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Structural and diffusion coefficient changes in amorphous Co-P Alloy
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Journal of Materials Science and Engineering B 2 (8) (2012) 482-486
Structural and Diffusion Coefficient Changes in
Amorphous Co-P Alloy
Pham Huu Kien 1, Le Thi Huong Dung1
and Nguyen Van Dang2
1. Department of Physics, Thai Nguyen University of Education, Luong Ngoc Quyen street, Thai Nguyen Viet Nam
2. Department of Physics and Technology, College of Science, Thai Nguyen University, Thai Nguyen Vietnam
Received: June 18, 2012 / Accepted: August 10, 2012 / Published: August 25, 2012.
Abstract: Structural and diffusion coefficient changes in amorphous Co-P solids are studied using the statistic relaxation model
containing 105
atoms. The pair radial distribution functions of simulation model are agreement with experimental data. A large number
of simplexes have been found varying the relaxation degree and concentration of phosphorus. It found a significant number of bubbles,
they could break up and leads to diffusion. This simulation result reveals that the decrease in diffusion coefficient upon thermal
annealing and concentration of phosphorus observed experimentally for the most amorphous Co-P alloy is interpreted as a result of
reduced number of bubbles in system.
Key words: Statistic relaxation, amorphous alloys, tracer diffusion, simplex, bubbles.
1. Introduction
Amorphous alloy (AMA) Co-P is a material of much
technological relevance and has important implications
in material science and geophysics [1-9]. There are
many works studied the structural of AMA Co-P. For
example, J. F. Sadoc et al. shows that the first peak
position of the pair radial distribution functions (PRDF)
are at 2.55, 2.32 and 3.34 Å responding with Co-Co,
Co-P and P-P pairs, respectively. They showed that the
tetrahedral close packing model confirmed by the
Voronoi polyhedral study [4]. Y. Waseda reveals that
the atom distance and coordination number in
amorphous Co82P18 are equal to 2.57 Å, 10.0 and 2.30
Å, 8.0 responding with Co-Co, Co-P pairs, respectively.
He proposed a concentration dependent of the first
peak position in G(r) for binary alloy glasses with P
and B [5]. However, these works had not revealed the
structural dependent on relaxation degree and
concentration of metalloid.
Corresponding author: Pham Huu Kien, Doctor, research
fields: computational physics, simulation of amorphous
materials. E-mail: [email protected].
Furthermore, it is found that many specific
properties of diffusion in AMA Co-P compared to
crystal counterpart. Study in Refs. [6, 7] shows that the
tracer-diffusivity in well-relaxed specimen is much
slower than one in as-quenched sample. This relaxation
effect commonly is interpreted by the reduction of
quasi-vacancies in super-saturation until the relaxation
is over. In well-relaxed state, conversely, the tracer
atoms diffuse via collective movement of a group of
neighboring atoms. However, the experimental data in
Refs. [8, 9] is in contradiction to that the diffusion
mechanism just described predicted. Computer
simulation, on other hand reveals unstableness of
vacancies in amorphous matrix [10]. Previous study
shows that the atomic cage like bubble functions as
diffusion vehicle for AMA. The bubble represents a
spherical void with five or more atoms lied on its
surface [11]. However, the analysis of this study based
only on AMA Fe80B20.
Therefore, the present paper focus study the
structural and diffusion coefficient changes in AMA
Co-P upon metalloid concentration and relaxation
degree based on all types of simplexes and bubbles in