de Lima J C, Raoux D, Charriere Y, Maurer M
LURE Bâtiment 209D, Faculté des Sciences, Orsay 91405, France.
J Phys Condens Matter. 2008 Mar 19;20(11):115103. doi: 10.1088/0953-8984/20/11/115103. Epub 2008 Feb 20.
The amorphous atomic structure of a melt-spun NiZr(3) alloy was investigated using the anomalous wide angle x-ray scattering (AWAXS) and reverse Monte Carlo (RMC) simulation techniques. The AWAXS data were collected at four incident photon energies, including ones close to the Ni and Zr K-edges, and four total structure factors S(K) were derived. Differential structure factors DAS(K) around the Ni and Zr atoms were calculated through the difference between the scattered intensities on a per-atom scale obtained at incident photon energy pairs (8330, 9455 eV) and (15622, 17993 eV). The contribution of the partial S(Ni-Ni)(K) for the Ni-DAS(K) factor is six times bigger than the one for the S(K) factors. Then, the use of the Ni-DAS(K) factor with four S(K) factors as input data for the RMC simulations has permitted us to obtain more stable partial S(Ni-Ni)(K), S(Ni-Zr)(K) and S(Zr-Zr)(K) factors. The partial S(ij)(K) factors are very close to those reported earlier for the amorphous NiZr(2) alloy. The structural data (coordination numbers and interatomic distances) for the first neighbors for both amorphous NiZr(2) and NiZr(3) alloys are also very similar.
采用反常广角X射线散射(AWAXS)和反向蒙特卡罗(RMC)模拟技术研究了熔纺NiZr(3)合金的非晶原子结构。在四个入射光子能量下收集了AWAXS数据,包括接近Ni和Zr K边的能量,并推导出四个总结构因子S(K)。通过在入射光子能量对(8330, 9455 eV)和(15622, 17993 eV)下获得的每原子尺度散射强度之间的差异,计算了Ni和Zr原子周围的差分结构因子DAS(K)。Ni-DAS(K)因子中部分S(Ni-Ni)(K)的贡献比S(K)因子中的大六倍。然后,将Ni-DAS(K)因子与四个S(K)因子作为RMC模拟的输入数据,使我们能够获得更稳定的部分S(Ni-Ni)(K)、S(Ni-Zr)(K)和S(Zr-Zr)(K)因子。部分S(ij)(K)因子与先前报道的非晶NiZr(2)合金的非常接近。非晶NiZr(2)和NiZr(3)合金第一近邻的结构数据(配位数和原子间距离)也非常相似。