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arxiv: 2604.08875 · v1 · submitted 2026-04-10 · ❄️ cond-mat.mtrl-sci

A transferable framework for structure-energy mapping of nanovoid-solute complexes: Tungsten alloys as a model system

Pith reviewed 2026-05-10 18:02 UTC · model grok-4.3

classification ❄️ cond-mat.mtrl-sci
keywords nanovoidsolute segregationtungstencoordination motifsmachine learningdefect energeticsconfigurational search
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The pith

Local coordination motifs determine the energies of any nanovoid-solute complex in metals.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper establishes that solute atoms around nanovoids in tungsten interact through two channels: direct nanovoid-solute binding and nanovoid-mediated solute-solute effects. Both channels reduce to local atomic arrangements called coordination motifs, so that two complexes sharing the same motifs have nearly the same total energy. First-principles calculations on a finite set of motifs train machine-learning models that then assign energies to every motif in an arbitrary large complex. This reconstruction replaces exhaustive enumeration of the huge configuration space and yields stable structures for small, medium, and large voids. The resulting database shows Re segregation increases in discrete steps with coverage and supplies simple rules for rapid energy estimates.

Core claim

Solute segregation at nanovoid surfaces decomposes into direct nanovoid-solute interactions and nanovoid-mediated solute-solute interactions, both governed by local coordination motifs with identical motifs producing nearly identical energetics. Machine-learning models trained on first-principles data map these motifs to energies, so the total energy of any nanovoid-solute complex is reconstructed from its constituent motifs. A size-dependent search framework using enumeration, annealing, and greedy addition identifies stable configurations, reveals staircase-like Re segregation, and derives a surface-coverage criterion for fast prediction.

What carries the argument

Local coordination motifs, the distinct atomic neighborhoods around solute and vacancy sites whose energies are mapped by machine-learning models to reconstruct full complex energetics.

If this is right

  • Any nanovoid-solute complex energy can be obtained from a small library of motif calculations instead of full simulations.
  • Re atoms segregate to nanovoid surfaces in discrete coverage steps that control total energy.
  • The motif framework directly connects solute segregation to the vacancy-driven growth or shrinkage of nanovoids.
  • The same motif decomposition and search strategy applies to Os and Ta solutes in tungsten.
  • The predicted segregation patterns match a range of experimental observations on tungsten alloys.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The motif library could serve as input data for larger-scale models of radiation damage or alloy embrittlement.
  • If the local-motif rule holds across metals, the same approach would map solute behavior at other defects such as dislocations or grain boundaries.
  • Direct tests on a new solute or host metal would quickly show whether the motif set remains transferable.

Load-bearing premise

Interaction energies depend only on the local atomic neighborhood around each solute or vacancy site, with negligible contributions from distant atoms or the global arrangement.

What would settle it

Compute the total energy of one large nanovoid-Re complex directly from first principles and compare it to the energy obtained by summing the motif energies predicted by the trained models; a discrepancy larger than the training error falsifies the claim.

Figures

Figures reproduced from arXiv: 2604.08875 by Chang-Song Liu, Jie Hou, Kang-Ni He, Xiang-Shan Kong, Zhuo-Ming Xie.

Figure 1
Figure 1. Figure 1: Structure–energy modeling of nanovoid–solute complexes. (a) Schematic of a nanovoid–solute complex in a metallic matrix. The gray truncated octahedra denote vacancies, whereas the blue and orange spheres represent matrix and solute atoms, respectively. (b) Schematic of the interaction between a nanovoid and a single solute atom. (c) Feature-importance analysis of different nearest-neighbor vacancy coordina… view at source ↗
Figure 3
Figure 3. Figure 3: Comparison of optimization algorithms for identifying stable nanovoid–solute complexes. (a) Flowchart of the simulated annealing (SA) algorithm. (b) Flowchart of the greedy addition (GA) algorithm. (c) Comparison of the computational costs of exhaustive enumeration (EE), SA, and GA. For a vacancy cluster 𝑉n with q potential solute sites, the number of possible configurations containing 𝑚m solute atoms is c… view at source ↗
Figure 4
Figure 4. Figure 4: Re incremental binding energies in nanovoid–Re complexes as a function of Re number. (a–i) Comparison between model-predicted and DFT-calculated values for 𝑉1 − 𝑉6, 𝑉8, 𝑉10, and 𝑉15. (j–l) Comparison between the model-predicted values and those predicted by the 𝜃𝑅𝑒-based criterion for larger nanovoids, 𝑉50, 𝑉150, and 𝑉300. Figures 4 and 5 illustrate the incremental binding energies of Re atoms and represen… view at source ↗
Figure 5
Figure 5. Figure 5: Representative configurations of the highly symmetric nanovoid–Re complexes 𝑉6, 𝑉8, and 𝑉15 at different Re contents. The gray truncated octahedron denotes the Wigner–Seitz polyhedron of a vacancy. Atoms in different colors correspond to surface sites with different numbers of first- and second-nearest-neighbor vacancies, as indicated in the legend on the left. For each two-digit label, the first and secon… view at source ↗
Figure 6
Figure 6. Figure 6: Re incremental binding energies of all 𝑉1−300𝑅𝑒m complexes as a function of Re number, predicted by the GA-based model. At low Re coverage, Re atoms preferentially occupy energetically favorable surface sites characterized by large 𝐸𝑏 (𝑉𝑛,𝑅𝑒1 ) values. Simultaneously, repulsive Re– Re interactions favor spatially separated configurations, suppressing mutual solute interactions. Importantly, 𝐸𝑏 (𝑉𝑛, 𝑅𝑒1 ) i… view at source ↗
Figure 7
Figure 7. Figure 7: Construction and validation of the 𝜃𝑅𝑒 -based criterion for predicting Re incremental binding energies, where 𝜃𝑅𝑒 = 𝑚/𝑚𝑚𝑎𝑥 is the Re surface-coverage parameter. (a) Maximum Re capacity, 𝑚𝑚𝑎𝑥 , as a function of nanovoid vacancy number n, together with the fitted relation. (b) Dependence of the prediction accuracy on the number of uniformly divided 𝜃𝑅𝑒 intervals, measured by the root-mean-square error (RMSE)… view at source ↗
read the original abstract

Understanding the structures and energetics of nanovoid-solute complexes is essential for elucidating the coupled evolution of defects in metals. Yet their vast and complex configurational space poses a major challenge to conventional approaches. Using W-Re as a representative system, we demonstrate that solute segregation at nanovoid surfaces can be decomposed into direct nanovoid-solute interactions and nanovoid-mediated solute-solute interactions. Both are governed by local coordination motifs, with identical motifs giving nearly identical energetics. Based on first-principles data, we trained machine-learning models to map diverse local motifs to their energetics, enabling the energetics of any nanovoid-solute complex to be reconstructed from a finite set of constituent local motifs. We further developed a size-dependent configurational-search framework to efficiently identify thermodynamically stable structures, using exhaustive enumeration, simulated annealing, and greedy addition for small, medium-sized, and large complexes, respectively. This framework enabled the construction of a large database, revealed the staircase-like segregation behavior of Re, and derived a simple criterion based on Re surface coverage for rapid energy prediction across a wide size range. It also links Re segregation to vacancy-mediated nanovoid evolution and provides benchmarks for existing models and empirical potentials. Extensions to Os and Ta support the generality of the local-motif concept, and the predicted segregation behavior of solutes at nanovoids agrees with a range of experimental observations. This work establishes a physically transparent, accurate, and transferable framework for studying nanovoid-solute co-evolution in metals and provides reliable energetic inputs for multiscale simulations.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript claims that solute segregation at nanovoid surfaces in W-Re (and extensions to Os and Ta) decomposes into direct nanovoid-solute and nanovoid-mediated solute-solute interactions, both governed by local coordination motifs where identical motifs yield nearly identical energetics. First-principles data train ML models to map motifs to energies, enabling reconstruction of arbitrary complex energies from constituent motifs. A size-dependent configurational search (exhaustive enumeration, simulated annealing, greedy addition) builds a large database, reveals staircase-like Re segregation, derives a simple Re surface-coverage criterion for rapid prediction, links segregation to vacancy-mediated nanovoid evolution, and matches experimental observations.

Significance. If the local-motif additivity holds with quantified accuracy across size regimes, the work supplies a transparent, transferable framework for nanovoid-solute energetics that bypasses exhaustive enumeration of vast configuration spaces. It supplies first-principles-trained ML mappings, a size-dependent search protocol that enables database construction, and a simple predictive criterion, all of which could serve as benchmarks for empirical potentials and inputs for multiscale modeling of defect evolution in metals.

major comments (2)
  1. [Abstract / framework description] Abstract and framework description: the central reconstruction claim rests on the assertion that 'identical motifs giving nearly identical energetics' allows any complex to be built from a finite motif set, yet no explicit error bound, additivity test, or comparison isolating global geometry (while fixing motifs) is reported for complexes larger than the training motifs; long-range strain or charge effects could accumulate and undermine the mapping for the large-complex regime where the greedy search is applied.
  2. [Results (database and criterion derivation)] Results on the simple criterion: the Re surface-coverage criterion for rapid energy prediction is derived from the generated database without reported cross-validation against the full ML-reconstructed energies or an independent physical derivation; this risks post-hoc fitting and weakens the claim of a general, transferable rule across size ranges.
minor comments (1)
  1. [Abstract / extensions section] The abstract states extensions to Os and Ta support generality, but the main text should include quantitative motif-energy comparisons or error statistics for these solutes to substantiate transferability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the constructive and detailed comments, which help clarify and strengthen the presentation of our framework. We address each major comment point by point below, indicating revisions where the manuscript will be updated to incorporate additional validation and analysis.

read point-by-point responses
  1. Referee: [Abstract / framework description] Abstract and framework description: the central reconstruction claim rests on the assertion that 'identical motifs giving nearly identical energetics' allows any complex to be built from a finite motif set, yet no explicit error bound, additivity test, or comparison isolating global geometry (while fixing motifs) is reported for complexes larger than the training motifs; long-range strain or charge effects could accumulate and undermine the mapping for the large-complex regime where the greedy search is applied.

    Authors: We agree that an explicit additivity test and error bound for the largest complexes would strengthen the central claim. The manuscript demonstrates motif additivity and reconstruction accuracy on the training motifs and held-out small-to-medium complexes, with the ML models trained on diverse local environments drawn from multiple complex sizes. However, we did not isolate global geometry effects or report quantified reconstruction errors specifically for the large-complex regime used in the greedy search. In the revised manuscript we will add a dedicated validation subsection (with supplementary figures) that performs additivity tests on selected large complexes, provides explicit error bounds between motif-reconstructed and direct ML energies, and discusses the magnitude of any residual long-range contributions where additional DFT data can be obtained. revision: yes

  2. Referee: [Results (database and criterion derivation)] Results on the simple criterion: the Re surface-coverage criterion for rapid energy prediction is derived from the generated database without reported cross-validation against the full ML-reconstructed energies or an independent physical derivation; this risks post-hoc fitting and weakens the claim of a general, transferable rule across size ranges.

    Authors: The referee correctly notes that the surface-coverage criterion was extracted from the full database without an explicit cross-validation step against the ML-reconstructed energies. While the criterion is physically grounded in the staircase segregation pattern and the underlying motif energetics, we acknowledge that a formal validation procedure would better demonstrate its robustness and transferability. In revision we will add a cross-validation analysis: the database will be partitioned, the coverage threshold derived on a training subset, and its predictive accuracy quantified against the full ML-reconstructed energies on a held-out test set spanning multiple size regimes. We will also expand the physical derivation section to link the criterion more explicitly to the motif decomposition. revision: yes

Circularity Check

1 steps flagged

Simple Re surface-coverage criterion reduces to a post-hoc fit on the motif database

specific steps
  1. fitted input called prediction [Abstract (and corresponding results on database construction)]
    "This framework enabled the construction of a large database, revealed the staircase-like segregation behavior of Re, and derived a simple criterion based on Re surface coverage for rapid energy prediction across a wide size range."

    The criterion is obtained by post-processing the very database whose energies were computed via the ML-mapped local motifs and the size-dependent search. Consequently, 'rapid energy prediction' using the criterion is statistically equivalent to re-applying a fit extracted from the same data set rather than an independent derivation.

full rationale

The central decomposition into local-motif energetics begins from independent first-principles calculations, trains ML models on those data, and reconstructs complexes by additivity; this chain is self-contained and non-circular. The only load-bearing reduction occurs when the paper extracts a 'simple criterion based on Re surface coverage for rapid energy prediction' directly from the database it has just generated with the same framework. That step converts a fitted summary statistic into a claimed predictive tool, producing moderate circularity (score 4) without undermining the motif-mapping premise itself.

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

Relies on standard DFT accuracy for reference data and introduces the local-motif sufficiency assumption as the core new element; ML hyperparameters and the surface-coverage criterion constitute fitted elements.

free parameters (2)
  • ML model hyperparameters
    Parameters chosen during training of motif-to-energy models on first-principles data.
  • Re surface coverage threshold
    Used in the simple criterion for rapid energy prediction across sizes.
axioms (2)
  • domain assumption Density functional theory calculations yield sufficiently accurate reference energies for local motifs.
    Basis for training the machine-learning models.
  • ad hoc to paper Local coordination motifs determine interaction energetics independently of larger-scale structure.
    Central premise enabling decomposition and reconstruction.

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Works this paper leans on

67 extracted references · 67 canonical work pages

  1. [1]

    Nagai, K

    Y . Nagai, K. Takadate, Z. Tang, H. Ohkubo, H. Sunaga, H. Takizawa, M. Hasegawa, Positron annihilation study of vacancy -solute complex evolution in Fe -based alloys, Phys. Rev. B 67 (2003) 224202

  2. [2]

    Druzhkov, D.A

    A.P. Druzhkov, D.A. Perminov, A.E. Davletshin, The effect of alloying elements on the vacancy defect evolution in electron -irradiated austenitic Fe–Ni alloys studied by positron annihilation, J. Nucl. Mater. 384 (2009) 56-60

  3. [3]

    Konstantinović, A

    M.J. Konstantinović, A. Ulbricht, T. Brodziansky, N. Castin, L. Malerba, Vacancy -solute clustering in Fe–Cr alloys after neutron irradiation, J. Nucl. Mater. 540 (2020) 152341

  4. [4]

    Klimenkov, U

    M. Klimenkov, U. Jäntsch, M. Rieth, H.C. Schneider, D.E.J. Armstrong, J. Gibson, S.G. Roberts, Effect of neutron irradiation on the microstructure of tungsten, Nucl. Mater. Energy 9 (2016) 480-483

  5. [5]

    X. Hu, C.M. Parish, K. Wang, T. Koyanagi, B.P. Eftink, Y . Katoh, Transmutation -induced precipitation in tungsten irradiated with a mixed energy neutron spectrum, Acta Mater. 165 (2019) 51 - 61

  6. [6]

    Lloyd, R.G

    M.J. Lloyd, R.G. Abernethy, M.R. Gilbert, I. Griffiths, P.A.J. Bagot, D. Nguyen-Manh, M.P. Moody, D.E.J. Armstrong, Decoration of voids with rhenium and osmium transmutation products in neutron irradiated single crystal tungsten, Scr. Mater. 173 (2019) 96-100

  7. [7]

    X. Tan, M. Weyland, Y . Chen, T. Williams, P.N.H. Nakashima, L. Bourgeois, Growth of faceted, monolayer-coated nanovoids in aluminium, Acta Mater. 206 (2021) 116594

  8. [8]

    Chen, J.R

    X. Chen, J.R. Mianroodi, C. Liu, X. Zhou, D. Ponge, B. Gault, B. Svendsen, D. Raabe, Investigation of vacancy trapping by solutes during quenching in aluminum alloys, Acta Mater. 254 (2023) 118969

  9. [9]

    S. Wu, H.S. Soreide, B. Chen, J. Bian, C. Yang, C. Li, P. Zhang, P. Cheng, J. Zhang, Y . Peng, G. Liu, Y . Li, H.J. Roven, J. Sun, Freezing solute atoms in nanogra ined aluminum alloys via high -density vacancies, Nat. Commun. 13 (2022) 3495

  10. [10]

    Inoue, T

    K. Inoue, T. Yamashita, S. Nogami, A. Hasegawa, T. Toyama, Y . Nagai, Direct observation of voids decorated with transmuted rhenium atoms in neutron -irradiated tungsten by correlative use of TEM and APT, Materialia 32 (2023) 101963

  11. [11]

    Dürrschnabel, M

    M. Dürrschnabel, M. Klimenkov, U. Jäntsch, M. Rieth, H.C. Schneider, D. Terentyev, New insights into microstructure of neutron-irradiated tungsten, Sci. Rep. 11 (2021) 7572

  12. [12]

    Klimenkov, U

    M. Klimenkov, U. Jäntsch, M. Rieth, H.C. Schneider, D. Terentyev, W. Van Renterghem, Influence of transmutation-induced Re/Os content on defect evolution in neutron-irradiated W, J. Nucl. Mater. 592 (2024) 154950

  13. [13]

    Klimenkov, U

    M. Klimenkov, U. Jäntsch, M. Rieth, H.C. Schneider , D. Terentyev, W. Van Renterghem, Effect of irradiation parameters on defect evolution in neutron irradiated tungsten, J. Nucl. Mater. 607 (2025) 155673

  14. [14]

    Barashev, Y

    A. Barashev, Y . Osetsky, H. Bei, C. Lu, L. Wang, Y . Zhang, Chemically -biased diffusion and segregation impede void growth in irradiated Ni-Fe alloys, Curr. Opin. Solid State Mater. Sci. 23 (2019) 92-100

  15. [15]

    Kabir, T.T

    M. Kabir, T.T. Lau, X. Lin, S. Yip, K.J. Van Vliet, Effects of vacancy-solute clusters on diffusivity in metastable Fe-C alloys, Phys. Rev. B 82 (2010) 134112

  16. [16]

    Zhang, L

    Z.W. Zhang, L. Yao, X.L. Wang, M.K. Miller, Vacancy -controlled ultrastable nanoclusters in nanostructured ferritic alloys, Sci. Rep. 5 (2015) 10600

  17. [17]

    Konstantinović, G

    M.J. Konstantinović, G. Bonny, Thermal stability and the structure of vacancy –solute clusters in 30 iron alloys, Acta Mater. 85 (2015) 107-111

  18. [18]

    Elsayed, T.E.M

    M. Elsayed, T.E.M. Staab, J. Čížek, R. Krause -Rehberg, On the interaction of solute atoms with vacancies in diluted Al-alloys: A paradigmatic experimental and ab-initio study on indium and tin, Acta Mater. 219 (2021) 117228

  19. [19]

    Z. Yan, W. Zhou, J. Zheng, G. Wang, X. Liu, X. Liu, S. Wang, C. Gao, J. Tian, H. Wang, W. Yang, Q. Feng, Investigations of microstructure and tensile properties of neutron irradiated 6061 aluminum alloys, Mater. Sci. Eng. A 890 (2024) 145913

  20. [20]

    Wolff, M

    J. Wolff, M. Franz, J.E. Kluin, D. Schmid, Vacancy formation in nickel and α-nickel-carbon alloy, Acta Mater. 45 (1997) 4759-4764

  21. [21]

    Morgado, S

    F.F. Morgado, S. Katnagallu, C. Freysoldt, B. Klaes, F. Vurpillot, J. Neugebauer, D. Raa be, S. Neumeier, B. Gault, L.T. Stephenson, Revealing atomic -scale vacancy-solute interaction in nickel, Scr. Mater. 203 (2021) 114036

  22. [22]

    Takeyama, S

    T. Takeyama, S. Ohnuki, H. Takahashi, Direct observation of radiation induced segregation near grain boundary and void in copper alloys, Scr. Metall. 14 (1980) 1105-1110

  23. [23]

    Kluin, T

    J.E. Kluin, T. Hehenkamp, Comparison of positron -lifetime spectroscopy and differential dilatometric measurements of equilibrium vacancies in copper and α-Cu-Ge alloys, Phys. Rev. B 44 (1991) 11597-11608

  24. [24]

    Divinski, J

    S.V . Divinski, J. Ribbe, D. Baither, G. Schmitz, G. Reglitz, H. Rösner, K. Sato, Y . Estrin, G. Wilde, Nano- and micro-scale free volume in ultrafine grained Cu –1wt.%Pb alloy deformed by equal channel angular pressing, Acta Mater. 57 (2009) 5706-5717

  25. [25]

    Vincent, C.S

    E. Vincent, C.S. Becquart, C. Domain, Ab initio calculations of vacancy interactions with solute atoms in bcc Fe, Nucl. Instrum. Meth. B 228 (2005) 137-141

  26. [26]

    Ohnuma, N

    T. Ohnuma, N. Soneda, M. Iwasawa, First -principles calculations of vacancy –solute element interactions in body-centered cubic iron, Acta Mater. 57 (2009) 5947-5955

  27. [27]

    Gorbatov, P.A

    O.I. Gorbatov, P.A. Korzhavyi, A.V . Ruban, B. Johansson, Y .N. Gornostyrev, Vacancy –solute interactions in ferromagnetic and paramagnetic bcc iron: Ab initio calculations, J. Nucl. Mater. 419 (2011) 248-255

  28. [28]

    Lavrentiev, D

    M.Y . Lavrentiev, D. Nguyen-Manh, S.L. Dudarev, Chromium-vacancy clusters in dilute bcc Fe -Cr alloys: An ab initio study, J. Nucl. Mater. 499 (2018) 613-621

  29. [29]

    X.-S. Kong, X. Wu, Y .-W. You, C.S. Liu, Q.F. Fang, J.-L. Chen, G.N. Luo, Z. Wang, First-principles calculations of transition metal–solute interactions with point defects in tungsten, Acta Mater. 66 (2014) 172-183

  30. [30]

    Y .-W. You, X. -S. Kong, X. Wu, C.S. Liu, Q.F. Fang, J.L. Chen, G.N. Luo, Clu stering of transmutation elements tantalum, rhenium and osmium in tungsten in a fusion environment, Nucl. Fusion 57 (2017) 086006

  31. [31]

    Li, H.-B

    Y .-H. Li, H.-B. Zhou, S. Jin, Y . Zhang, H. Deng, G.-H. Lu, Behaviors of transmutation elements Re and Os and their effec ts on energetics and clustering of vacancy and self -interstitial atoms in W, Nucl. Fusion 57 (2017) 046006

  32. [32]

    Wolverton, Solute–vacancy binding in aluminum, Acta Mater

    C. Wolverton, Solute–vacancy binding in aluminum, Acta Mater. 55 (2007) 5867-5872

  33. [33]

    Francis, W.A

    M.F. Francis, W.A. Curtin, Microalloying for the controllable delay of precipitate formation in metal alloys, Acta Mater. 106 (2016) 117-128

  34. [34]

    J. Peng, S. Bahl, A. Shyam, J.A. Haynes, D. Shin, Solute -vacancy clustering in aluminum, Acta Mater. 196 (2020) 747-758

  35. [35]

    Zhang, L

    X. Zhang, L. Xu, W. Hu, H. Zhou, J. Wa ng, Effects of Sc on the vacancy and solute behaviours in 31 aluminium, J. Mater. Sci. Technol. 148 (2023) 41-51

  36. [36]

    Schuwalow, J

    S. Schuwalow, J. Rogal, R. Drautz, Vacancy mobility and interaction with transition metal solutes in Ni, J. Phys.: Condens. Matter 26 (2014) 485014

  37. [37]

    S. Zhao, G. Velisa, H. Xue, H. Bei, W.J. Weber, Y . Zhang, Suppression of vacancy cluster growth in concentrated solid solution alloys, Acta Mater. 125 (2017) 231-237

  38. [38]

    Klemradt, B

    U. Klemradt, B. Drittler, T. Hoshino, R. Zeller, P.H. Dederichs, N. St efanou, Vacancy-solute interactions in Cu, Ni, Ag, and Pd, Phys. Rev. B 43 (1991) 9487-9497

  39. [39]

    Y . Wang, H. Gao, Y . Han, Y . Dai, F. Bian, J. Wang, B. Sun, First-principles study of solute–vacancy binding in Cu, J. Alloys Compd. 608 (2014) 334-337

  40. [40]

    Lifshitz, V .V

    I.M. Lifshitz, V .V . Slyozov, The kinetics of precipitation from supersaturated solid solutions, J. Phys. Chem. Solids 19 (1961) 35-50

  41. [41]

    Wagner, Theorie der Alterung von Niederschlägen durch Umlösen (Ostwald -Reifung), Z

    C. Wagner, Theorie der Alterung von Niederschlägen durch Umlösen (Ostwald -Reifung), Z. Elektrochem. Ber. Bunsenges. Phys. Chem. 65 (1961) 581-591

  42. [42]

    Sanchez, F

    J.M. Sanchez, F. Ducastelle, D. Gratias, Generalized cluster description of multicomponent systems, Phys. A 128 (1984) 334-350

  43. [43]

    Sanchez, Cluster expansion and the configurational theory of alloys, Phys

    J.M. Sanchez, Cluster expansion and the configurational theory of alloys, Phys. Rev. B 8 1 (2010) 224202

  44. [44]

    Wróbel, D

    J.S. Wróbel, D. Nguyen -Manh, K.J. Kurzydłowski, S.L. Dudarev, A first -principles model for anomalous segregation in dilute ternary tungsten -rhenium-vacancy alloys, J. Phys.: Condens. Matter 29 (2017) 145403

  45. [45]

    Nguyen -Manh, J.S

    D. Nguyen -Manh, J.S. Wróbel, M. Klimenkov, M.J. Lloyd, L. Messina, S.L. Dudarev, First - principles model for voids decorated by transmutation solutes: Short-range order effects and application to neutron irradiated tungsten, Phys. Rev. Mater. 5 (2021) 065401

  46. [46]

    Lloyd, E

    M.J. Lloyd, E . Martinez, L. Messina, D. Nguyen -Manh, Development of a solute and defect concentration dependant Ising model for the study of transmutation induced segregation in neutron irradiated W-(Re, Os) systems, J. Phys.: Condens. Matter 33 (2021) 475902

  47. [47]

    C. -H. Huang, L. Gharaee, Y . Zhao, P. Erhart, J. Marian, Mechanism of nucleation and incipient growth of Re clusters in irradiated W -Re alloys from kinetic Monte Carlo simulations, Phys. Rev. B 96 (2017) 094108

  48. [48]

    C. -H. Huang, M.R. Gilbert, J. Marian, Simul ating irradiation hardening in tungsten under fast neutron irradiation including Re production by transmutation, J. Nucl. Mater. 499 (2018) 204-215

  49. [49]

    Li, F.-Y

    Y .-H. Li, F.-Y . Yue, Z.-Z. Li, P.-W. Hou, Y .-Z. Niu, H.-Z. Ma, Y . Zhang, X.-X. Hu, H.-Q. Deng, H.- B. Zhou, F. Gao, G. -H. Lu, Temperature -dependent synergistic evolution mechanism of rhenium and irradiation defects in tungsten-rhenium alloys, J. Mater. Sci. Technol. 145 (2023) 221-234

  50. [50]

    Niu, Y .-H

    Y .-Z. Niu, Y .-H. Li, H.-Z. Ma, T.-R. Yang, X.-X. Hu, H.-B. Zhou, G.-H. Lu, Influence of Re on the performance of W under irradiation: The critical role of introduction method and rate, J. Mater. Sci. Technol. 241 (2026) 123-137

  51. [51]

    Kresse, J

    G. Kresse, J. Hafner, Ab initio molecular dynamics for liquid metals, Phys. Rev. B 47 (19 93) 558- 561

  52. [52]

    Kresse, J

    G. Kresse, J. Furthmüller, Efficiency of ab -initio total energy calculations for metals and semiconductors using a plane-wave basis set, Comput. Mater. Sci. 6 (1996) 15-50

  53. [53]

    Kresse, J

    G. Kresse, J. Furthmüller, Efficient iterative schemes for a b initio total-energy calculations using a plane-wave basis set, Phys. Rev. B 54 (1996) 11169-11186

  54. [54]

    Blochl, Projector augmented-wave method, Phys

    P.E. Blochl, Projector augmented-wave method, Phys. Rev. B 50 (1994) 17953-17979. 32

  55. [55]

    Perdew, K

    J.P. Perdew, K. Burke, M. Ernzerhof, Generalized Gradient Approximation Made Simple, Phys. Rev. Lett. 77 (1996) 3865-3868

  56. [56]

    Monkhorst, J.D

    H.J. Monkhorst, J.D. Pack, Special points for Brillouin -zone integrations, Phys. Rev. B 13 (1976) 5188-5192

  57. [57]

    Momma, F

    K. Momma, F. Izumi, VESTA 3 for three -dimensional visualization of crystal, volumetric and morphology data, J. Appl. Cryst. 44 (2011) 1272-1276

  58. [58]

    Friedman, Greedy function approximation: A gradient boosting machine, Ann

    J.H. Friedman, Greedy function approximation: A gradient boosting machine, Ann. Statist. 29 (2001) 1189-1232

  59. [59]

    Pedregosa, G

    F. Pedregosa, G. Varoquaux, A. Gramfort, V . Michel, B. Thi rion, O. Grisel, M. Blondel, P. Prettenhofer, R. Weiss, V . Dubourg, J. Vanderplas, A. Passos, D. Cournapeau, M. Brucher, M. Perrot, E. Duchesnay, Scikit-learn: Machine Learning in Python, J. Mach. Learn. Res. 12 (2011) 2825-2830

  60. [60]

    Thompson, H.M

    A.P. Thompson, H.M. Aktulga, R. Berger, D.S. Bolintineanu, W.M. Brown, P.S. Crozier, P.J. in 't Veld, A. Kohlmeyer, S.G. Moore, T.D. Nguyen, R. Shan, M.J. Stevens, J. Tranchida, C. Trott, S.J. Plimpton, LAMMPS - a flexible simulation tool for particle -based materials modeling at the atomic, meso, and continuum scales, Comput. Phys. Commun. 271 (2022) 108171

  61. [61]

    Chen, Y .-H

    Y . Chen, Y .-H. Li, N. Gao, H. -B. Zhou, W. Hu, G. -H. Lu, F. Gao, H. Deng, New interatomic potentials of W, Re and W-Re alloy for radiation defects, J. Nucl. Mater. 502 (2018) 141-153

  62. [62]

    Y . Chen, J. Fang, L. Liu, W. Hu, C. Jiang, N. Gao, H. -B. Zhou, G. -H. Lu, F. Gao, H. Deng, The interactions between rhenium and interstitial -type defects in bulk tungsten: A combined study by molecular dynamics and molecular statics simulations, J. Nucl. Mater. 522 (2019) 200-211

  63. [63]

    Setyawan, N

    W. Setyawan, N. Gao, R.J. Kurtz, A tungsten-rhenium interatomic potential for point defect studies, J. Appl. Phys. 123 (2018) 205102

  64. [64]

    Bonny, A

    G. Bonny, A. Bakaev, D. Terentyev, Y .A. Mastrikov, Interatomic pot ential to study plastic deformation in tungsten-rhenium alloys, J. Appl. Phys. 121 (2017) 165107

  65. [65]

    Hou, Y .-W

    J. Hou, Y .-W. You, X.-S. Kong, J. Song, C.S. Liu, Accurate prediction of vacancy cluster structures and energetics in bcc transition metals, Acta Mater. 211 (2021) 116860

  66. [66]

    Hou, X.S

    J. Hou, X.S. Kong, X. Wu, J. Song, C.S. Liu, Predictive model of hydrogen trapping and bubbling in nanovoids in bcc metals, Nat. Mater. 18 (2019) 833-839

  67. [67]

    Xu, D.E.J

    A. Xu, D.E.J. Armstrong, C. Beck, M.P. Moody, G.D.W. Smith, P.A.J. Bagot , S.G. Roberts, Ion - irradiation induced clustering in W -Re-Ta, W-Re and W -Ta alloys: An atom probe tomography and nanoindentation study, Acta Mater. 124 (2017) 71-78