Compact representation of the local atomic structure of matter for machine learning in XANES spectroscopy data processing

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Resumo

A method for representing data on the local structure of atoms in the form of histograms of paired radial distribution functions is proposed. This method is used to construct a structure descriptor needed to determine the structure of materials using machine learning and artificial intelligence techniques. A special feature of the method is the use of two sets of paired radial distribution functions simultaneously: for pairs of all types of atoms and for pairs with a selected absorbing atom. The developed approach was tested on the problem of determining the local atomic structure of the environment of the silver color center in sodium silicate glasses using data from X-ray absorption near-edge structure for the Ag K-edge. The information content of the proposed structure descriptor is demonstrated by the ability to reconstruct the three-dimensional structure of a silver color center model from the corresponding pairwise distance histograms. Using several machine learning methods, it was shown that the proposed descriptor allows to achieve high-quality reproduction (mean square error ~10–3) of X-ray absorption near-edge structure spectra for silver color centers in glass, which makes it possible to reduce the time for calculating X-ray absorption near-edge structure spectra by 4 orders of magnitude. The resulting machine learning model allows us to establish a fundamental connection between the atomic structure of silver color centers in glasses and the Ag X-ray absorption near-edge structure spectrum, which is necessary for determining the structure of glasses.

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Sobre autores

I. Viklenko

Southern Federal University

Autor responsável pela correspondência
Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

V. Srabionyan

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

V. Durymanov

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

Ya. Gladchenko-Dzhevelekis

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

V. Razdorov

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

L. Avakyan

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

L. Bugaev

Southern Federal University

Email: viklenko@sfedu.ru
Rússia, 344090, Rostov-on-Don

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2. Fig. 1. Illustration of pairs of atoms of types A and B taken into account when constructing the FRPA, in the absence (a) and presence (b, c) of the selected X-ray photon-absorbing atom A*.

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3. Fig. 2. Representation of information about the local atomic environment of a color center using histograms of the radial distribution relative to the absorbing atom (upper row) and histograms of all possible pairwise distances. The inset shows the corresponding structure of the color center.

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4. Fig. 3. Schematic representation of the optimization procedure for the structure of the A–A subsystem. The dotted line shows the correct arrangement of atoms of type A, and the solid black color shows the initial parameters of the system.

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5. Fig. 4. Schematic representation of the procedure for optimizing the relative position of subsystems A and B. The dotted line shows the position of subsystem A, the dashed line shows the position of subsystem B, and the dashed line shows the expected position of subsystem B relative to subsystem A.

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6. Fig. 5. Comparison of histograms of pairwise distances (top row) and histograms of radial distribution relative to the absorbing atom in the color center: original (dashed) and reconstructed (solid lines); the inset shows the three-dimensional reconstructed structure of the color center.

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7. Fig. 6. The value of the root-mean-square error of prediction of XANES spectra of the used machine learning models on the training (dark gray) and testing (light gray) data subsets.

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8. Fig. 7. Comparison of the X-ray absorption spectra near the K-edge of Ag obtained using the gradient boosting model (solid line) and the spectra calculated in the FDMNES program (dashed line) for the training (top) and validation (bottom) data subsets.

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9. Fig. 8. Comparison of the X-ray absorption spectra near the K-edge of Ag obtained using the gradient boosting model (solid line) and the spectrum calculated in the FMNESS program (dashed line) of a color center in a sodium silicate glass matrix with the structure obtained in [22] (shown in the inset).

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