Ab-initio grain boundary thermodynamics beyond the dilute limit

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Ab-initio grain boundary thermodynamics beyond the dilute limit. / Spitaler, Tobias; Scheiber, Daniel; Dösinger, Christoph Alexander et al.
in: Acta materialia, Jahrgang 286.2025, Nr. 1 March, 120725, 14.01.2025.

Publikationen: Beitrag in FachzeitschriftArtikelForschung(peer-reviewed)

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Spitaler T, Scheiber D, Dösinger CA, Hodapp M, Romaner L. Ab-initio grain boundary thermodynamics beyond the dilute limit. Acta materialia. 2025 Jan 14;286.2025(1 March):120725. doi: 10.1016/j.actamat.2025.120725

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@article{9a6fc3ba2d504a39889f3a9ee5522872,
title = "Ab-initio grain boundary thermodynamics beyond the dilute limit",
abstract = "Ab-initio calculations are frequently used to compute segregation energies and to investigate the segregation behavior of alloying elements in metals. But the segregation is considered mostly in the dilute limit, without considering interactions between solute atoms. Therefore, a formulation of the grain boundary Gibbs free energy within the compound energy formalism is proposed, which allows to analyze the segregation beyond the dilute limit and to establish a link between DFT segregation energies, the grain boundary energy and the expected excess. The segregation of Ti in bcc bulk is studied and we perform density functional theory calculations to obtain endmember energies. For a complete description of energetics, we train a moment tensor potential to parameterize the model. The segregation of Ti in bcc W bulk is studied and the symmetrical Σ3[110]({\=1}11) grain boundary is studied in detail. Our results show that the bulk and grain boundary thermodynamics need to be considered simultaneously when calculating the segregation beyond the dilute limit. The segregation of Ti changes from an anti-segregation to a segregation behavior with increasing Ti content. Although an increased Ti content reduces the grain boundary energy, the grain boundary is still higher in energy than the bulk and no thermodynamic stabilization of nanocrystalline W-Ti is expected. The results are compared to different models from literature.",
keywords = "DFT, Grain boundary energy, Grain boundary segregation, Non-dilute limit, W-Ti",
author = "Tobias Spitaler and Daniel Scheiber and D{\"o}singer, {Christoph Alexander} and Max Hodapp and Lorenz Romaner",
note = "Publisher Copyright: {\textcopyright} 2025 The Authors",
year = "2025",
month = jan,
day = "14",
doi = "10.1016/j.actamat.2025.120725",
language = "English",
volume = "286.2025",
journal = "Acta materialia",
issn = "1359-6454",
publisher = "Acta Materialia Inc",
number = "1 March",

}

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TY - JOUR

T1 - Ab-initio grain boundary thermodynamics beyond the dilute limit

AU - Spitaler, Tobias

AU - Scheiber, Daniel

AU - Dösinger, Christoph Alexander

AU - Hodapp, Max

AU - Romaner, Lorenz

N1 - Publisher Copyright: © 2025 The Authors

PY - 2025/1/14

Y1 - 2025/1/14

N2 - Ab-initio calculations are frequently used to compute segregation energies and to investigate the segregation behavior of alloying elements in metals. But the segregation is considered mostly in the dilute limit, without considering interactions between solute atoms. Therefore, a formulation of the grain boundary Gibbs free energy within the compound energy formalism is proposed, which allows to analyze the segregation beyond the dilute limit and to establish a link between DFT segregation energies, the grain boundary energy and the expected excess. The segregation of Ti in bcc bulk is studied and we perform density functional theory calculations to obtain endmember energies. For a complete description of energetics, we train a moment tensor potential to parameterize the model. The segregation of Ti in bcc W bulk is studied and the symmetrical Σ3[110](1̄11) grain boundary is studied in detail. Our results show that the bulk and grain boundary thermodynamics need to be considered simultaneously when calculating the segregation beyond the dilute limit. The segregation of Ti changes from an anti-segregation to a segregation behavior with increasing Ti content. Although an increased Ti content reduces the grain boundary energy, the grain boundary is still higher in energy than the bulk and no thermodynamic stabilization of nanocrystalline W-Ti is expected. The results are compared to different models from literature.

AB - Ab-initio calculations are frequently used to compute segregation energies and to investigate the segregation behavior of alloying elements in metals. But the segregation is considered mostly in the dilute limit, without considering interactions between solute atoms. Therefore, a formulation of the grain boundary Gibbs free energy within the compound energy formalism is proposed, which allows to analyze the segregation beyond the dilute limit and to establish a link between DFT segregation energies, the grain boundary energy and the expected excess. The segregation of Ti in bcc bulk is studied and we perform density functional theory calculations to obtain endmember energies. For a complete description of energetics, we train a moment tensor potential to parameterize the model. The segregation of Ti in bcc W bulk is studied and the symmetrical Σ3[110](1̄11) grain boundary is studied in detail. Our results show that the bulk and grain boundary thermodynamics need to be considered simultaneously when calculating the segregation beyond the dilute limit. The segregation of Ti changes from an anti-segregation to a segregation behavior with increasing Ti content. Although an increased Ti content reduces the grain boundary energy, the grain boundary is still higher in energy than the bulk and no thermodynamic stabilization of nanocrystalline W-Ti is expected. The results are compared to different models from literature.

KW - DFT

KW - Grain boundary energy

KW - Grain boundary segregation

KW - Non-dilute limit

KW - W-Ti

UR - http://www.scopus.com/inward/record.url?scp=85215385302&partnerID=8YFLogxK

U2 - 10.1016/j.actamat.2025.120725

DO - 10.1016/j.actamat.2025.120725

M3 - Article

VL - 286.2025

JO - Acta materialia

JF - Acta materialia

SN - 1359-6454

IS - 1 March

M1 - 120725

ER -