Structural evolution of NiAg heterogeneous alloys upon annealing

NiAg heterogeneous alloys were studied by x-ray diffraction and x-ray absorption spectroscopy at the Ni K-edge using a total electron yield detection. In the as-deposited alloys of 0.10 and 0.15 Ni atomic fraction, most of the Ni atoms are in substitutional sites in the Ag matrix. At higher Ni concentration, the Ni atoms outside the Ag-rich phase become numerous enough to group together in small clusters. An important disorder in the neighbourhood of Ni atoms is demonstrated. At low annealing temperature (up to C), in and , some Ni atoms are still present in substitutional sites in the Ag matrix and the small Ni particles are under strain. A very short-range order exists in this state. After a C annealing, the Ni particles grow, and the Ag-rich phase remains in a steady structural state. After a higher annealing (C), the local Ni atomic environment becomes well ordered and typical of the pure Ni FCC phase. The Ag-rich crystallites are impoverished in Ni atoms and grow with elimination of defects. Ni grains are generally smaller than 1 nm for as-deposited alloys and reach several nanometres after a C annealing for 10 min.

[1]  Arnold C. Vermeulen,et al.  Applicabilities of the Warren-Averbach Analysis and an Alternative Analysis for Separation of Size and Strain Broadening , 1994 .

[2]  E. Stern,et al.  Number of relevant independent points in x-ray-absorption fine-structure spectra. , 1993, Physical review. B, Condensed matter.

[3]  C. Michaelsen On the structure and homogeneity of solid solutions: The limits of conventional X-ray diffraction , 1995 .

[4]  Mittemeijer,et al.  Formation of crystalline AgxNi1-x solid solutions of unusually high supersaturation by laser ablation deposition. , 1994, Physical review letters.

[5]  Jiang,et al.  Giant magnetoresistance in nonmultilayer magnetic systems. , 1992, Physical review letters.

[6]  E. J. Mittemeijer,et al.  Laser ablation deposition of Cu‐Ni and Ag‐Ni films: Nonconservation of alloy composition and film microstructure , 1994 .

[7]  N. Binsted,et al.  A rapid, exact curved-wave theory for EXAFS calculations , 1984 .

[8]  B. Warren,et al.  X-Ray Diffraction , 2014 .

[9]  A. Fert,et al.  Giant magnetoresistance in magnetic nanostructures , 1995 .

[10]  B. Rodmacq,et al.  Structural Evolution of Ag–Co and Ag–Ni Alloys Studied by Anomalous Small-Angle X-ray Scattering , 1998 .

[11]  B. Diény,et al.  Nanostructure of Giant Magnetoresistance Heterogeneous Alloys Ni0.20Ag0.80 After Annealing , 1997 .

[12]  T. Girardeau,et al.  TEY device operating near liquid nitrogen temperature , 1994 .

[13]  T. C. Huang,et al.  Residual stress/strain analysis in thin films by X-ray diffraction , 1995 .

[14]  Alp,et al.  Structure of copper microclusters isolated in solid argon. , 1986, Physical Review Letters.

[15]  Forces between surfaces with weakly end-adsorbed polymers , 1997 .

[16]  J. F. Hamilton,et al.  Extended X-Ray-Absorption Fine Structure of Small Cu and Ni Clusters: Binding-Energy and Bond-Length Changes with Cluster Size , 1979 .

[17]  S. Maekawa,et al.  Giant magneto-transport phenomena in inhomogeneous materials , 1995 .

[18]  B. Diény,et al.  Low temperature total electron yield EXAFS study of CoxAg1−x granular alloys , 1996 .

[19]  Santucci,et al.  Extended x-ray-absorption fine-structure and near-edge-structure studies on evaporated small clusters of Au. , 1985, Physical review. B, Condensed matter.

[20]  B. Diény,et al.  Spin-disorder and spin-valve magnetoresistance in granular alloys , 1995 .

[21]  R. Averback,et al.  Formation of supersaturated solid solutions in the immiscible Ni–Ag system by mechanical alloying , 1996 .

[22]  Jaouen,et al.  Sampling depth in conversion-electron detection used for x-ray absorption. , 1992, Physical review. B, Condensed matter.

[23]  Grzegorz Głladyszewski Studying the interface of Au-Cu superlattices , 1989 .

[24]  Young,et al.  Giant magnetoresistance in heterogeneous Cu-Co alloys. , 1992, Physical review letters.