TY - JOUR
T1 - Studies on the local structure of dilute 3d transition metal ternary dopants in L12 ordered Ni3Al-based alloys
AU - Balasubramanian, M.
AU - Lyver, R.
AU - Budnick, J. I.
AU - Pease, D. M.
PY - 1997
Y1 - 1997
N2 - We have utilized the technique of XAFS to study the local environment of transition metal (TM) ternary dopants (Ti, V, Cr, Mn, Fe and Co) in Ni75TMxAl25-x. In γ-Ni3Al, the first shell around Al consists of 12 Ni atoms. Ni is surrounded by 8 Ni and 4 Al atoms. In all cases, the dopant K-edge XAFS results show only Ni backscattering contribution in the first peak of the Fourier transform. Al backscattering contribution is either completely absent or is so weak that it is masked by the strong dopant-Ni bond. The number of Ni near neighbors suggests that for Ti, V, Cr, Mn and Fe absorbers, a majority of the dopant atoms occupy the Al sublatice. However, even in the case of Co dopants where studies by others indicate that the Co atoms occupy the Ni sublattice, no Al backscattering contribution can be detected. Also, the XANES of the various dopants exhibit a special feature at the edge, which appears to be due to p-d mixing.
AB - We have utilized the technique of XAFS to study the local environment of transition metal (TM) ternary dopants (Ti, V, Cr, Mn, Fe and Co) in Ni75TMxAl25-x. In γ-Ni3Al, the first shell around Al consists of 12 Ni atoms. Ni is surrounded by 8 Ni and 4 Al atoms. In all cases, the dopant K-edge XAFS results show only Ni backscattering contribution in the first peak of the Fourier transform. Al backscattering contribution is either completely absent or is so weak that it is masked by the strong dopant-Ni bond. The number of Ni near neighbors suggests that for Ti, V, Cr, Mn and Fe absorbers, a majority of the dopant atoms occupy the Al sublatice. However, even in the case of Co dopants where studies by others indicate that the Co atoms occupy the Ni sublattice, no Al backscattering contribution can be detected. Also, the XANES of the various dopants exhibit a special feature at the edge, which appears to be due to p-d mixing.
UR - https://www.scopus.com/pages/publications/33750649441
U2 - 10.1051/jp4:19972133
DO - 10.1051/jp4:19972133
M3 - Article
AN - SCOPUS:33750649441
SN - 1155-4339
VL - 7
SP - C2-1043-C2-1045
JO - Journal De Physique. IV : JP
JF - Journal De Physique. IV : JP
IS - 2 Part 2
ER -