scholarly journals Null-collision meshless Monte-Carlo - A new reverse Monte-Carlo algorithm designed for laser-source emission in absorbing/scattering inhomogeneous media

Author(s):  
M. Sans ◽  
M. El Hafi ◽  
V. Eymet ◽  
V. Forest ◽  
R. Fournier ◽  
...  
2005 ◽  
Vol 17 (17) ◽  
pp. 2605-2616 ◽  
Author(s):  
G Opletal ◽  
T C Petersen ◽  
D G McCulloch ◽  
I K Snook ◽  
I Yarovsky

Carbon ◽  
2003 ◽  
Vol 41 (12) ◽  
pp. 2403-2411 ◽  
Author(s):  
Tim Petersen ◽  
Irene Yarovsky ◽  
Ian Snook ◽  
Dougal G McCulloch ◽  
George Opletal

1997 ◽  
Vol 11 (24) ◽  
pp. 1047-1055 ◽  
Author(s):  
M. Andrecut

A simple Reverse Monte Carlo algorithm for structure simulations of multi-component amorphous solids is presented. The described algorithm is based on the standard reverse Monte Carlo method,1,2 developed for the monoatomic case, the application for poliatomic case being assured by using the Warren–Krutter–Morningstar approximation.3 An application for metal-metalloid glasses is also presented.


1996 ◽  
Vol 29 (3) ◽  
pp. 285-290 ◽  
Author(s):  
W. Montfrooij ◽  
R. L. McGreevy ◽  
R. Hadfield ◽  
N. H. Andersen

A Monte Carlo algorithm for the analysis of powder diffraction patterns is presented. One aim of this algorithm, which can be used as a supplement to the regular Rietveld refinement, is to provide a self-consistent determination of the thermal displacements of the atoms. This is achieved by modelling the total scattered intensity, comprising both the Bragg peak intensity and the diffuse contribution to the spectrum from the scattering density of an assembly of atoms. This assembly, which is constructed by the reverse Monte Carlo technique so as to yield a best fit with the data, is then used to calculate the average atomic thermal displacements. This allows for a refinement that, in principle, no longer requires angle-dependent background parameters, and that is well suited for dealing with highly anisotropic Debye–Waller factors and split atomic sites.


2001 ◽  
Vol 114 (2) ◽  
pp. 907 ◽  
Author(s):  
Fernando Luı́s B. da Silva ◽  
Wilmer Olivares-Rivas ◽  
Léo Degrève ◽  
Torbjörn Åkesson

2014 ◽  
Vol 70 (a1) ◽  
pp. C1445-C1445 ◽  
Author(s):  
Matteo Sestu ◽  
Anna Corrias ◽  
Maria Casula ◽  
Gabriele Navarra

Debye scattering equation is known since 1915 [1]. Altought this formula can, in principle, describe scattering from any multiple particle systems, its application is normally limited to small domains as clusters or low-sized nanoparticles. This is mostly due to the very high computational effort needed. Indeed, computing time strongly depends on the number of atoms. In recent years, the availability of highly performant graphics processing units (GPU) allowed their use for general purposes including strongly demanding scientific applications. This feature was exploited in the Debye Function Analysis to study more complex systems with several thousand of atoms [2]. Here, we present a refinement code using both the Debye scattering equation implemented on a commercial GPU and the Reverse Monte Carlo algorithm [3] to study the structure of two disordered nano-sized iron oxy-hydroxides, feroxyhite and ferrihydrite. The determination of their structure appears rather complex. Different interpretations of the X-ray diffraction pattern have been put forward and debates remain about the exact nature of their crystalline structure. The proposed models show some structural features that are not in accordance with the known structures of other iron oxy-hydroxides: goethite, akaganeite and lepidocrocite. To evaluate their validity, these models are used as starting atom sets in the refinement procedure. To reach a quantitative agreement between the experimental diffraction pattern and the calculated one, the atom positions are randomly modified. X-ray diffraction pattern is calculed using Debye scattering equation; to speed up calculation time, a parallelized version of the equation is optimized to run on Nvidia GeForce 690 GPU.


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