2019
DOI: 10.1103/physrevb.100.054204
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Partial structure investigation of the traditional bulk metallic glass Pd40Ni40P20

Abstract: Local structures of Pd40Ni40P20 bulk metallic glass (BMG) were investigated by combining anomalous x-ray scattering close to the Pd and Ni K absorption edges, x-ray diffraction, neutron diffraction, and reverse Monte Carlo modeling, from which partial structure factors Sij(Q) and partial pair distribution functions gij (r) as well as three-dimensional atomic configurations were carefully obtained around the constituent elements. A disagreement is found in the local structures with an ab initio molecular dynami… Show more

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Cited by 35 publications
(43 citation statements)
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“…With regard to this, the large‐box RMC simulation could be the only method of choice to feedback an amorphous structural model from the PDF data. The first RMC modeling of amorphous SiO 2 was performed in 1990, [ 138 ] and since then the algorithm has been optimized significantly, capable of combining MD and DFT, and triggered the RMC studies in a variety of amorphous systems such as metallic glasses, [ 139 ] hydrated complexes, [ 69 ] SiO x , [ 79 ] amorphous MOFs, [ 140 ] porous carbon, [ 141 ] and so on. Despite the above success, nonetheless, this method is frequently questioned as to whether the PDF data itself can carry such a huge information about every random atomic position in an amorphous system, and whether the retrieved chemical or topological results are model‐independent.…”
Section: Principles and Methodsmentioning
confidence: 99%
“…With regard to this, the large‐box RMC simulation could be the only method of choice to feedback an amorphous structural model from the PDF data. The first RMC modeling of amorphous SiO 2 was performed in 1990, [ 138 ] and since then the algorithm has been optimized significantly, capable of combining MD and DFT, and triggered the RMC studies in a variety of amorphous systems such as metallic glasses, [ 139 ] hydrated complexes, [ 69 ] SiO x , [ 79 ] amorphous MOFs, [ 140 ] porous carbon, [ 141 ] and so on. Despite the above success, nonetheless, this method is frequently questioned as to whether the PDF data itself can carry such a huge information about every random atomic position in an amorphous system, and whether the retrieved chemical or topological results are model‐independent.…”
Section: Principles and Methodsmentioning
confidence: 99%
“…Thus, the differential signal ∆V(k, R= 2.8 nm) affords a discrimination into two different MRO types dominant at different k-values, i.e. k = 5.3 nm −1 -"icosahedral-like" and k = 4.5 nm −1 -"crystal-like" for NiP [56][57][58] and PdNiP [59][60][61] . With respect to the "crystal-like" regime, it should be noted that the presence of nano-crystals is excluded since all NBDPs exhibit only speckle patterns 29,62 for all six sample states, i.e.…”
Section: Fluctuation Electron Microscopymentioning
confidence: 99%
“…Generally, the application of persistent homology to amorphous MRO structures is challenging, as the definition of characteristic regions (i.e., groups of loops) adopted in the original studies (20)(21)(22)(23)31) is not unique; that is, they use an "optimal cycle" for the geometric characterizations. Here, we introduce a self-consistent and rigorous definition of characteristic regions by separating them according to the number of contained atoms (see below for definitions).…”
Section: Introductionmentioning
confidence: 99%