Near-edge x-ray absorption fine-structure study of ion-beam-induced phase transformation in Gd2(Ti1-yZry)2O7 -: art. no. 033518

被引:14
作者
Nachimuthu, P [1 ]
Thevuthasan, S
Shutthanandan, V
Adams, EM
Weber, WJ
Begg, BD
Shuh, DK
Lindle, DW
Gullikson, EM
Perera, RCC
机构
[1] Univ Nevada, Dept Chem, Las Vegas, NV 89154 USA
[2] Univ Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720 USA
[3] Pacific NW Natl Lab, Richland, WA 99352 USA
[4] Australian Nucl Sci & Technol Org, Menai, NSW 2234, Australia
关键词
D O I
10.1063/1.1840097
中图分类号
O59 [应用物理学];
学科分类号
摘要
The structural and electronic properties of Gd-2(Ti1-yZry)(2)O-7 (y=0-1) pyrochlores following a 2.0-MeV Au2+ ion-beam irradiation (similar to5.0x10(14) Au2+/cm(2)) have been investigated by Ti 2p and O 1s near-edge x-ray absorption fine structure (NEXAFS). The irradiation of Gd-2(Ti1-yZry)(2)O-7 leads to the phase transformation from the ordered pyrochlore structure (Fd3m) to the defect fluorite structure (Fm3m) regardless of Zr concentration. Irradiated Gd-2(Ti1-yZry)(2)O-7 with yless than or equal to0.5 are amorphous, although significant short-range order is present. Contrasting to this behavior, compositions with ygreater than or equal to0.75 retain crystallinity in the defect fluorite structure following irradiation. The local structures of Zr4+ in the irradiated Gd-2(Ti1-yZry)(2)O-7 with ygreater than or equal to0.75 determined by NEXAFS are the same as in the cubic fluorite-structured yttria-stabilized zirconia (Y-ZrO2), thereby providing conclusive evidence for the phase transformation. The TiO6 octahedra present in Gd-2(Ti1-yZry)(2)O-7 are completely modified by ion-beam irradiation to TiOx polyhedra, and the Ti coordination is increased to eight with longer Ti-O bond distances. The similarity between cation sites and the degree of disorder in Gd2Zr2O7 facilitate the rearrangement and relaxation of Gd, Zr, and O ions/defects. This inhibits amorphization during the ion-beam-induced phase transition to the radiation-resistant defect fluorite structure, which is in contrast to the ordered Gd2Ti2O7. (C) 2005 American Institute of Physics.
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