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REVIEW 5 major objections 5 minor 39 references

Microstructural Studies Using Generative Adversarial Network (GAN): a Case Study

T0 review · 5 major / 5 minor · reviewed 2026-08-07 · deepseek-v4-flash

Pith's one-line read A GAN trained on phase-field spinodal microstructures generates synthetic images whose finite-element mechanical response matches the original simulations.

desk verdict Plausible GAN-for-microstructure pipeline, but the FEM 'excellent agreement' rests on a single matched pair and the coarsening 'validation' is built into the sorting procedure. read the letter →

arxiv 2506.05860 v1 pith:CXCLJ4DX submitted 2025-06-06 cond-mat.mtrl-sci

classification cond-mat.mtrl-sci
keywords generativeadversarialnetworkspinodaldecompositionphase-fieldmicrostructuregenerationfiniteelementmethodcoarseningsyntheticmicrostructureselastoplasticproperties
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

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

The reading

The paper claims that a generative adversarial network, trained only on images of spinodal decomposition produced by phase-field simulation, can generate synthetic microstructures that are physically and mechanically faithful to the real simulations. The authors support this by showing that the generated microstructures obey the theoretical coarsening law $r \propto t^{1/3}$, and that finite-element simulations of their elastoplastic response give true stress–plastic strain curves in excellent agreement with curves from actual phase-field microstructures. The practical gain is speed: on the same machine, 20000 microstructures take about 1800 seconds from phase-field simulation but about 40 seconds from the trained GAN. This makes the GAN a cheap database generator for FEM-based property prediction and any application needing many realistic synthetic images.

What carries the argument

The load-bearing object is a Wasserstein GAN, a GAN variant trained with the Earth-Mover distance for stability, whose generator upsamples random noise through transposed convolutions to 256×256 grayscale images and is trained on roughly 10,000 phase-field microstructures from the Cahn-Hilliard equation for a binary alloy undergoing spinodal decomposition. The argument then leans on a post-hoc labeling scheme: average pixel value maps an image to a composition, and sorting a composition's images by average particle size reconstructs a time axis. Validation uses the coarsening law $r^3 \propto t$, the two-point correlation function $S_2(r)$, and a finite-element pipeline—OOF2 image meshing followed by an Abaqus elastoplastic solve with periodic boundary conditions—that turns morphology into true stress–plastic strain curves.

What would settle it

Draw many GAN and phase-field images at a fixed composition without particle-count matching, compute the FEM stress–strain curves for each, and compare the distributions: if the phase-field curves fall outside the GAN spread, the reported agreement was selection, not generation. As a second check, shuffle the time labels during training and re-run the coarsening analysis: if the sorted $r^3$ versus $t$ plot stays linear, the coarsening law is an artifact of sorting by particle size.

Watch

Extended reading notes

Core claim

The central claim is that the GAN is capable of producing synthetic microstructures which obey the theoretically predicted coarsening rate and whose mechanical properties, computed by the finite element method, show excellent agreement with phase-field-generated microstructures. Composition of a generated image is read from its average pixel value, and time is reconstructed by sorting the images of a given composition by average particle size; under that ordering the cube of the average radius grows linearly in time for both the 5,000- and 10,000-image training sets. For compositions 0.28, 0.30, and 0.32, true stress–plastic strain curves from GAN and phase-field microstructures with similar particle counts are reported to be in excellent agreement and within the rule-of-mixtures bounds. The paper also reports Fréchet Inception Distance values between 59 and 75, taken as evidence that the model has learned the distribution rather than memorizing training images, and sequential correlation above 0.9 in the generated sequence.

Load-bearing premise

The FEM validation matches one GAN image to one phase-field image per composition using only particle count, so the claimed excellent agreement assumes that a single favorable pair represents the whole output distribution of each model.

Editorial extensions

If this is right

  • Trained GAN models can replace phase-field simulation as the source of large microstructure datasets for FEM-based property prediction, reducing generation time by a factor of roughly 45 in the reported case.
  • Property calculations could sample thousands of microstructures instead of a handful, yielding distributions of mechanical response rather than single curves.
  • The workflow should transfer to other microstructure classes, such as precipitate growth, grain growth, or solidification, wherever phase-field training images can be produced.
  • Because the GAN generates from noise, it removes the RNN/LSTM requirement of seeding each prediction with a phase-field image.
  • The agreement between GAN and phase-field FEM curves implies that the morphology statistics relevant to elastoplastic response are captured in the synthetic database.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • Inference: The sorting-by-particle-size step is what turns an unordered GAN into a time series, but it also means the GAN has no direct time control; conditioning the generator explicitly on composition and time would remove the need for post-hoc sorting.
  • Inference: The FEM comparison matches a single GAN image to a single phase-field image per composition; a stronger test would compute the spread of stress–strain curves over many random GAN samples and check whether the phase-field curve falls inside that distribution.
  • Inference: The moderate FID scores suggest the generated images are not pixel-identical to phase-field ones, so properties highly sensitive to fine morphological details, such as percolation or local stress concentrations, may not match as well as the area-averaged response shown here.
  • Inference: A natural extension is to apply the same validation machinery to other generative models, such as diffusion models, on the same phase-field dataset to quantify the trade-off between GAN speed and any mode-coverage advantages.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

5 major / 5 minor

Summary. The paper trains a Wasserstein GAN on 2D phase-field simulations of spinodal decomposition in a binary A-B alloy, generates synthetic microstructure images, and then reports three types of validation: (i) generated images follow the theoretical LSW coarsening law r^3 ~ t, (ii) consecutive generated images have high sequential correlation, and (iii) finite-element elastoplastic stress-strain curves computed on GAN-generated microstructures agree excellently with those computed on phase-field microstructures. The claimed payoff is an orders-of-magnitude cheaper source of microstructures for FEM property prediction.

Significance. If the central claims were established, the paper would deliver a practically useful demonstration that generative models can supply large numbers of realistic spinodal microstructures for downstream mechanical-property calculations, and the comparative timing estimate (40 s for 20,000 images versus 1,800 s for phase-field) is attractive. The paper also openly discusses limitations such as lack of explicit physical constraints and limited extrapolation outside training composition/time ranges. However, the current evidence does not establish the claims at the level claimed: the coarsening and sequential-correlation evidence is produced after sorting generated images by particle size, and the FEM agreement rests on a single hand-matched image pair per composition. The authors are to be credited for attempting a downstream-task validation rather than reporting only image-quality metrics, but the validation design currently precludes a distribution-level statement.

major comments (5)
  1. [Section 3, Figure 6(b)] The coarsening-law validation is circular. The generated images are sorted in ascending order by average particle size, and the sorted rank is then used as time; measuring the cube of the average radius against this constructed time guarantees an increasing trend and cannot test the physical r proportional to t^(1/3) law against the phase-field data. To validate coarsening, the GAN should be conditioned on an explicit time label (or trained on separate time slices), and generated images at each labeled time should be compared with phase-field images of the same time.
  2. [Section 3, Figure 6(c)] The sequential-correlation analysis is also a consequence of the sorting procedure: consecutive images in a list sorted by particle size are similar by construction, so a high Pearson correlation (>0.9) does not indicate that the generator produces temporally consistent sequences. The GAN is trained on shuffled images without time labels, and there is no temporal-conditioning mechanism that could produce a time-ordered sequence; the order is imposed after generation.
  3. [Section 3, Figure 7] The FEM comparison rests on exactly one GAN-generated image and one phase-field image per composition, matched to have a similar number of particles, and the paper reports no error bars, replicate curves, or statistical test for the flow stress. This does not establish agreement for the generator's output distribution, especially given the reported FID scores of 59.75-73.88, which indicate a nontrivial distributional gap. The authors should compare multiple random draws from each generator (or use a distributional metric over the FEM responses) and report the mean and variance of the stress-strain response.
  4. [Section 2.3 and Table 1] The architecture description is internally inconsistent: the text says the model implements a Wasserstein GAN with the Wasserstein loss in Eq. (5), but Table 1 lists Binary Cross-Entropy as the loss function, and the Lipschitz-constraint implementation (gradient clipping or gradient penalty) is not specified. Please reconcile the loss description and provide the missing training details, such as the clipping parameter or gradient-penalty coefficient and the number of critic updates per generator update.
  5. [Section 3, Figure 5 and composition assignment] The composition of generated images is inferred from the average pixel value, but no calibration or uncertainty analysis is provided for this mapping. Since the phase-field images have known composition from the simulation setting, the paper can easily demonstrate the accuracy of the average-pixel-value proxy on the training data; without this, the grouping into composition bins and the subsequent FEM comparison are built on an unvalidated assumption.
minor comments (5)
  1. [Abstract vs. Section 5] The abstract says 'excellent agreement' for the FEM comparison while Section 5 says 'good match'; please use consistent wording.
  2. [Section 2.4] The phrase 'plain strain' appears twice and should be 'plane strain'.
  3. [Section 6, Data availability] The data availability statement says 'available in this link' and 'available in this link' without actual URLs or repository identifiers, making the reproducibility claim unverifiable; please provide concrete links.
  4. [Section 2.4, Eq. (6)-(7)] The notation in the constraint equations is not fully defined: the coefficients A_m, A_n, etc., and how the sums expand to the periodic-boundary conditions are left implicit; a short explanation would help readability.
  5. [References [29]-[31]] References [29]-[31] are only loosely connected to the microstructure-generation topic and are not cited in any of the validation arguments; consider removing or integrating them more substantively.

Circularity Check

2 steps flagged · score 6.0 of 10

Coarsening-rate and sequential-correlation claims are largely constructed by the paper's own sorting procedure, while the FEM agreement rests on selected single-image comparisons.

  1. self definitional [Section 3, Figure 6(b) and surrounding text]
    "Next, we methodically sort the microstructures in ascending order for a given composition based on the average particle size. ... Figure 6(b) depicts the cube of the average radius as a function of time. ... Clearly, GAN is capable of producing synthetic microstructures, which obey the theoretically predicted coarsening rate."

    The 'time' axis for the GAN-generated microstructures is not produced by the model; it is assigned as the rank after sorting images by average particle size. Measuring the cube of the average radius against this constructed time therefore guarantees a monotonic increase in r with the assigned t. The reported r^3 vs t trend is an artifact of the sorting step, not independent evidence that the GAN learned the coarsening law. Any set of generated images with a spread of particle sizes would show an increasing r^3 curve after sorting, so the validation reduces to the sorting procedure by construction.

  2. self definitional [Section 3, Figure 6(c) and surrounding text]
    "Next, we methodically sort the microstructures in ascending order for a given composition based on the average particle size. ... Interestingly, synthetic microstructures generated by GAN also have reasonably high sequential correlation (>0.9). This finding is pivotal as it confirms the model’s reliability in producing sequentially dependent microstructures, which is essential for temporal evolution studies."

    The 'consecutive pairs' used to compute the Pearson sequential correlation are consecutive in the sorted-by-average-particle-size order. Sorting by particle size forces neighboring images to have similar particle sizes and hence similar two-point statistics, inflating the pixel-level correlation coefficient. The high sequential correlation is therefore a property of the ordering imposed by the authors, not a property of temporal dynamics learned by the GAN. The claim that the GAN produces sequentially dependent microstructures reduces to the sorting step by construction.

full rationale

The strongest load-bearing claims of temporal physical validity are circular: chronological order for GAN-generated microstructures is defined by sorting them by average particle size, and the same sorted sequence is then used to demonstrate both the r proportional to t^(1/3) coarsening law and high sequential correlation. These validations are largely constructed by the sorting procedure, so the score is elevated. The FEM property comparison is not circular in the same way, but it is statistically weak: for each composition one GAN image and one phase-field image with a similar number of particles are selected, and the reported FID scores (59.75-73.88) indicate nontrivial distributional mismatch, so 'excellent agreement' for the generator's full output distribution is not established. No load-bearing self-citation chain was found, and the image-generation, FID, and FEM pipeline retain independent content, which prevents a higher score.

Assumptions & free parameters 3 free parameters · 5 assumptions · 0 invented entities

The central physical-fidelity claims rest mainly on the assumption that GAN output can be labeled by composition and time after the fact, and on the phase-field model that generated the training set. No new entities are postulated. The FEM property comparison is more independent but is under-sampled.

free parameters (3)
  • Training set selection (set 4 with maximum standard deviation) = set 4, std 0.3155
    The authors chose one of four random 5000-image splits because it had the largest standard deviation, a hand decision that can affect the diversity and quality of generated microstructures.
  • GAN hyperparameters = learning rate 2e-4, batch size 32
    Standard values are used without an optimization study; they control the reported image quality and the convergence claims.
  • Composition and time assignment for generated images = average pixel value for composition, particle-size ordering for time
    Generated images are grouped by average pixel value and sorted by average particle size to stand in for composition and chronological time; the temporal-evolution tests depend on this hand-applied mapping.
assumptions (5)
  • domain assumption Cahn-Hilliard equation with double-well free energy (Eqs. 1-3) generates physically valid spinodal microstructures.
    The training data set is produced solely by this model, so the GAN can only learn patterns that this simulation family contains.
  • ad hoc to paper Average pixel value is a valid proxy for composition, and sorting by average particle size reconstructs the true time ordering.
    Used in Section 3 to label and order GAN outputs before physical-fidelity tests; no independent validation of this mapping is given.
  • ad hoc to paper Matching particle count between GAN and phase-field images is sufficient for a fair mechanical-property comparison.
    Figure 7 selects images with a similar number of particles and then compares stress-strain curves; other microstructural statistics are not fully controlled.
  • domain assumption Pure iron and pure chromium single-crystal properties from the cited literature are valid inputs for the phase-level elastoplastic FEM model.
    The virtual compression test uses these literature values without re-validation for the two-phase microstructure geometry.
  • domain assumption WGAN convergence can be judged by loss oscillation and visual inspection every 100 epochs.
    No quantitative convergence criterion or formal stopping rule is provided, so training stability and mode-collapse avoidance are asserted rather than measured.

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Cite this review

Pith. "Pith review of Microstructural Studies Using Generative Adversarial Network (GAN): a Case Study." pith.science (2026). https://pith.science/paper/CXCLJ4DX

@misc{pith2026250605860,
  author       = {Pith},
  title        = {Pith review of: Microstructural Studies Using Generative Adversarial Network (GAN): a Case Study},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/CXCLJ4DX}},
  note         = {Machine review of arXiv:2506.05860}
}
read the original abstract

The generative adversarial network (GAN) is one of the most widely used deep generative models for synthesizing high-quality images with the same statistics as the training set. Finite element method (FEM) based property prediction often relies on synthetically generated microstructures. The phase-field model is a computational method of generating realistic microstructures considering the underlying thermodynamics and kinetics of the material. Due to the expensive nature of the simulations, it is not always feasible to use phase-field for synthetic microstructure generation. In this work, we train a GAN with microstructures generated from the phase-field simulations. Mechanical properties calculated using the finite element method on synthetic and actual phase field microstructures show excellent agreement. Since the GAN model generates thousands of images within seconds, it has the potential to improve the quality of synthetic microstructures needed for FEM calculations or any other applications requiring a large number of realistic synthetic images at minimal computational cost.

Figures

Figures reproduced from arXiv: 2506.05860 by the authors.

Figure 1
Figure 1. Schematic diagram of accelerated microstructure-property correlation: training data generation, GAN model training, synthetic microstructure prediction, [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Microstructures for different phase fractions captured during the spinodal decomposition. Time evolution is simulated by the phase-field method. microstructures. The ability of GAN to generate diverse and re￾alistic microstructures can significantly accelerate material dis￾covery and development. Recent advancements in deep learning have led to the de￾velopment of sophisticated architectures that go beyond con￾venti… view at source ↗
Figure 3
Figure 3. Schematic representation of a Generative Adversarial Network (GAN). The diagram illustrates the adversarial training process where the generator [PITH_FULL_IMAGE:figures/full_fig_p004_3.png] view at source ↗
Figures from the paper (4 more)
Figure 4
Figure 4. Figure 4: Methodology for computing elastoplastic behavior: (a) Meshed microstructure from OOF2, (b) Categorization of nodes on the imported microstructure in [PITH_FULL_IMAGE:figures/full_fig_p006_4.png]
Figure 5
Figure 5. Figure 5: Frequency distribution of different compositions among the GAN￾predicted images. In the above equations, A is the area of the microstructure; σi j,ϵi j are the area-averaged values of stress and strain, respec￾tively; nel is the total number of finite elements of the m…
Figure 6
Figure 6. Figure 6: (a) Synthetic microstructures generated with GAN, using noise as input for initial composition [PITH_FULL_IMAGE:figures/full_fig_p007_6.png]
Figure 7
Figure 7. Figure 7: Top row: Phase-field and GAN-predicted microstructures having di [PITH_FULL_IMAGE:figures/full_fig_p008_7.png]

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Reference graph

Works this paper leans on

39 extracted references · 39 canonical work pages

  1. [1]

    Roters, P

    F. Roters, P. Eisenlohr, L. Hantcherli, D.D. Tjahjanto, T.R. Bieler, and D. Raabe. Overview of constitutive laws, kine- matics, homogenization and multiscale methods in crystal plasticity finite-element modeling: Theory, experiments, applications.Acta Materialia, 58(4):1152–1211, 2010

  2. [2]

    Dassault Systémes Simulia Corp, United States, 2009

    Michael Smith.ABAQUS/Standard User’s Manual, Ver- sion 6.9. Dassault Systémes Simulia Corp, United States, 2009

  3. [3]

    Langer, E.R

    S.A. Langer, E.R. Fuller, and W.C. Carter. Oof: an image- based finite-element analysis of material microstructures. Computing in Science&Engineering, 3(3):15–23, 2001

  4. [4]

    Fromm, Kunok Chang, David L

    Bradley S. Fromm, Kunok Chang, David L. McDow- ell, Long-Qing Chen, and Hamid Garmestani. Link- ing phase-field and finite-element modeling for pro- cess–structure–property relations of a ni-base superalloy. Acta Materialia, 60(17):5984–5999, 2012

  5. [5]

    Albert Linda, Ankit Singh Negi, Vishal Panwar, Rupesh Chafle, Somnath Bhowmick, Kaushik Das, and Rajdip Mukherjee.µ2mech: A software package combining mi- crostructure modeling and mechanical property predic- tion.Physica Scripta, 99(5):055256, apr 2024

  6. [6]

    Wenqi Liu, Junhe Lian, Nikolaos Aravas, and Sebastian Münstermann. A strategy for synthetic microstructure generation and crystal plasticity parameter calibration of fine-grain-structured dual-phase steel.International Jour- nal of Plasticity, 126:102614, 2020

  7. [7]

    Groeber and Michael A

    Michael A. Groeber and Michael A. Jackson. Dream.3d: A digital representation environment for the analysis of microstructure in 3d.Integrating Materials and Manufac- turing Innovation, 3:56–72, 2014

  8. [8]

    Mukherjee, T.A

    R. Mukherjee, T.A. Abinandanan, and M.P. Gurura- jan. Phase field study of precipitate growth: Effect of misfit strain and interface curvature.Acta Materialia, 57(13):3947–3954, 2009

Show all 39 references
  1. [9]

    Mukherjee, T.A

    R. Mukherjee, T.A. Abinandanan, and M.P. Gururajan. Precipitate growth with composition-dependent diffusiv- ity: Comparison between theory and phase field simula- tions.Scripta Materialia, 62(2):85–88, 2010

  2. [10]

    Gururajan and T.A

    M.P. Gururajan and T.A. Abinandanan. Phase field study of precipitate rafting under a uniaxial stress.Acta Materi- alia, 55(15):5015–5026, 2007. 10

  3. [11]

    Effect of strong nonuniformity in grain bound- ary energy on 3-D grain growth behavior: A phase- field simulation study.Computational Materials Science, 127:67–77, 2017

    Kunok Chang, Long-Qing Chen, Carl E Krill, and Nele Moelans. Effect of strong nonuniformity in grain bound- ary energy on 3-D grain growth behavior: A phase- field simulation study.Computational Materials Science, 127:67–77, 2017

  4. [12]

    Verma and R

    M. Verma and R. Mukherjee. Grain growth stagnation in solid state thin films: A phase-field study.Journal of Applied Physics, 130(2):025305, 2021

  5. [13]

    C. E. Krill, L. Helfen, D. Michels, H. Natter, A. Fitch, O. Masson, and R. Birringer. Size-dependent grain- growth kinetics observed in nanocrystalline fe.Phys. Rev. Lett., 86:842–845, Jan 2001

  6. [14]

    David Molnar, Rajdip Mukherjee, Abhik Choudhury, Alejandro Mora, Peter Binkele, Michael Selzer, Britta Nestler, and Siegfried Schmauder. Multiscale simulations on the coarsening of cu-rich precipitates inα-fe using ki- netic monte carlo, molecular dynamics and phase-field simu...

  7. [15]

    Phase-field simulation for the evolu- tion of solid/liquid interface front in directional solidifica- tion process.Journal of Materials Science&Technology, 35(6):1044–1052, 2019

    Yuhong Zhao, Bing Zhang, Hua Hou, Weipeng Chen, and Meng Wang. Phase-field simulation for the evolu- tion of solid/liquid interface front in directional solidifica- tion process.Journal of Materials Science&Technology, 35(6):1044–1052, 2019

  8. [16]

    Subhradeep Chatterjee, TA Abinandanan, and Kamanio Chattopadhyay. Phase-field simulation of fusion interface events during solidification of dissimilar welds: effect of composition inhomogeneity.Metallurgical and Materials Transactions A, 39:1638–1646, 2008

  9. [17]

    Effect of co-existing external fields on a binary spin- odal system: A phase-field study.Journal of Physics and Chemistry of Solids, 132:236–243, 2019

    Rupesh Chafle, Somnath Bhowmick, and Rajdip Mukher- jee. Effect of co-existing external fields on a binary spin- odal system: A phase-field study.Journal of Physics and Chemistry of Solids, 132:236–243, 2019

  10. [18]

    Mushongera, and Kumar Ankit

    Rahul Raghavan, William Farmer, Leslie T. Mushongera, and Kumar Ankit. Multiphysics approaches for modeling nanostructural evolution during physical vapor deposition of phase-separating alloy films.Computational Materials Science, 199:110724, 2021

  11. [19]

    Parallel computing for phase-field models.The International journal of high performance computing applications, 28(1):61–72, 2014

    Alexander V ondrous, Michael Selzer, Johannes Hötzer, and Britta Nestler. Parallel computing for phase-field models.The International journal of high performance computing applications, 28(1):61–72, 2014

  12. [20]

    Murdock, Steven K

    Anthony Yu-Tung Wang, Ryan J. Murdock, Steven K. Kauwe, Anton O. Oliynyk, Aleksander Gurlo, Jakoah Br- goch, Kristin A. Persson, and Taylor D. Sparks. Ma- chine learning for materials scientists: An introductory guide toward best practices.Chemistry of Materials, 32(12):4954–4...

  13. [21]

    Physics-embedded graph network for accelerating phase- field simulation of microstructure evolution in additive manufacturing.npj Computational Materials, 8(1):201, 2022

    Tianju Xue, Zhengtao Gan, Shuheng Liao, and Jian Cao. Physics-embedded graph network for accelerating phase- field simulation of microstructure evolution in additive manufacturing.npj Computational Materials, 8(1):201, 2022

  14. [22]

    Learn- ing two-phase microstructure evolution using neural op- erators and autoencoder architectures.npj Computational Materials, 8(1):190, 2022

    Vivek Oommen, Khemraj Shukla, Somdatta Goswami, Rémi Dingreville, and George Em Karniadakis. Learn- ing two-phase microstructure evolution using neural op- erators and autoencoder architectures.npj Computational Materials, 8(1):190, 2022

  15. [23]

    Peichen Wu, Ashif Sikandar Iquebal, and Kumar Ankit. Emulating microstructural evolution during spinodal de- composition using a tensor decomposed convolutional and recurrent neural network.Computational Materials Sci- ence, 224:112187, 2023

  16. [24]

    C Hu, S Martin, and R Dingreville. Accelerating phase- field predictions via recurrent neural networks learn- ing the microstructure evolution in latent space.Com- puter Methods in Applied Mechanics and Engineering, 397:115128, 2022

  17. [25]

    Accelerating phase-field-based mi- crostructure evolution predictions via surrogate models trained by machine learning methods.npj Computational Materials, 7(1):1–11, 2021

    David Montes de Oca Zapiain, James A Stewart, and Rémi Dingreville. Accelerating phase-field-based mi- crostructure evolution predictions via surrogate models trained by machine learning methods.npj Computational Materials, 7(1):1–11, 2021

  18. [26]

    Time series forecasting of multiphase microstructure evo- lution using deep learning.Computational Materials Sci- ence, 247:113518, 2025

    Saurabh Tiwari, Prathamesh Satpute, and Supriyo Ghosh. Time series forecasting of multiphase microstructure evo- lution using deep learning.Computational Materials Sci- ence, 247:113518, 2025

  19. [27]

    Accelerating microstructure mod- eling via machine learning: A method combining autoen- coder and convlstm.Phys

    Owais Ahmad, Naveen Kumar, Rajdip Mukherjee, and Somnath Bhowmick. Accelerating microstructure mod- eling via machine learning: A method combining autoen- coder and convlstm.Phys. Rev. Mater., 7:083802, Aug 2023

  20. [28]

    Integrated phase field and ma- chine learning study of microstructure evolution during interface-controlled spinodal decomposition.Solid State Phenomena, 357:101–106, 6 2024

    Owais Ahmad, Rakesh Maurya, Rajdip Mukherjee, and Somnath Bhowmick. Integrated phase field and ma- chine learning study of microstructure evolution during interface-controlled spinodal decomposition.Solid State Phenomena, 357:101–106, 6 2024

  21. [29]

    Generative artificial intelligence: Analyzing its future applications in additive manufacturing.Big Data and Cognitive Computing, 8(7), 2024

    Erik Westphal and Hermann Seitz. Generative artificial intelligence: Analyzing its future applications in additive manufacturing.Big Data and Cognitive Computing, 8(7), 2024

  22. [30]

    Generative artificial intelligence and its applications in materials science: Current situation and future perspectives.Journal of Materiomics, 9(4):798– 816, 2023

    Yue Liu, Zhengwei Yang, Zhenyao Yu, Zitu Liu, Dahui Liu, Hailong Lin, Mingqing Li, Shuchang Ma, Maxim Avdeev, and Siqi Shi. Generative artificial intelligence and its applications in materials science: Current situation and future perspectives.Journal of Materiomics, 9(4):798–...

  23. [31]

    M Vinodhini and Sujatha Rajkumar. A deep learning ap- proach for predicting and optimizing the v2x network pa- rameters for sustainable smart transportation systems.En- gineering Research Express, 7(1):015268, feb 2025. 11

  24. [32]

    Free Energy of a Nonuniform System

    John W Cahn and John E Hilliard. Free Energy of a Nonuniform System. I. Interfacial Free Energy.The Jour- nal of Chemical Physics, 28(2):258–267, 1958

  25. [33]

    On spinodal decomposition.Acta metal- lurgica, 9(9):795–801, 1961

    John W Cahn. On spinodal decomposition.Acta metal- lurgica, 9(9):795–801, 1961

  26. [34]

    Generative adversarial networks-based syn- thetic microstructures for data-driven materials design

    Ryuichi Narikawa, Yoshihito Fukatsu, Zhi-Lei Wang, Toshio Ogawa, Yoshitaka Adachi, Yuji Tanaka, and Shin Ishikawa. Generative adversarial networks-based syn- thetic microstructures for data-driven materials design. Advanced Theory and Simulations, 5(5):2100470, 2022

  27. [35]

    Alexander Henkes and Henning Wessels. Three- dimensional microstructure generation using generative adversarial neural networks in the context of continuum micromechanics.Computer Methods in Applied Mechan- ics and Engineering, 400:115497, 2022

  28. [36]

    Predic- tive microstructure image generation using denoising dif- fusion probabilistic models.Acta Materialia, 261:119406, 2023

    Erfan Azqadan, Hamid Jahed, and Arash Arami. Predic- tive microstructure image generation using denoising dif- fusion probabilistic models.Acta Materialia, 261:119406, 2023

  29. [37]

    Fritz, D

    R. Fritz, D. Wimler, A. Leitner, V . Maier-Kiener, and D. Kiener. Dominating deformation mechanisms in ultrafine-grained chromium across length scales and tem- peratures.Acta Materialia, 140:176 – 187, 2017

  30. [38]

    Plane strain compression test and simple shear test of sin- gle crystal pure iron.Procedia Engineering, 81:1342– 1347, 2014

    Shintaro Yabe, Motoki Terano, and Masahiko Yoshino. Plane strain compression test and simple shear test of sin- gle crystal pure iron.Procedia Engineering, 81:1342– 1347, 2014. 11th International Conference on Technology of Plasticity, ICTP 2014, 19-24 October 2014, Nagoya Con...

  31. [39]

    Hertzberg, R.P

    R.W. Hertzberg, R.P. Vinci, and J.L. Hertzberg.Deforma- tion and Fracture Mechanics of Engineering Materials. Wiley, 2012. 12

Pith tools

Reviewed August 7, 2026 · model on record in the stance chip above.