TY - JOUR
T1 - Helium effects on EUROFER97 martensitic steel irradiated by dual-beam from 1 to 50 dpa at 250 and 300 °C with 10 He appm/dpa
AU - Yu, Gang
AU - Li, Xiaoqiang
AU - Yu, Jinnan
AU - Wu, Yican
AU - Kinoshita, H.
AU - Takahashi, H.
AU - Victoria, M.
PY - 2004/8/1
Y1 - 2004/8/1
N2 - Reduced activation martensitic steel specimens were irradiated by dual-beam from 0.1 to 50 dpa at 250 and 300 °C with 10 He appm/dpa. The in-situ microstructure observation shows that the bubbles were present after 1.7 dpa for 250 °C irradiation and after 0.1 dpa for 300 °C irradiation. The bubble size distribution is a Maxwell distribution, which evolves to a bimodal distribution with increasing damage dose. The transition occurs after 10 dpa at 300 °C irradiation and after 30 dpa at 250 °C irradiation. The bubble concentration and peak bubble size are similar for various doses at 250 °C, and are 3.8×1021 m-3 and 2.5 nm, respectively. The size of cavities at the second peak of the bimodal distribution is around 6 nm. The cavity size distribution increases and spreads out with damage dose increase. The dislocation loops are typical interstitial dislocation loops that evolve from black-white spots to visible interstitial loops. The size range of interstitial loops is between 2.5 and 11 nm and the dislocation loop density increases monotonically with the damage dose.
AB - Reduced activation martensitic steel specimens were irradiated by dual-beam from 0.1 to 50 dpa at 250 and 300 °C with 10 He appm/dpa. The in-situ microstructure observation shows that the bubbles were present after 1.7 dpa for 250 °C irradiation and after 0.1 dpa for 300 °C irradiation. The bubble size distribution is a Maxwell distribution, which evolves to a bimodal distribution with increasing damage dose. The transition occurs after 10 dpa at 300 °C irradiation and after 30 dpa at 250 °C irradiation. The bubble concentration and peak bubble size are similar for various doses at 250 °C, and are 3.8×1021 m-3 and 2.5 nm, respectively. The size of cavities at the second peak of the bimodal distribution is around 6 nm. The cavity size distribution increases and spreads out with damage dose increase. The dislocation loops are typical interstitial dislocation loops that evolve from black-white spots to visible interstitial loops. The size range of interstitial loops is between 2.5 and 11 nm and the dislocation loop density increases monotonically with the damage dose.
UR - https://www.scopus.com/pages/publications/3342935832
U2 - 10.1016/j.jnucmat.2004.04.300
DO - 10.1016/j.jnucmat.2004.04.300
M3 - 会议文章
AN - SCOPUS:3342935832
SN - 0022-3115
VL - 329-333
SP - 1003
EP - 1007
JO - Journal of Nuclear Materials
JF - Journal of Nuclear Materials
IS - 1-3 PART B
T2 - Proceedings of the 11th Conference on Fusion Research
Y2 - 7 December 2003 through 12 December 2003
ER -