REVIEW 6 major objections 4 minor 36 references
Crystal models get a new layer: coordination polyhedra as learnable graph nodes, cutting band-gap error to 0.292 eV on Materials Project data.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · deepseek-v4-flash
2026-08-01 22:17 UTC pith:NDK363YY
load-bearing objection The polyhedral-graph idea is worth a second look, but the paper's central mechanistic claim is untested: no ablations, single-seed results, and a contaminated band-gap target leave the 0.012 eV gain over ALIGNN unexplained. the 6 major comments →
Dual-Level Atomic and Coordination Geometry Learning for Crystal Property Prediction Using Graph Neural Networks
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
CPGN constructs a coordination polyhedron graph alongside the usual atom and line graphs. Each Voronoi-derived coordination shell becomes a node described by seven geometric descriptors (coordination number, bond-length distortion, angle variance, volume proxy, mean bond length, electronegativity mismatch, and coordination type), and edges between polyhedra encode whether they share a corner, edge, or face. The three graphs are updated in interleaved layers with bidirectional cross-attention between atom and polyhedron embeddings. The paper reports a formation-energy MAE of 0.060 eV/atom and the best band-gap MAE of 0.292 eV on the Materials Project, with competitive or better results on JAR
What carries the argument
The coordination polyhedron graph G_P: a coarse-grained graph where nodes are Voronoi tessellation shells (using Pymatgen's VoronoiNN within an 8 Å cutoff) and edges carry a scalar connectivity type — 0.0 for corner-sharing, 0.5 for edge-sharing, 1.0 for face-sharing. This graph injects explicitly encoded local geometry (distortion, angle variance, volume proxy, electronegativity mismatch) and inter-polyhedral topology into the learned representation, which the paper argues is what standard atom-only message passing must rediscover implicitly.
Load-bearing premise
The paper assumes that the Voronoi shells within an 8 Å cutoff are chemically meaningful coordination polyhedra, even though the mean coordination number at that cutoff (14.2) is well above typical chemical coordination numbers.
What would settle it
A reader could run the published CPGN code on the same Materials Project split but with a stricter Voronoi cutoff (e.g., 5 Å or a low-weight Voronoi factor) and compare band-gap MAE. If the polyhedral graph at a physically accurate coordination shell performs no better than the atom+line graph alone, the paper's central claim — that explicit polyhedral geometry drives the gain — is falsified.
If this is right
- If CPGN's band-gap result holds, explicit polyhedral geometry becomes a validated alternative to deeper or higher-order message passing for geometry-sensitive electronic properties.
- The three-graph architecture offers a template for injecting crystallographic prior knowledge into GNNs without abandoning atomic resolution.
- The reported stability classifier (accuracy 0.988, F1 0.993) shows that sharing a single latent fingerprint across regression and classification heads can preserve physical consistency.
- The parameter count (~4.85M on Materials Project) stays comparable to ALIGNN while adding a third graph stream, suggesting the polyhedral prior is relatively cheap to add.
- On QM9, the model's HOMO/LUMO results indicate the same polyhedral machinery transfers to molecular orbital prediction, though with less gain over baselines than on crystalline band gaps.
Where Pith is reading between the lines
- A natural testable extension is to ablate each of the seven polyhedron descriptors and each sharing-type edge weight, to see which geometric features actually drive the band-gap improvement — the paper does not report such ablations.
- The 8 Å cutoff that yields a mean of 14.2 neighbours per atom may be too generous to represent true coordination polyhedra (typically 4–9 neighbours), so part of the reported gain could come from added model capacity rather than from chemically accurate polyhedra; a stricter cutoff or a learnable neighbor selection would settle this.
- Because the polyhedron graph is built on Voronoi shells, its benefit likely depends on the quality of the input relaxed structures; applying CPGN to unrelaxed or disordered structures, which the paper lists as future work, would reveal how brittle the geometric prior is.
- The cross-attention module is the largest parameter component (32.6%), so the paper's claim that gains come from polyhedral geometry rather than attention capacity could be probed by replacing cross-attention with a simple concatenation baseline.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes the Coordination Polyhedron Graph Network (CPGN), a multi-scale GNN that augments an atom graph and a line graph with a third graph whose nodes are Voronoi-derived coordination polyhedra and whose edges encode corner/edge/face sharing. The model alternates message passing on the three graphs, couples atom and polyhedron streams with scalar-gated cross-attention, and uses a shared latent vector for formation energy, band gap, and stability prediction. Results are reported on Materials Project 2018.6.1, JARVIS-DFT, and QM9; the headline numbers are a formation-energy MAE of 0.060 eV/atom and a band-gap MAE of 0.292 eV on Materials Project, with the band-gap result claimed as state of the art among the compared methods.
Significance. If the reported gains were robustly attributable to the polyhedron stream, CPGN would provide a useful inductive bias for geometry-sensitive crystal properties, and the paper's public code and detailed graph statistics would be a helpful resource. However, the central causal claim—that coordination-polyhedron geometry improves accuracy—is not currently isolated by controlled experiments. The architecture contribution is clearly described, but the evidence would need ablation studies, multi-seed uncertainty quantification, and clarification of the label-proxy issues before the claim can be accepted.
major comments (6)
- [§3 Steps 2–5; Tables 3, 7, 8, 13] The central claim that 'explicitly incorporating coordination polyhedra significantly enhances crystal representation learning' is not tested by ablation. The only comparisons are between the complete CPGN and independently trained or published baselines, which differ in parameter count (Table 10: CPGN 4.85M vs ALIGNN 4.03M), training protocol, and in Table 13 include numbers the authors state they could not reproduce. No experiment removes G_P, the 7-D descriptors, or the cross-attention while holding the backbone, capacity, and training protocol fixed. The observed differences (e.g., 0.012 eV on band gap) could therefore be due to model capacity or optimization rather than the polyhedral inductive bias. A parameter-matched ablation with the polyhedron stream disabled is necessary. The architecture description is also internally inconsistent: §4 (end of Step 4) says total trainable para
- [§4.1–4.3; all result tables] Every experiment uses a single random seed (SEED=42) and no standard deviations or seed ranges are reported. Since several headline improvements are small (band gap 0.292 vs ALIGNN 0.304; QM9 HOMO-LUMO gap 0.038 equal to ALIGNN; Materials Project formation energy tied with SchNet at 0.060), the reported ranking is not statistically supported. Multi-seed results with mean ± std should be provided for the main tables.
- [§3 Step 7; Table 3] The band-gap target includes the proxy max(0,−0.8E_f) for materials whose DFT band gap is unavailable. The fraction of test labels that are proxy values is not reported, and the proxy is a deterministic function of the formation-energy label used in the same multi-task objective (Eq. 10). For those samples the 'band-gap' prediction is effectively a recalibrated formation energy, so the 0.292 eV band-gap MAE may partly reflect learning of E_f rather than electronic structure. The authors should report the proxy fraction in train/test, give separate MAEs for true DFT gaps and proxy labels, and re-run the comparison with only true band-gap labels.
- [§4.3; Tables 3–4] The text reports validation MAE=0.0645 and test MAE=0.0666 eV/atom for formation energy, while the abstract, Table 3, and conclusions state 0.060 eV/atom. Similarly, §4.3 refers to 'CGCNN (23.85)' as a MAD:MAE ratio, whereas Table 4 lists CGCNN=11.7 and 23.85 is SSFormer's value in Table 13. These discrepancies concern the paper's central quantitative claims and must be resolved, with a clear statement of which split and checkpoint produce each reported number.
- [§3 Step 2; §5.2] The VoronoiNN shells at r_cut=8 Å yield a mean of 14.2 neighbors per atom, well above typical chemical coordination numbers, yet the descriptors normalize by 12 and cap CN at min(CN,12)/12. As written, the 'coordination polyhedra' may be effectively inflated Voronoi shells rather than chemically recognized coordination polyhedra. The authors should validate the construction (e.g., distribution of polyhedron node counts, comparison with known coordination numbers in reference structures, sensitivity to r_cut) to support the claim that the descriptors and sharing-type edges are physically interpretable.
- [§4.3.1; Tables 5–6] The stability label is 'obtained directly from the stability field... or approximated as 1 if E_f < 0, and 0 otherwise.' Since formation energy is the primary training target of the shared backbone, a stability classifier built on that backbone can achieve high accuracy by thresholding E_f. The reported accuracy/F1 (Table 5) and the comparison in Table 6 are therefore not a meaningful test of the polyhedral representation for stability, and the approximation should at least be reported and analyzed separately.
minor comments (4)
- [Figures and tables] Figure numbering is inconsistent: Figure 11 is used both for stability confusion matrices in §4.3.1 and for QM9 inference-time plots in §5.3. There is a floating 'Table??' reference near Table 6, and the Figure 2 caption contains a typo ('formaework').
- [§4.3 vs §4.5] The evaluation protocol for baselines is stated inconsistently: §4.3 says CGCNN, MEGNet, SchNet, and ALIGNN were reproduced, while §4.5 says QM9 baseline results were taken directly from the original papers. The authors should state, for each dataset, which baselines were rerun and under what split and hyperparameters.
- [§4.1 and §4.4] The MP split is described as a random shuffle with seed 42 (60,000/5,000/4,239), while some public benchmark comparisons use the standard MP split. If the published baseline numbers in Table 13 were obtained on a different split, the comparison is not controlled. Please state explicitly whether the same split was used for all baseline metrics.
- [§5.3; Table 12] The baseline inference times are 'estimated from published scaling characteristics' and are therefore only qualitative. The speed comparison should be labeled as approximate, or the baselines should be measured on the same hardware and code.
Circularity Check
Partial circularity: band-gap and stability evaluation targets are definitionally tied to the co-trained formation-energy target via proxies, so two reported prediction metrics partly reduce to formation-energy regression; the network/graph derivation and formation-energy benchmark are not circular.
specific steps
-
self definitional
[Section 3, Step 7 (Training), after Eq. (10); reported in Abstract and Tables 3/4]
"The band-gap target is taken directly from the DFT-computed value in the dataset where available, with a proxy of max(0,−0.8E f ) applied only in its absence."
For every entry lacking a DFT band gap, the target is the deterministic function max(0,−0.8E_f). Since E_f is the primary co-trained target (Eq. 10: L = MAE_Ef + 0.1·MAE_Eg), the band-gap head on those entries is scored against a rescaling of the formation-energy target. The advertised 'state-of-the-art' band-gap MAE of 0.292 eV is therefore partly a re-statement of formation-energy accuracy rather than independent evidence that coordination-polyhedron geometry improves band-gap prediction. The affected fraction is undisclosed, so the size of the reduction cannot be assessed from the paper.
-
self definitional
[Section 4.3.1 (Stability Classification), Eqs. (12)-(13) and Table 5]
"The stability label is obtained directly from the stability field in the MP JSON file when available, or approximated as 1 if E f <0, and 0 otherwise. Because the stability prediction shares the same backbone as formation-energy regression ... which is why the classifier achieves aaccuracy of 0.989..."
Where the MP stability field is unavailable, the label is defined as the sign of E_f, while E_f is the primary target of the same shared latent backbone. The stability head can therefore succeed by thresholding the formation-energy prediction; the reported 0.9882 accuracy and 0.9913 ROC-AUC are partly a check on the formation-energy regressor, not independent evidence that the coordination-polyhedron representation encodes thermodynamic stability. The paper's own 'this is why ... 0.989' sentence acknowledges the dependence, yet the number is presented as a CPGN stability result.
full rationale
The core derivation (CIF/POSCAR to atom/line/polyhedron graphs, message passing, cross-attention, and the formation-energy head) is self-contained: the 7-D polyhedron descriptors are computed from structures, not from targets, and no fitted parameter is renamed as a prediction. The formation-energy MAE of 0.060 eV/atom is anchored to the standard MP 2018.6.1 split with reproduced baselines, so the primary benchmark retains independent content. There is no load-bearing self-citation chain. The circularity is confined to the auxiliary prediction targets: for an undisclosed subset, Eg and stability are defined as functions of the co-trained Ef (max(0,−0.8Ef) and 1_{Ef<0}), making the reported band-gap SOTA and stability accuracy partly self-referential re-statements of formation-energy accuracy. Because the band-gap result is one of the paper's two headline findings, this is partial circularity (not full: the graph-construction and formation-energy claims are not reduced to their inputs). Data-quality issues such as the lack of an ablation, single-seed runs, and parameter-count differences are evidentiary weaknesses, not circularity.
Axiom & Free-Parameter Ledger
free parameters (7)
- Voronoi/bond cutoff r_cut =
8.0 Å
- Auxiliary loss weight λ_aux =
0.1
- Polyhedron connectivity weights =
corner 0.0, edge 0.5, face 1.0
- Band-gap proxy coefficients =
max(0, −0.8·E_f)
- Polyhedron descriptor normalizations =
CN/12, angle variance/10000, d̄³/100, d̄/r_cut
- Training seed and hyperparameters =
seed 42, LR 3e-4, weight decay 1e-5, L=4, d_h=256, patience 50
- Stability class weight =
3.0
axioms (6)
- domain assumption VoronoiNN shells within 8 Å equal chemically meaningful coordination polyhedra (Section 3, Step 2).
- ad hoc to paper The seven hand-crafted geometric descriptors capture the physics relevant to formation energy, band gap, and stability (Section 3, Step 2).
- domain assumption DFT labels in MP 2018.6.1, JARVIS-DFT, and QM9 are ground truth for training and evaluation (Section 4).
- domain assumption A random seed-42 split yields i.i.d. validation/test sets with no leakage (Section 4.1).
- domain assumption Line-graph edges between bonds sharing a destination atom capture bond-angle geometry (Section 3, Step 3).
- domain assumption A single training run at seed 42 is representative of model performance (Section 4.1, Table 2).
invented entities (3)
-
Coordination polyhedron graph G_P
no independent evidence
-
Scalar-gated bidirectional cross-attention between atom and polyhedron streams
no independent evidence
-
7-D polyhedron descriptor vector
no independent evidence
read the original abstract
Accurate prediction of crystal properties remains a key challenge in computational materials science. While graph neural networks (GNNs) such as CGCNN, MEGNet, ALIGNN, and SchNet have shown strong performance, they primarily represent crystals at the atomic level and implicitly learn local chemical environments through message passing. However, many material properties are governed by coordination polyhedra, the fundamental structural units formed by atoms and their neighboring atoms. To address this limitation, we propose the Coordination Polyhedron Graph Network (CPGN), a multi-scale GNN that jointly learns atomic, bond, and coordination-polyhedron representations. CPGN constructs three coupled graphs: an atom graph encoding elemental and bonding information, a line graph capturing angular interactions, and a coordination polyhedron graph describing Voronoi-derived local environments through corner-, edge-, and face-sharing relationships. Physically meaningful geometric descriptors are incorporated for each polyhedron, while an interleaved message-passing mechanism with bidirectional cross-attention enables effective information exchange across structural levels. Extensive evaluations on the Materials Project, JARVIS-DFT, and QM9 benchmark datasets demonstrate that CPGN outperforms existing state-of-the-art GNN models. It achieves a formation-energy MAE of 0.060 eV/atom and a band-gap MAE of 0.292 eV on the Materials Project, while providing competitive multi-property prediction on JARVIS-DFT and superior HOMO prediction on QM9. The results highlight that explicit modeling of coordination polyhedra improves crystal representation learning and enables accurate, physically interpretable prediction of material properties.
Figures
Reference graph
Works this paper leans on
-
[1]
Quantifying uncertainty in high- throughput density functional theory: A comparison of aflow, materials project, and oqmd.Physical Review Materials, 7(5):053805, 2023
Vinay I Hegde, Christopher KH Borg, Zachary Del Rosario, Yoolhee Kim, Maxwell Hutchinson, Erin Antono, Julia Ling, Paul Saxe, James E Saal, and Bryce Meredig. Quantifying uncertainty in high- throughput density functional theory: A comparison of aflow, materials project, and oqmd.Physical Review Materials, 7(5):053805, 2023. 21
2023
-
[2]
Recent advances and applications of deep learning methods in materials science.npj Computational Materials, 8(1):59, 2022
Kamal Choudhary, Brian DeCost, Chi Chen, Anubhav Jain, Francesca Tavazza, Ryan Cohn, Cheol Woo Park, Alok Choudhary, Ankit Agrawal, Simon JL Billinge, et al. Recent advances and applications of deep learning methods in materials science.npj Computational Materials, 8(1):59, 2022
2022
-
[3]
Graph convolutional neural networks with global attention for improved materials property prediction.Physical Chemistry Chemical Physics, 22(32):18141–18148, 2020
Steph-Yves Louis, Yong Zhao, Alireza Nasiri, Xiran Wang, Yuqi Song, Fei Liu, and Jianjun Hu. Graph convolutional neural networks with global attention for improved materials property prediction.Physical Chemistry Chemical Physics, 22(32):18141–18148, 2020
2020
-
[4]
Crystal graph convolutional neural networks for an accurate and interpretable prediction of material properties.Physical review letters, 120(14):145301, 2018
Tian Xie and Jeffrey C Grossman. Crystal graph convolutional neural networks for an accurate and interpretable prediction of material properties.Physical review letters, 120(14):145301, 2018
2018
-
[5]
Atomistic line graph neural network for improved materials property predictions.npj Computational Materials, 7(1):185, 2021
Kamal Choudhary and Brian DeCost. Atomistic line graph neural network for improved materials property predictions.npj Computational Materials, 7(1):185, 2021
2021
-
[6]
Graph networks as a universal machine learning framework for molecules and crystals.Chemistry of Materials, 31(9):3564–3572, 2019
Chi Chen, Weike Ye, Yunxing Zuo, Chen Zheng, and Shyue Ping Ong. Graph networks as a universal machine learning framework for molecules and crystals.Chemistry of Materials, 31(9):3564–3572, 2019
2019
-
[7]
Periodic graph transformers for crystal material property prediction.Advances in Neural Information Processing Systems, 35:15066–15080, 2022
Keqiang Yan, Yi Liu, Yuchao Lin, and Shuiwang Ji. Periodic graph transformers for crystal material property prediction.Advances in Neural Information Processing Systems, 35:15066–15080, 2022
2022
-
[8]
Jianan Nie, Peiyao Xiao, Kaiyi Ji, and Peng Gao. Recinet: Reciprocal space-aware long-range modeling for crystalline property prediction.arXiv preprint arXiv:2502.02748, 2025
Pith/arXiv arXiv 2025
-
[9]
Pscg-net: A multiscale crystal graph neural network for accelerated materials discovery.Journal of Chemical Information and Modeling, 65(20):10871–10884, 2025
Guangyao Chen, Zhilong Wang, and Fengqi You. Pscg-net: A multiscale crystal graph neural network for accelerated materials discovery.Journal of Chemical Information and Modeling, 65(20):10871–10884, 2025
2025
-
[10]
From polyhedra to crystals: a graph- theoretic framework for crystal structure generation.CrystEngComm, 2026
Tomoyasu Yokoyama, Kazuhide Ichikawa, and Hisashi Naito. From polyhedra to crystals: a graph- theoretic framework for crystal structure generation.CrystEngComm, 2026
2026
-
[11]
Local coordina- tion versus overall topology in crystal structures: deriving knowledge from crystallographic databases
Alexander P Shevchenko, Igor A Blatov, Elena V Kitaeva, and Vladislav A Blatov. Local coordina- tion versus overall topology in crystal structures: deriving knowledge from crystallographic databases. Crystal Growth & Design, 17(2):774–785, 2017
2017
-
[12]
Commentary: The materials project: A materials genome approach to accelerating materials innovation.APL Materials, 1:011002, 2013
Anubhav Jain, Shyue Ping Ong, Geoffroy Hautier, Wei Chen, William Davidson Richards, Stephen Dacek, Shreyas Cholia, Dan Gunter, David Skinner, Gerbrand Ceder, et al. Commentary: The materials project: A materials genome approach to accelerating materials innovation.APL Materials, 1:011002, 2013
2013
-
[13]
Schnet– a deep learning architecture for molecules and materials.The Journal of Chemical Physics, 148(24), 2018
Kristof T Sch¨ utt, Huziel E Sauceda, P-J Kindermans, Alexandre Tkatchenko, and K-R M¨ uller. Schnet– a deep learning architecture for molecules and materials.The Journal of Chemical Physics, 148(24), 2018
2018
-
[14]
Examining graph neural networks for crystal structures: Limitations and opportunities for capturing periodicity.Science Advances, 9:eadi3245, 2023
Cong Fu, Handong Ye, Meng Wen, Yining Feng, Kerk Schwarz, Yuyang Sun, Mihir Bhatt, Tarak Bhatt, Subhajit Sanyal, Zhirong Deng, et al. Examining graph neural networks for crystal structures: Limitations and opportunities for capturing periodicity.Science Advances, 9:eadi3245, 2023
2023
-
[15]
Garrity, Andrew C
Kamal Choudhary, Kevin F. Garrity, Andrew C. E. Reid, Brian DeCost, Adam J. Biacchi, Angela R. Hight Walker, Zachary Starrett, Igor Buda, Igal Fleischer, James Park, et al. The joint automated repository for various integrated simulations (jarvis) for data-driven materials design.npj Computa- tional Materials, 6:173, 2020
2020
-
[16]
Quantum chemistry structures and properties of 134 kilo molecules.Scientific data, 1(1):1–7, 2014
Raghunathan Ramakrishnan, Pavlo O Dral, Matthias Rupp, and O Anatole Von Lilienfeld. Quantum chemistry structures and properties of 134 kilo molecules.Scientific data, 1(1):1–7, 2014
2014
-
[17]
Fast and uncertainty-aware directional message passing for non-equilibrium molecules.NeurIPS 2020 Workshop on Machine Learning for Molecules, 2020
Johannes Gasteiger, Florian Becker, and Stephan G¨ unnemann. Fast and uncertainty-aware directional message passing for non-equilibrium molecules.NeurIPS 2020 Workshop on Machine Learning for Molecules, 2020
2020
-
[18]
Gemnet: Universal directional graph neural networks for molecules.Advances in Neural Information Processing Systems, 34:6790–6802, 2021
Johannes Gasteiger, Florian Becker, and Stephan G¨ unnemann. Gemnet: Universal directional graph neural networks for molecules.Advances in Neural Information Processing Systems, 34:6790–6802, 2021
2021
-
[19]
Spherical message passing for 3d molecular graphs.International Conference on Learning Representations (ICLR), 2022
Yi Liu, Limei Wang, Meng Liu, Xuan Zhang, Bora Oztekin, and Shuiwang Ji. Spherical message passing for 3d molecular graphs.International Conference on Learning Representations (ICLR), 2022. 22
2022
-
[20]
Heilman, Weiyi Gong, and Qimin Yan
Alexander J. Heilman, Weiyi Gong, and Qimin Yan. Crystal hypergraph convolutional networks.arXiv preprint arXiv:2411.12616, 2024
Pith/arXiv arXiv 2024
-
[21]
A universal graph deep learning interatomic potential for the periodic table.Nature Computational Science, 2:718–728, 2022
Chi Chen and Shyue Ping Ong. A universal graph deep learning interatomic potential for the periodic table.Nature Computational Science, 2:718–728, 2022
2022
-
[22]
Bartel, and Gerbrand Ceder
Bowen Deng, Peichen Zhong, KyuJung Jun, Janosh Riebesell, Kevin Han, Christopher J. Bartel, and Gerbrand Ceder. Chgnet as a pretrained universal neural network potential for charge-informed atom- istic modelling.Nature Machine Intelligence, 5:1031–1041, 2023
2023
-
[23]
Ilyes Batatia, D´ avid P´ eter Kov´ acs, Gregor N. C. Simm, Christoph Ortner, and G´ abor Cs´ anyi. Mace: Higher order equivariant message passing neural networks for fast and accurate force fields.Advances in Neural Information Processing Systems, 35:11423–11436, 2022
2022
-
[24]
High-throughput identification and characterization of two-dimensional materials using density functional theory.Scientific reports, 7(1):5179, 2017
Kamal Choudhary, Irina Kalish, Ryan Beams, and Francesca Tavazza. High-throughput identification and characterization of two-dimensional materials using density functional theory.Scientific reports, 7(1):5179, 2017
2017
-
[25]
Computational screening of high-performance optoelectronic materials using optb88vdw and tb-mbj formalisms.Scientific data, 5(1):180082, 2018
Kamal Choudhary, Qin Zhang, Andrew CE Reid, Sugata Chowdhury, Nhan Van Nguyen, Zachary Trautt, Marcus W Newrock, Faical Yannick Congo, and Francesca Tavazza. Computational screening of high-performance optoelectronic materials using optb88vdw and tb-mbj formalisms.Scientific data, 5(1):180082, 2018
2018
-
[26]
Elastic properties of bulk and low-dimensional materials using van der waals density functional.Physical review
Kamal Choudhary, Gowoon Cheon, Evan Reed, and Francesca Tavazza. Elastic properties of bulk and low-dimensional materials using van der waals density functional.Physical review. B, 98(1):10–1103, 2018
2018
-
[27]
Accelerated discovery of efficient solar cell materials using quantum and machine-learning methods
Kamal Choudhary, Marnik Bercx, Jie Jiang, Ruth Pachter, Dirk Lamoen, and Francesca Tavazza. Accelerated discovery of efficient solar cell materials using quantum and machine-learning methods. Chemistry of materials, 31(15):5900–5908, 2019
2019
-
[28]
Machine learning with force-field-inspired descriptors for materials: Fast screening and mapping energy landscape.Physical review materials, 2(8):083801, 2018
Kamal Choudhary, Brian DeCost, and Francesca Tavazza. Machine learning with force-field-inspired descriptors for materials: Fast screening and mapping energy landscape.Physical review materials, 2(8):083801, 2018
2018
-
[29]
High-throughput discovery of topologically non-trivial materials using spin-orbit spillage.Scientific reports, 9(1):8534, 2019
Kamal Choudhary, Kevin F Garrity, and Francesca Tavazza. High-throughput discovery of topologically non-trivial materials using spin-orbit spillage.Scientific reports, 9(1):8534, 2019
2019
-
[30]
The joint automated repository for various integrated simulations (jarvis) for data-driven materials design
Kamal Choudhary, Kevin F Garrity, Andrew CE Reid, Brian DeCost, Adam J Biacchi, Angela R Hight Walker, Zachary Trautt, Jason Hattrick-Simpers, A Gilad Kusne, Andrea Centrone, et al. The joint automated repository for various integrated simulations (jarvis) for data-driven materials design. npj computational materials, 6(1):173, 2020
2020
-
[31]
Prediction errors of molecular machine learning models lower than hybrid dft error.Journal of chemical theory and computation, 13(11):5255–5264, 2017
Felix A Faber, Luke Hutchison, Bing Huang, Justin Gilmer, Samuel S Schoenholz, George E Dahl, Oriol Vinyals, Steven Kearnes, Patrick F Riley, and O Anatole Von Lilienfeld. Prediction errors of molecular machine learning models lower than hybrid dft error.Journal of chemical theory and computation, 13(11):5255–5264, 2017
2017
-
[32]
Fast and uncertainty-aware directional message passing for non-equilibrium molecules.Machine Learning for Molecules Workshop at NeurIPS, 2020
Johannes Gasteiger, Shankari Giri, Johannes T Margraf, and Stephan G¨ unnemann. Fast and uncertainty-aware directional message passing for non-equilibrium molecules.Machine Learning for Molecules Workshop at NeurIPS, 2020
2020
-
[33]
Strategies for pre-training graph neural networks.International Conference on Learning Representa- tions (ICLR), 2020
Weihua Hu, Bowen Liu, Joseph Gomes, Marinka Zitnik, Percy Liang, Vijay Pande, and Jure Leskovec. Strategies for pre-training graph neural networks.International Conference on Learning Representa- tions (ICLR), 2020
2020
-
[34]
Ssformer: Self-supervised transformer model for predicting the properties of crystalline materials.Computational Materials Science, 263:114447, 2026
Jie Feng, Tao Sun, and Jianmei Yuan. Ssformer: Self-supervised transformer model for predicting the properties of crystalline materials.Computational Materials Science, 263:114447, 2026
2026
-
[35]
Jiahao Kang, Liang Yang, Jingjie Zeng, Zhi Sun, Hongfei Lin, and Junpeng Li. Graph isomorphism attention network combined with pre-trained language models: a novel approach for crystal material property prediction.Neural Computing and Applications, 37(30):25061–25076, 2025
2025
-
[36]
Benchmarking materi- als property prediction methods: the matbench test set and automatminer reference algorithm.npj Computational Materials, 6(1):138, 2020
Alexander Dunn, Qi Wang, Alex Ganose, Daniel Dopp, and Anubhav Jain. Benchmarking materi- als property prediction methods: the matbench test set and automatminer reference algorithm.npj Computational Materials, 6(1):138, 2020. 23
2020
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.