, which prevents the vacancy-interstitial recombination. More importantly, the H effects are significantly magnified in the surface region. On the one hand, the maximum kinetic energy transferred from 400 eV H to W can reach up to ∼21 eV due to the double-hit process, which is two times higher than that predicted by elastic collision model. On the other hand, the momentum transferred to W is completely random, including both the recoil direction upward and downward from the surface. Accordingly, the lowest TDE in W surface is only 15–21 eV at sub-surface layers with the depth of 6.7–11.1 Å, which is lower than the maximum kinetic energy transferred to W. Therefore, the low-energy HIs irradiation can create the defects in W surface directly. Our findings provide deep insight into defect production in W at sub-threshold energy and have wider implications for materials performance under low-energy ions irradiation. |
| format | Article |
| id | doaj-art-6cf734bbee64400a969e8022aedd5f2d |
| institution | Directory of Open Access Journals |
| issn | 0029-5515 |
| language | English |
| publishDate | 2024-01-01 |
| publisher | IOP Publishing |
| record_format | Article |
| spelling | doaj-art-6cf734bbee64400a969e8022aedd5f2d2025-08-19T23:04:57ZengIOP PublishingNuclear Fusion0029-55152024-01-0164505600410.1088/1741-4326/ad3091Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effectsHao-Xuan Huang0Yu-Hao Li1Jin-Liang Li2Fang-Fei Ma3Qing-Yuan Ren4Li-Min Liu5Hong-Bo Zhou6https://orcid.org/0000-0001-5585-6154Guang-Hong Lu7Department of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDepartment of Physics, Beihang University , Beijing 100191, China; Beijing Key Laboratory of Advanced Nuclear Materials and Physics, Beihang University , Beijing 100191, ChinaDespite the low solubility of hydrogen isotopes (HIs) in tungsten (W), their concentration can reach up to ∼10 at.% after low-energy plasma irradiation. This is generally attributed to the vacancies that may accommodate excessive HIs. However, the kinetic energy of incident HIs transferred to W is far below the energy threshold to create a Frenkel pair, the underlying mechanism of defect production is still unclear. Here, we investigate the influence of H on the defect production in W using the molecular dynamic (MD) simulations. It is found that the threshold displacement energy (TDE) in bulk W slight decreases with the increasing of H concentration. This is due to the formation of H-vacancy complexes, which prevents the vacancy-interstitial recombination. More importantly, the H effects are significantly magnified in the surface region. On the one hand, the maximum kinetic energy transferred from 400 eV H to W can reach up to ∼21 eV due to the double-hit process, which is two times higher than that predicted by elastic collision model. On the other hand, the momentum transferred to W is completely random, including both the recoil direction upward and downward from the surface. Accordingly, the lowest TDE in W surface is only 15–21 eV at sub-surface layers with the depth of 6.7–11.1 Å, which is lower than the maximum kinetic energy transferred to W. Therefore, the low-energy HIs irradiation can create the defects in W surface directly. Our findings provide deep insight into defect production in W at sub-threshold energy and have wider implications for materials performance under low-energy ions irradiation.https://doi.org/10.1088/1741-4326/ad3091defect productionsub-threshold energyhydrogen supersaturationtungstenmolecular dynamics |
| spellingShingle | Hao-Xuan Huang Yu-Hao Li Jin-Liang Li Fang-Fei Ma Qing-Yuan Ren Li-Min Liu Hong-Bo Zhou Guang-Hong Lu Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects defect production sub-threshold energy hydrogen supersaturation tungsten molecular dynamics |
| title | Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects |
| title_full | Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects |
| title_fullStr | Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects |
| title_full_unstemmed | Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects |
| title_short | Defect production in tungsten under sub-threshold energy irradiation: role of hydrogen and surface effects |
| title_sort | defect production in tungsten under sub threshold energy irradiation role of hydrogen and surface effects |
| topic | defect production sub-threshold energy hydrogen supersaturation tungsten molecular dynamics |
| url | https://doi.org/10.1088/1741-4326/ad3091 |
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