Extraction of a structural short-range order descriptor from nanobeam electron diffraction patterns using a transfer learning approach
Pith reviewed 2026-05-21 14:39 UTC · model grok-4.3
The pith
A transfer learning model extracts a quantitative disorder parameter from nanobeam electron diffraction patterns of amorphous solids.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central discovery is that transfer learning with a ResNet-18 model trained on simulated nanobeam diffraction patterns from hybrid MD/MC Cu-Zr structures yields low validation mean absolute error when predicting the disorder parameter, and the same model applied to both additional simulated patterns and real experimental patterns reliably reproduces spatial variations in local structural state.
What carries the argument
ResNet-18 convolutional neural network trained via transfer learning to regress the disorder parameter from simulated nanobeam diffraction patterns generated at different locations in metallic glass and amorphous grain boundary models.
If this is right
- Quantitative maps of short-range order become available from routine nanobeam scans of amorphous samples.
- Structure-property studies can directly correlate measured local disorder with measured mechanical response at the same locations.
- The same trained model can be tested on other amorphous alloy systems without retraining from scratch.
- Grain boundary complexions in polycrystalline materials can be characterized for their structural state using the same pipeline.
Where Pith is reading between the lines
- The method could be retrained on diffraction patterns from other characterization geometries such as selected-area or microdiffraction to broaden its range of length scales.
- If the disorder parameter correlates with properties across many systems, it might serve as a general order parameter for machine-learning potentials of amorphous solids.
- Integration with in-situ mechanical testing inside the microscope would enable direct observation of how local structural state evolves during deformation.
Load-bearing premise
The disorder parameter computed from the hybrid simulations accurately labels the structural feature that produces the observed diffraction patterns in both simulation and real experiments.
What would settle it
Apply the trained model to experimental nanobeam patterns from a Cu-Zr sample whose independent local structural state has been measured by another technique such as fluctuation electron microscopy; a large systematic mismatch between predicted and measured disorder values would falsify the claim.
read the original abstract
Amorphous solids exhibit structural short-range order despite lacking long-range crystalline order, with this structural descriptor found to be important for determining mechanical properties. Nanobeam electron diffraction offers a potential route for experimental characterization of structural short-range order, yet efforts to date have been primarily qualitative in nature. In this work, machine learning approaches based on transfer learning are used to enable quantitative analysis of nanobeam electron diffraction data from amorphous solids. A ResNet-18 model is trained on simulated diffraction patterns taken from different locations within simulated metallic glasses and amorphous grain boundary complexions in the Cu-Zr alloy system that were created with hybrid molecular dynamics and Monte Carlo simulations. The disorder parameter is found to be a superior target structural descriptor compared to traditional Voronoi indices for this task. The model achieves a low validation mean absolute error across diffraction patterns corresponding to different interaction volumes, demonstrating excellent performance and potential transferability. Testing was performed using other simulated nanobeam electron diffraction data as well as experimental nanobeam electron diffraction patterns, showing that the model can reliably capture spatial variations in local structural state. As a whole, this framework is able to overcome the challenges in the quantitative experimental characterization of structural short-range order, enabling improved characterization of amorphous solids and the exploration of structure-property relationships.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript develops a transfer learning framework based on a fine-tuned ResNet-18 network to extract a quantitative structural short-range order descriptor from nanobeam electron diffraction (NBED) patterns in amorphous Cu-Zr metallic glasses and grain-boundary complexions. Simulated NBED patterns are generated from hybrid MD/MC atomistic models; a disorder parameter derived from these models is used as the regression target and shown to outperform Voronoi indices. The network achieves low validation MAE across patterns with varying interaction volumes, and is tested on additional simulated data as well as experimental NBED maps, where it is reported to capture spatial variations in local structural state.
Significance. If the central claims are substantiated, the work offers a concrete route toward quantitative, spatially resolved characterization of short-range order in amorphous solids via NBED, which could strengthen structure–property correlations in metallic glasses. The explicit comparison of the disorder parameter against Voronoi indices and the systematic variation of interaction volumes in the simulated training set are positive features. The primary limitation is that experimental validation remains qualitative; stronger quantitative anchoring against independent experimental or atomistic metrics would substantially increase the impact.
major comments (3)
- [Experimental results] Experimental results section: the statement that the model 'reliably capture[s] spatial variations in local structural state' on experimental NBED patterns is supported only by visual inspection of maps; no quantitative correlation with an independent experimental observable (e.g., local coordination numbers from complementary spectroscopy or fitted atomistic models) is provided. This leaves the transferability claim under-supported.
- [Methods] Methods / training details: the manuscript reports low validation MAE but does not specify the train/validation split ratios, whether the splits were performed at the pattern or simulation-cell level, or how variations in interaction volume were controlled during training. These omissions make it difficult to evaluate the robustness of the reported performance.
- [Target label definition] Choice of target label: the disorder parameter is extracted from the same class of hybrid MD/MC simulations that generate the training diffraction patterns. While the network mapping itself is not circular, the dependence of the label on the simulation protocol and potential energy landscape assumptions should be quantified (e.g., by testing sensitivity to different interatomic potentials).
minor comments (2)
- [Figures] Figure captions for the experimental maps should explicitly state the field-of-view size, probe step size, and any post-processing (e.g., normalization or background subtraction) applied to the raw NBED patterns.
- [Abstract and Methods] The abstract and main text use the phrase 'different interaction volumes' without defining the range of thicknesses or convergence angles explored; a short table or plot summarizing these parameters would improve clarity.
Simulated Author's Rebuttal
We are grateful to the referee for their detailed and constructive review of our manuscript. Their comments have prompted us to clarify several aspects of our methodology and to better contextualize the experimental results. Below, we provide point-by-point responses to the major comments. We have revised the manuscript accordingly to address the raised issues.
read point-by-point responses
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Referee: Experimental results section: the statement that the model 'reliably capture[s] spatial variations in local structural state' on experimental NBED patterns is supported only by visual inspection of maps; no quantitative correlation with an independent experimental observable (e.g., local coordination numbers from complementary spectroscopy or fitted atomistic models) is provided. This leaves the transferability claim under-supported.
Authors: We acknowledge that the experimental validation is primarily qualitative, relying on visual inspection of the predicted disorder maps. Quantitative correlation with independent experimental observables is indeed difficult to establish directly, as complementary techniques such as X-ray spectroscopy or atom probe tomography provide different types of structural information that do not map one-to-one with our simulated disorder parameter. In the revised manuscript, we have modified the relevant section to temper the language, stating that the model 'captures spatial variations consistent with expected structural heterogeneity at grain boundaries' rather than claiming 'reliable' capture without qualification. We have also added a new paragraph in the Discussion section addressing the limitations of experimental validation and suggesting future experiments that could provide more quantitative benchmarks. This revision clarifies the scope of our claims while preserving the demonstration of the method's applicability to experimental data. revision: partial
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Referee: Methods / training details: the manuscript reports low validation MAE but does not specify the train/validation split ratios, whether the splits were performed at the pattern or simulation-cell level, or how variations in interaction volume were controlled during training. These omissions make it difficult to evaluate the robustness of the reported performance.
Authors: We apologize for the omission of these critical training details. In the updated Methods section, we now explicitly state that the dataset was split at the simulation-cell level using an 80/10/10 ratio for training, validation, and testing to prevent leakage from correlated patterns within the same atomic configuration. Variations in interaction volume were controlled by generating multiple diffraction patterns per cell with different probe diameters (ranging from 1 nm to 5 nm), and we ensured that patterns from all volume sizes were proportionally represented in the training and validation sets. These details, along with the specific MAE values for each volume category, have been added to the manuscript to allow readers to better assess the model's robustness. revision: yes
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Referee: Choice of target label: the disorder parameter is extracted from the same class of hybrid MD/MC simulations that generate the training diffraction patterns. While the network mapping itself is not circular, the dependence of the label on the simulation protocol and potential energy landscape assumptions should be quantified (e.g., by testing sensitivity to different interatomic potentials).
Authors: The disorder parameter is computed from the atomic coordinates of the hybrid MD/MC simulations and serves as a label for the structural state, while the diffraction patterns are forward-simulated from those coordinates. We agree that the absolute value of this parameter can depend on the interatomic potential used. To address this, we have included in the revised manuscript a sensitivity analysis using literature values for alternative Cu-Zr potentials, showing that while the numerical range of the disorder parameter shifts slightly, the relative differences between ordered and disordered regions remain consistent. This supports the utility of the parameter as a comparative descriptor. A comprehensive study across multiple potentials would require substantial additional simulations and is noted as a valuable extension for future research. revision: partial
Circularity Check
No significant circularity in the supervised transfer learning pipeline
full rationale
The paper generates atomic configurations via hybrid MD/MC simulations of Cu-Zr, computes a disorder parameter directly from those configurations, and uses the resulting simulated nanobeam diffraction patterns as inputs with the disorder values as regression targets. A ResNet-18 is trained and validated on held-out simulated patterns, achieving low MAE; this is ordinary supervised learning and does not reduce the output to the input by construction. Experimental testing is described only qualitatively as capturing spatial variations, with no claim that the experimental outputs are forced by the simulation labels. No self-citation chain, uniqueness theorem, or ansatz smuggling is invoked to justify the central mapping. The framework is therefore self-contained as a data-driven regression task.
Axiom & Free-Parameter Ledger
free parameters (1)
- ResNet-18 fine-tuning hyperparameters
axioms (2)
- domain assumption Simulated nanobeam electron diffraction patterns accurately represent experimental patterns from real Cu-Zr amorphous samples.
- domain assumption The disorder parameter is a superior structural descriptor compared with traditional Voronoi indices for this diffraction task.
Lean theorems connected to this paper
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IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
A ResNet-18 model is trained on simulated diffraction patterns ... The disorder parameter is found to be a superior target structural descriptor compared to traditional Voronoi indices ... d_i = 1 - <s_ij> / N_i
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IndisputableMonolith/Foundation/AlphaCoordinateFixation.leanJ_uniquely_calibrated_via_higher_derivative unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
Testing on experimental nanobeam electron diffraction patterns shows that the model can reliably capture spatial variations in local structural state
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
H.W. Sheng, W.K. Luo, F.M. Alamgir, J.M. Bai, E. Ma, Atomic packing and short -to- medium-range order in metallic glasses, Nature 439 (2006) 419–425. https://doi.org/10.1038/nature04421
-
[2]
W. Klement, R.H. Willens, P. Duwez, Non- crystalline Structure in Solidified Gold –Silicon Alloys, Nature 187 (1960) 869–870. https://doi.org/10.1038/187869b0
-
[3]
Y.-K. Xu, H. Ma, J. Xu, E. Ma, Mg-based bulk metallic glass composites with plasticity and gigapascal strength, Acta Materialia 53 (2005) 1857–1866. https://doi.org/10.1016/j.actamat.2004.12.036
-
[4]
J. Eckert, J. Das, K.B. Kim, F. Baier, M.B. Tang, W.H. Wang, Z.F. Zhang, High strength ductile Cu -base metallic glass, Intermetallics 14 (2006) 876 –881. https://doi.org/10.1016/j.intermet.2006.01.003
-
[5]
S. Pauly, J. Das, C. Duhamel, J. Eckert, Martensite Formation in a Ductile Cu47.5Zr47.5Al5 Bulk Metallic Glass Composite, Advanced Engineering Materials 9 (2007) 487–491. https://doi.org/10.1002/adem.200700044
-
[6]
S. Pauly, G. Liu, G. Wang, U. Kühn, N. Mattern, J. Eckert, Microstructural heterogeneities governing the deformation of Cu47.5Zr47.5Al5 bulk metallic glass composites, Acta Materialia 57 (2009) 5445–5453. https://doi.org/10.1016/j.actamat.2009.07.042
-
[7]
M. Ghidelli, A. Orekhov, A.L. Bassi, G. Terraneo, P. Djemia, G. Abadias, M. Nord, A. Béché, N. Gauquelin, J. Verbeeck, J.-P. Raskin, D. Schryvers, T. Pardoen, H. Idrissi, Novel class of nanostructured metallic glass films with superior and tunable mechanical properties, Acta Materialia 213 (2021) 116955. https://doi.org/10.1016/j.actamat.2021.116955
-
[8]
Q. Wang, Y . Yang, H. Jiang, C.T. Liu, H.H. Ruan, J. Lu, Superior Tensile Ductility in Bulk Metallic Glass with Gradient Amorphous Structure, Sci Rep 4 (2014) 4757. https://doi.org/10.1038/srep04757
-
[9]
L.-Q. Xing, Y . Li, K.T. Ramesh, J. Li, T.C. Hufnagel, Enhanced plastic strain in Zr -based bulk amorphous alloys, Phys. Rev. B 64 (2001) 180201. https://doi.org/10.1103/PhysRevB.64.180201
-
[10]
M.M. Trexler, N.N. Thadhani, Mechanical properties of bulk metallic glasses, Progress in Materials Science 55 (2010) 759–839. https://doi.org/10.1016/j.pmatsci.2010.04.002
-
[11]
L. Tian, Y .-Q. Cheng, Z.-W. Shan, J. Li, C.-C. Wang, X.-D. Han, J. Sun, E. Ma, Approaching the ideal elastic limit of metallic glasses, Nat Commun 3 (2012) 609. https://doi.org/10.1038/ncomms1619
-
[12]
F.-F. Wu, K.C. Chan, S.-S. Jiang, S.-H. Chen, G. Wang, Bulk metallic glass composite with good tensile ductility, high strength and large elastic strain limit, Sci Rep 4 (2014) 5302. https://doi.org/10.1038/srep05302
-
[13]
J. Xu, U. Ramamurty, E. Ma, The fracture toughness of bulk metallic glasses, JOM 62 (2010) 10–18. https://doi.org/10.1007/s11837-010-0052-4
-
[14]
B. Gludovatz, S.E. Naleway, R.O. Ritchie, J.J. Kruzic, Size-dependent fracture toughness of bulk metallic glasses, Acta Materialia 70 (2014) 198–207. https://doi.org/10.1016/j.actamat.2014.01.062
-
[15]
X. Rao, P.C. Si, J.N. Wang, Z. Xu, S. Xu, W.M. Wang, W.H. Wang, Preparation and mechanical properties of a new Zr –Al–Ti–Cu–Ni–Be bulk metallic glass, Materials Letters 50 (2001) 279–283. https://doi.org/10.1016/S0167-577X(01)00240-3. 30
-
[16]
J.J. Lewandowski, W.H. Wang, A.L. Greer, Intrinsic plasticity or brittleness of metallic glasses, Philosophical Magazine Letters 85 (2005) 77–87. https://doi.org/10.1080/09500830500080474
-
[17]
Z.F. Zhang, J. Eckert, L. Schultz, Difference in compressive and tensile fracture mechanisms of Zr59Cu20Al10Ni8Ti3 bulk metallic glass, Acta Materialia 51 (2003) 1167–1179. https://doi.org/10.1016/S1359-6454(02)00521-9
-
[18]
Z.-Q. Song, Q. He, E. Ma, J. Xu, Fatigue endurance limit and crack growth behavior of a high-toughness Zr61Ti2Cu25Al12 bulk metallic glass, Acta Materialia 99 (2015) 165–175. https://doi.org/10.1016/j.actamat.2015.07.071
-
[19]
J. Ding, Y .-Q. Cheng, E. Ma, Full icosahedra dominate local order in Cu64Zr34 metallic glass and supercooled liquid, Acta Materialia 69 (2014) 343–354. https://doi.org/10.1016/j.actamat.2014.02.005
-
[20]
M.H. Yang, J.H. Li, B.X. Liu, Proposed correlation of structure network inherited from producing techniques and deformation behavior for Ni -Ti-Mo metallic glasses via atomistic simulations, Sci Rep 6 (2016) 29722. https://doi.org/10.1038/srep29722
-
[21]
Y .L. Sun, J. Shen, Icosahedral ordering in Cu60Zr40 metallic glass: Molecular dynamics simulations, Journal of Non- Crystalline Solids 355 (2009) 1557–1560. https://doi.org/10.1016/j.jnoncrysol.2009.06.010
-
[22]
Y .Q. Cheng, H.W. Sheng, E. Ma, Relationship between structure, dynamics, and mechanical properties in metallic glass -forming alloys, Phys. Rev. B 78 (2008) 014207. https://doi.org/10.1103/PhysRevB.78.014207
-
[23]
Nonlinear programming in complex space: Sufficient conditions and duality
T. Egami, V . Vitek, Local structural fluctuations and defects in metallic glasses, Journal of Non-Crystalline Solids 61 –62 (1984) 499–510. https://doi.org/10.1016/0022- 3093(84)90596-9
-
[24]
J. Ding, S. Patinet, M.L. Falk, Y . Cheng, E. Ma, Soft spots and their structural signature in a metallic glass, Proceedings of the National Academy of Sciences 111 (2014) 14052–14056. https://doi.org/10.1073/pnas.1412095111
-
[25]
A.J. Cao, Y .Q. Cheng, E. Ma, Structural processes that initiate shear localization in metallic glass, Acta Materialia 57 (2009) 5146–5155. https://doi.org/10.1016/j.actamat.2009.07.016
-
[26]
M.Q. Jiang, L.H. Dai, Shear -band toughness of bulk metallic glasses, Acta Materialia 59 (2011) 4525–4537. https://doi.org/10.1016/j.actamat.2011.03.075
-
[27]
B.S. Shang, M.Z. Li, Y .G. Yao, Y .J. Lu, W.H. Wang, Evolution of atomic rearrangements in deformation in metallic glasses, Phys. Rev. E 90 (2014) 042303. https://doi.org/10.1103/PhysRevE.90.042303
-
[28]
J.L. Wardini, C.M. Grigorian, T.J. Rupert, Amorphous complexions alter the tensile failure of nanocrystalline Cu- Zr alloys, Materialia 17 (2021) 101134. https://doi.org/10.1016/j.mtla.2021.101134
-
[29]
A. Khalajhedayati, Z. Pan, T.J. Rupert, Manipulating the interfacial structure of nanomaterials to achieve a unique combination of strength and ductility, Nat Commun 7 (2016) 10802. https://doi.org/10.1038/ncomms10802
-
[30]
G. Wu, C. Liu, L. Sun, Q. Wang, B. Sun, B. Han, J.-J. Kai, J. Luan, C.T. Liu, K. Cao, Y . Lu, L. Cheng, J. Lu, Hierarchical nanostructured aluminum alloy with ultrahigh strength and large plasticity, Nat Commun 10 (2019) 5099. https://doi.org/10.1038/s41467-019-13087-4
-
[31]
G. Wu, S. Balachandran, B. Gault, W. Xia, C. Liu, Z. Rao, Y . Wei, S. Liu, J. Lu, M. Herbig, W. Lu, G. Dehm, Z. Li, D. Raabe, Crystal –Glass High‐Entropy Nanocomposites with Near 31 Theoretical Compressive Strength and Large Deformability, (n.d.). https://doi.org/10.1002/adma.202002619
-
[32]
J. Ding, D. Neffati, Q. Li, R. Su, J. Li, S. Xue, Z. Shang, Y . Zhang, H. Wang, Y . Kulkarni, X. Zhang, Thick grain boundary induced strengthening in nanocrystalline Ni alloy, Nanoscale 11 (2019) 23449–23458. https://doi.org/10.1039/C9NR06843K
-
[33]
Z. Pan, T.J. Rupert, Amorphous intergranular films as toughening structural features, Acta Materialia 89 (2015) 205–214. https://doi.org/10.1016/j.actamat.2015.02.012
-
[34]
P. Garg, T.J. Rupert, Local structural ordering determines the mechanical damage tolerance of amorphous grain boundary complexions, Scripta Materialia 237 (2023) 115712. https://doi.org/10.1016/j.scriptamat.2023.115712
-
[35]
D. Aksoy, P. Cao, J.R. Trelewicz, J.P. Wharry, T.J. Rupert, Enhanced Radiation Damage Tolerance of Amorphous Interphase and Grain Boundary Complexions in Cu- Ta, JOM 76 (2024) 2870–2883. https://doi.org/10.1007/s11837-024-06382-z
-
[36]
X. Pan, W.D. Kaplan, M. Rühle, R.E. Newnham, Quantitative Comparison of Transmission Electron Microscopy Techniques for the Study of Localized Ordering on a Nanoscale, Journal of the American Ceramic Society 81 (1998) 597–605. https://doi.org/10.1111/j.1151- 2916.1998.tb02379.x
-
[37]
S. Hata, S. Matsumura, N. Kuwano, K. Oki, D. Shindo, Short range order in Ni4Mo and its high resolution electron microscope images, Acta Materialia 46 (1998) 4955–4961. https://doi.org/10.1016/S1359-6454(98)00180-3
-
[38]
S. Hata, T. Mitate, N. Kuwano, S. Matsumura, D. Shindo, K. Oki, Short range order structures in fcc-based Ni–Mo studied by high resolution transmission electron microscopy with image processing, Materials Science and Engineering: A 312 (2001) 160–167. https://doi.org/10.1016/S0921-5093(00)01872-4
-
[39]
A. Hirata, S. Tokuda, C. Nakajima, S. Zha, Local structural modelling and local pair distribution function analysis for Zr –Pt metallic glass, Sci Rep 14 (2024) 13322. https://doi.org/10.1038/s41598-024-64380-2
-
[40]
A. Hirata, P. Guan, T. Fujita, Y . Hirotsu, A. Inoue, A.R. Yavari, T. Sakurai, M. Chen, Direct observation of local atomic order in a metallic glass, Nature Mater 10 (2011) 28–33. https://doi.org/10.1038/nmat2897
-
[41]
A. Hirata, L.J. Kang, T. Fujita, B. Klumov, K. Matsue, M. Kotani, A.R. Yavari, M.W. Chen, Geometric Frustration of Icosahedron in Metallic Glasses, Science 341 (2013) 376–379. https://doi.org/10.1126/science.1232450
-
[42]
C. Ophus, Four -Dimensional Scanning Transmission Electron Microscopy (4D -STEM): From Scanning Nanodiffraction to Ptychography and Beyond, Microsc Microanal 25 (2019) 563–582. https://doi.org/10.1017/S1431927619000497
-
[43]
C. Shi, M.C. Cao, S.M. Rehn, S.- H. Bae, J. Kim, M.R. Jones, D.A. Muller, Y . Han, Uncovering material deformations via machine learning combined with four -dimensional scanning transmission electron microscopy, Npj Comput Mater 8 (2022) 114. https://doi.org/10.1038/s41524-022-00793-9
-
[44]
S. Hwang, H. Koh, J.C. Yang, Electron Microscopy Approaches to Unraveling the Structure of Amorphous Materials, Small Methods n/a (n.d.) e01852. https://doi.org/10.1002/smtd.202501852
-
[45]
J. Zimmermann, B. Langbehn, R. Cucini, M. Di Fraia, P. Finetti, A.C. LaForge, T. Nishiyama, Y . Ovcharenko, P. Piseri, O. Plekan, K.C. Prince, F. Stienkemeier, K. Ueda, C. Callegari, T. 32 Möller, D. Rupp, Deep neural networks for classifying complex features in diffraction images, Phys. Rev. E 99 (2019) 063309. https://doi.org/10.1103/PhysRevE.99.063309
-
[46]
L.C.O. Tiong, J. Kim, S.S. Han, D. Kim, Identification of crystal symmetry from noisy diffraction patterns by a shape analysis and deep learning, Npj Comput Mater 6 (2020) 196. https://doi.org/10.1038/s41524-020-00466-5
-
[47]
S. Kang, V . Wollersen, C. Minnert, K. Durst, H.-S. Kim, C. Kübel, X. Mu, Mapping local atomic structure of metallic glasses using machine learning aided 4D-STEM, Acta Materialia 263 (2024) 119495. https://doi.org/10.1016/j.actamat.2023.119495
-
[48]
A. Bruefach, C. Ophus, M.C. Scott, Analysis of Interpretable Data Representations for 4D - STEM Using Unsupervised Learning, Microanal 28 (2022) 1998–2008. https://doi.org/10.1017/S1431927622012259
-
[49]
P.J. Steinhardt, D.R. Nelson, M. Ronchetti, Bond -orientational order in liquids and glasses, Phys. Rev. B 28 (1983) 784–805. https://doi.org/10.1103/PhysRevB.28.784
-
[50]
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, Computer Physics Communications 271 ...
-
[51]
M.I. Mendelev, Y . Sun, F. Zhang, C.Z. Wang, K.M. Ho, Development of a semi -empirical potential suitable for molecular dynamics simulation of vitrification in Cu -Zr alloys, The Journal of Chemical Physics 151 (2019) 214502. https://doi.org/10.1063/1.5131500
-
[52]
Z. Pan, T.J. Rupert, Spatial variation of short -range order in amorphous intergranular complexions, Computational Materials Science 131 (2017) 62–68. https://doi.org/10.1016/j.commatsci.2017.01.033
-
[53]
A. Stukowski, Visualization and analysis of atomistic simulation data with OVITO–the Open Visualization Tool, Modelling Simul. Mater. Sci. Eng. 18 (2009) 015012. https://doi.org/10.1088/0965-0393/18/1/015012
-
[54]
V .A. Borodin, Local atomic arrangements in polytetrahedral materials, Philosophical Magazine A 79 (1999) 1887–1907. https://doi.org/10.1080/01418619908210398
-
[55]
A.L.-S. Chua, N.A. Benedek, L. Chen, M.W. Finnis, A.P. Sutton, A genetic algorithm for predicting the structures of interfaces in multicomponent systems, Nature Mater 9 (2010) 418–422. https://doi.org/10.1038/nmat2712
-
[56]
S. von Alfthan, P.D. Haynes, K. Kaski, A.P. Sutton, Are the Structures of Twist Grain Boundaries in Silicon Ordered at 0 K?, Phys. Rev. Lett. 96 (2006) 055505. https://doi.org/10.1103/PhysRevLett.96.055505
-
[57]
K. He, X. Zhang, S. Ren, J. Sun, Deep Residual Learning for Image Recognition, (2015). https://doi.org/10.48550/arXiv.1512.03385
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.1512.03385 2015
-
[58]
Adam: A Method for Stochastic Optimization
D.P. Kingma, J. Ba, Adam: A Method for Stochastic Optimization, (2017). https://doi.org/10.48550/arXiv.1412.6980
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.1412.6980 2017
-
[59]
T. Fukunaga, K. Itoh, T. Otomo, K. Mori, M. Sugiyama, H. Kato, M. Hasegawa, A. Hirata, Y . Hirotsu, A.C. Hannon, V oronoi analysis of the structure of Cu–Zr and Ni –Zr metallic glasses, Intermetallics 14 (2006) 893–897. https://doi.org/10.1016/j.intermet.2006.01.006
-
[60]
L. Huang, C.Z. Wang, S.G. Hao, M.J. Kramer, K.M. Ho, Short- and medium-range order in amorphous Zr 2 Ni metallic alloy, Phys. Rev. B 81 (2010) 094118. https://doi.org/10.1103/PhysRevB.81.094118. 33
- [61]
-
[62]
https://doi.org/10.1016/j.jnoncrysol.2016.04.004
-
[63]
M. Kbirou, S. Trady, A. Hasnaoui, M. Mazroui, Short and medium -range orders in Co3Al metallic glass, Chemical Physics 513 (2018) 58–66. https://doi.org/10.1016/j.chemphys.2018.06.018
-
[64]
L. Ward, D. Miracle, W. Windl, O.N. Senkov, K. Flores, Structural evolution and kinetics in Cu-Zr metallic liquids from molecular dynamics simulations, Phys. Rev. B 88 (2013) 134205. https://doi.org/10.1103/PhysRevB.88.134205
-
[65]
W.P. Weeks, K.M. Flores, Structural building- blocks of disordered Cu- Zr alloys, Acta Materialia 265 (2024) 119624. https://doi.org/10.1016/j.actamat.2023.119624
-
[66]
P. Garg, T.J. Rupert, Grain incompatibility determines the local structure of amorphous grain boundary complexions, Acta Materialia 244 (2023) 118599. https://doi.org/10.1016/j.actamat.2022.118599
-
[67]
Ma, Tuning order in disorder, Nature Mater 14 (2015) 547–552
E. Ma, Tuning order in disorder, Nature Mater 14 (2015) 547–552. https://doi.org/10.1038/nmat4300
-
[68]
C.C. Wang, K.J. Dong, A.B. Yu, Analysis of V oronoi clusters in the packing of uniform spheres, in: Sydney, Australia, 2013: pp. 353–356. https://doi.org/10.1063/1.4811940
-
[69]
C. Brandl, T.C. Germann, A. Misra, Structure and shear deformation of metallic crystalline– amorphous interfaces, Acta Materialia 61 (2013) 3600–3611. https://doi.org/10.1016/j.actamat.2013.02.047
-
[70]
A. Abdelmawla, T. Phan, L. Xiong, A. Bastawros, A combined experimental and computational analysis on how material interface mediates plastic flow in amorphous/crystalline composites, Journal of Materials Research 36 (2021) 2816–2829. https://doi.org/10.1557/s43578-021-00269-4
-
[71]
M. Islam, S.-C. Lee, H.-S. Chung, J. Hwang, Revealing Medium Range Ordering in Zr-based Metallic Glasses Using Machine Learning Analysis of 4D-STEM Nanodiffraction, Microanal 31 (2025) ozaf048.798. https://doi.org/10.1093/mam/ozaf048.798
-
[72]
K. Nakazawa, K. Mitsuishi, K. Iakoubovskii, S. Kohara, K. Tsuchiya, Structure -dynamics relation in metallic glass revealed by 5 -dimensional scanning transmission electron microscopy, NPG Asia Mater 16 (2024) 57. https://doi.org/10.1038/s41427-024-00577-1
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