TY - JOUR
T1 - Effect of laser beam thermal shock on the helium ion irradiation damage behavior of W-TiC-Y2O3 composites
AU - Xu, Meng–Yao Y.
AU - Luo, Lai–Ma M.
AU - Xu, Yue
AU - Zan, Xiang
AU - Xu, Qiu
AU - Tokunaga, Kazutoshi
AU - Zhu, Xiao–Yong Y.
AU - Wu, Yu–Cheng C.
N1 - Publisher Copyright:
© 2018 Elsevier B.V.
PY - 2018/10
Y1 - 2018/10
N2 - In this work, a W-TiC-Y2O3 composite was successfully prepared using a wet chemical method, and the thermal shock behavior of the composite was studied under a laser beam. The influence of the thermal shock of the laser-beamed W-TiC-Y2O3 composite on the radiation damage behavior of helium ions was also explored. The results show that after laser beam thermal shock, the W-TiC-Y2O3 composite exhibited ablation and remelting in the molten region. Three different morphologies were observed on the material surface after thermal shock: molten zone, heat-affected zone and unaffected zone. Second-phase agglomeration occurred in the heat-affected zone. After helium irradiation, nanotendrils are formed in the unaffected area and the heat-affected area. However, the degree of irradiation damage in the melting zone is much lighter. This is mainly due to the columnar structure in melting zone.
AB - In this work, a W-TiC-Y2O3 composite was successfully prepared using a wet chemical method, and the thermal shock behavior of the composite was studied under a laser beam. The influence of the thermal shock of the laser-beamed W-TiC-Y2O3 composite on the radiation damage behavior of helium ions was also explored. The results show that after laser beam thermal shock, the W-TiC-Y2O3 composite exhibited ablation and remelting in the molten region. Three different morphologies were observed on the material surface after thermal shock: molten zone, heat-affected zone and unaffected zone. Second-phase agglomeration occurred in the heat-affected zone. After helium irradiation, nanotendrils are formed in the unaffected area and the heat-affected area. However, the degree of irradiation damage in the melting zone is much lighter. This is mainly due to the columnar structure in melting zone.
UR - http://www.scopus.com/inward/record.url?scp=85049348843&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85049348843&partnerID=8YFLogxK
U2 - 10.1016/j.jnucmat.2018.06.043
DO - 10.1016/j.jnucmat.2018.06.043
M3 - Article
AN - SCOPUS:85049348843
SN - 0022-3115
VL - 509
SP - 198
EP - 203
JO - Journal of Nuclear Materials
JF - Journal of Nuclear Materials
ER -