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Chinese Journal of Materials Research  2016, Vol. 30 Issue (9): 641-648    DOI: 10.11901/1005.3093.2015.529
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Irradiation Hardening and Defects Distribution in CLAM Steel under Deuterium and Helium Ion Irradiation
Zhenyu FU,Zequn WANG,Pingping LIU,Yinping WEI,Farong WAN,Qian ZHAN
School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China
Cite this article: 

Zhenyu FU,Zequn WANG,Pingping LIU,Yinping WEI,Farong WAN,Qian ZHAN. Irradiation Hardening and Defects Distribution in CLAM Steel under Deuterium and Helium Ion Irradiation. Chinese Journal of Materials Research, 2016, 30(9): 641-648.

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Abstract  

The irradiation behavior of a China low activation martensitic (CLAM) steel was investigated by advanced transmission electron microscopy combined with nano-indentation measurement. The CLAM steel was irradiated by single-(D+), single-(He+) and sequential-(D+ plus He+ subsequently) ions respectively at room temperature. The nano-indentation hardness results show that all of the irradiated specimens exhibited obvious hardening. The irradiation hardening rate was obtained for each specimens by fitting the experimental data using the modified NGK model, in which D+ implanted samples had the lowest radiation hardening level while the one for He+ injection and D+ + He+ implanted samples were significant. The microstructure analysis indicates that the defect density gradually increased first and then decreased along the implantation depth direction. High-density irradiation induced defects were present at the vicinity of the implantation peak depth. Homogeneously distributed fine bubbles were observed in both single-(He+) and sequential-(D+ plus He+ subsequently) irradiated samples with the bubble appearance at shallower depth for the latter ones because of the synergistic effect. No bubbles were found in single-(D+) irradiated samples. The hardening rate of He+ implanted samples, in which both dislocation loops and helium bubbles occurred, is greater than D+ implanted samples. In D++He+ irradiated samples, certain defects occurred by D+ will recover when the samples are being irradiated by He+. Therefore, the hardening rate of D++He+ irradiated samples is not equivalent to the rate of D+ irradiated samples plus He+ irradiated samples. Irradiation hardening results from the synergistic reaction.

Key words:  metallic materials      CLAM steel      irradiation effect      defects distribution      bubble     
Received:  07 September 2015     
Fund: *Supported by National Magnetic Con?nement Fusion Program Nos 2014GB104003 & 2014GB120001, National Natural Science Foundation of China No 51371031

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https://www.cjmr.org/EN/10.11901/1005.3093.2015.529     OR     https://www.cjmr.org/EN/Y2016/V30/I9/641

Ion irradiation Fluence / ionscm-2 Temperature / ℃ Energy / keV
D+ 1×1017 150
He+ 5×1016 room temperature 380
D++He+ 1×1017+5×1016 150/380
Table 1  Irradiation condition
Fig.1  DPA and ion concentration curves based on SRIM (a) D+ irradiation; (b) He+ irradiation
Fig.2  Cross section and top view of indenter
Fig.3  Nano hardness curves of irradiated and unirradiated CLAM
Ion irradiation HL HS A k t
He+ 7.06724 4.90348 538.6809 0.00258 14.41192
D+ 4.90441 4.19019 634.188 0.04355 38.9387
D++He+ 7.60068 4.80226 757.6145 0.00368 11.06666
Table 2  HL, Hs based on NGK model
Fig.4  NGK model fitting curves of irradiated CLAM steel (a) D+ irradiated; (b) He+ irradiated; (c) D++He+ irradiated
Fig.5  TEM image of microstructure in unirradiated CLAM steel (a); EDPs of M23C6 (b) and MC (c)
Fig.6  Cross-section TEM image of CLAM after D+ irradiation
Fig.7  Cross-section TEM image of microstructure in CLAM after He+ irradiation (a, b), and corresponding to different depth area (c-f)
Fig.8  Cross-section TEM images of CLAM after H++ He+ irradiation (a), and microstructures of different depth area (b-d)
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