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A combinatorial scheme to tailor saturated displacement damage in heavy-ion irradiated tungsten via post-irradiation annealing

  • Shiwei Wang*
  • , Hanqing Wang
  • , Xiaoou Yi*
  • , Yuhan Sun
  • , Shangkun Shen
  • , Wangguo Guo
  • , Qigui Yang
  • , Long Cheng
  • , Yue Yuan
  • , Xingzhong Cao
  • , Engang Fu*
  • , Guang Hong Lu
  • *此作品的通讯作者
  • Peking University
  • Beihang University
  • University of Science and Technology Beijing
  • CAS - Institute of High Energy Physics

科研成果: 期刊稿件文章同行评审

摘要

Tungsten has demonstrated a competitive figure of merit in its application to plasma-facing components (PFCs) of fusion reactors. During service, the material is exposed to high temperatures and high-level displacement damage. A common interest is fostered in the nuclear materials community to address the issue of defect evolution at operating temperatures, and how they recover throughout service. During maintenance, the application of in situ thermal repair technologies is tempting, featuring attractive efficiency in defect removal via an optimal selection of post-irradiation annealing (PIA) parameters. In previous studies, we examined the role of PIA temperature, PIA duration, and initial defect concentration on defect evolution, and redefined the damage recovery stages for tungsten, but this was done from a room-temperature heavy-ion irradiation perspective; see Wang et al (2023 J. Nucl. Mater. 581 154454), Wang et al (2024 Acta Mater. 273 119942). In this study, the scope is expanded to displacement damage saturation induced by heavy-ions at high temperatures, relevant to the service conditions of tungsten-based PFCs. The damage microstructure evolution in response to varied irradiation temperatures (T Irr) and PIA temperatures (T PIA) was assessed via transmission electron microscopy and Doppler broadening positron annihilation spectroscopy. Irradiation hardening was evaluated via nano-indentation. A scientific framework is proposed to guide thermal healing of displacement damage in tungsten via PIA treatment. It was ineffective when T PIA ⩽ T Irr. An adverse effect of PIA-induced secondary hardening occurred when T PIA (stage III) > T Irr (stage III). The optimal PIA scheme was confirmed when T PIA (stage IV) > T Irr (stages III–IV), eluding PIA-induced secondary hardening and minimizing PIA-enhanced recrystallization.

源语言英语
期刊论文编号056015
期刊Nuclear Fusion
66
5
DOI
出版状态已出版 - 1 5月 2026

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