This contribution presents some developments of the gnxas methodology and suite of programs, providing full analysis of raw experimental XAS data through advanced multiple-scattering simulations. The main features of the gnxas suite of programs, including the basic theoretical background based on an n-body expansion of the x-ray absorption cross section, as well as useful information about the gnxas flow diagram and practical usage are reviewed. The new gnxas graphical interface w-gnxas is specifically illustrated. The recent implementation of Reverse Monte Carlo algorithms allowing for multiatomic structural refinement into the rmc-gnxas package is also presented in detail with specific examples.

gnxas: Advances in the suite of programs for multiple-scattering analysis of X-ray absorption data

Trapananti A;
2018

Abstract

This contribution presents some developments of the gnxas methodology and suite of programs, providing full analysis of raw experimental XAS data through advanced multiple-scattering simulations. The main features of the gnxas suite of programs, including the basic theoretical background based on an n-body expansion of the x-ray absorption cross section, as well as useful information about the gnxas flow diagram and practical usage are reviewed. The new gnxas graphical interface w-gnxas is specifically illustrated. The recent implementation of Reverse Monte Carlo algorithms allowing for multiatomic structural refinement into the rmc-gnxas package is also presented in detail with specific examples.
2018
Istituto Officina dei Materiali - IOM -
Inglese
204
221
256
http://www.scopus.com/inward/record.url?eid=2-s2.0-85045290038&partnerID=q2rCbXpz
X ray absorption | Extended X ray absorption fine structure spectroscopy | x-ray absorption
5
info:eu-repo/semantics/article
262
Iesari, F; Hatada, K; Trapananti, A; Minicucci, M; Di Cicco, A
01 Contributo su Rivista::01.01 Articolo in rivista
none
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/345546
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