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ALIGNN: Atomistic Line Graph Neural Network

Updated 16 December 2025
  • ALIGNN is a geometric deep learning model that utilizes dual graph representations to explicitly encode pairwise, three-body, and four-body interactions in atomistic systems.
  • It employs an alternating, edge-gated message passing algorithm that integrates atomic, bond, and angular features, yielding state-of-the-art predictive performance.
  • The framework’s computational efficiency and interpretability support diverse applications, predicting materials properties such as energies, spectra, and force fields.

The Atomistic Line Graph Neural Network (ALIGNN) is a class of geometric deep learning models specifically designed to represent and predict properties of atomistic systems—such as crystals, molecules, alloys, and frameworks—by directly encoding both pairwise (bond) and higher-order (angular) structural information. ALIGNN achieves this through a dual-graph message passing architecture: an atomistic graph representing atoms and their pairwise interactions, and its line graph encoding three-body (bond-angle) relationships. The method is extensible to capture four-body (dihedral) correlations through additional line graphs. ALIGNN and its variants have established state-of-the-art performance across a range of atomistic prediction tasks, including formation energies, spectral properties, force fields, adsorption, and nonlinear optical coefficients.

1. Dual Graph Representation: Atomistic and Line Graphs

ALIGNN constructs two coupled graphs for each atomic structure:

  • Atomistic Graph G=(V,E)\mathcal{G} = (\mathcal{V}, \mathcal{E}): Nodes iVi\in\mathcal{V} represent atoms, with initial features typically drawn from atomic descriptors (e.g., atomic number, group, electronegativity). Edges (i,j)E(i,j)\in\mathcal{E} represent chemical or geometric bonds, featurized by radial basis expansions of interatomic distance dijd_{ij}.
  • Line Graph L(G)=(VL,EL)\mathcal{L}(\mathcal{G}) = (\mathcal{V}_L, \mathcal{E}_L): Each node in VL\mathcal{V}_L corresponds to an edge in G\mathcal{G} (“bond-node”). An edge in L(G)\mathcal{L}(\mathcal{G}) connects two bonds sharing an atom, encoding the bond angle as a feature (e.g., via a radial or Gaussian basis for αijk\alpha_{ijk} at central atom jj between bonds (i,j)(i,j) and (j,k)(j,k)) (Choudhary et al., 2021).

For extended angular correlations, ALIGNN-d ("d" for dihedral) introduces a second line graph L(G)\mathcal{L}'(\mathcal{G}), whose edges correspond to dihedral angles αijkl\alpha'_{ijkl} formed between planes defined by consecutive bond pairs, using periodic basis encoding to preserve the inherent periodicity of dihedrals (Hsu et al., 2021).

This dual-(or multi-)graph representation allows explicit encoding of three- and four-body geometrical invariants that are critical for disambiguating chiral or highly-coordinated environments.

2. Edge-Gated Message Passing and Mathematical Formulation

At the heart of ALIGNN is an alternating, edge-gated message passing protocol spanning both G\mathcal{G} and L(G)\mathcal{L}(\mathcal{G}):

  • Atomistic Graph Update (per atom ii at layer \ell):

hi+1=hi+SiLU(LayerNorm(Wshi+jN(i)e^ij(Wdhj)))h_i^{\ell+1} = h_i^\ell + \text{SiLU}\left(\text{LayerNorm}\bigl(W_s^\ell h_i^\ell + \sum_{j\in\mathcal{N}(i)}\hat{e}_{ij}^\ell \odot (W_d^\ell h_j^\ell)\bigr)\right)

with an edge-gating function e^ij=σ(eij)jσ(eij)+ϵ\hat{e}_{ij}^\ell = \frac{\sigma(e_{ij}^\ell)}{\sum_{j'}\sigma(e_{ij'}^\ell)+\epsilon} (where σ\sigma is sigmoid), followed by bond embedding update:

eij+1=eij+SiLU(LayerNorm(Wg[hihjeij]))e_{ij}^{\ell+1} = e_{ij}^\ell + \text{SiLU}\left(\text{LayerNorm}(W_g^\ell[h_i^\ell\oplus h_j^\ell\oplus e_{ij}^\ell])\right)

  • Line Graph Update (per bond-node (ij)(ij)):

b(ij)+1=b(ij)+SiLU(LayerNorm(Wsb(ij)+(jk)NLa^(ij),(jk)(Wdb(jk))))b_{(ij)}^{\ell+1} = b_{(ij)}^\ell + \text{SiLU}\Bigl(\text{LayerNorm}\bigl(W_s^\ell b_{(ij)}^\ell + \sum_{(jk)\in\mathcal{N}_L}\hat a_{(ij),(jk)}^\ell \odot (W_d^\ell b_{(jk)}^\ell)\bigr)\Bigr)

a(ij),(jk)+1=a(ij),(jk)+SiLU(LayerNorm[Wg(b(ij)b(jk)a(ij),(jk))])a_{(ij),(jk)}^{\ell+1} = a_{(ij),(jk)}^\ell + \text{SiLU}\Bigl(\text{LayerNorm}[W_g^\ell(b_{(ij)}^\ell\oplus b_{(jk)}^\ell\oplus a_{(ij),(jk)}^\ell)]\Bigr)

Here, b(ij)eijb_{(ij)}^\ell \equiv e_{ij}^\ell and a^\hat a represents the bond-angle gate.

For ALIGNN-d, this machinery is extended to a second line-graph layer, propagating dihedral embeddings.

Aligning these updates enables the network to cooperate across pairwise, three-body, and four-body geometric descriptors, admitting expressive representations critical for geometry-sensitive properties (Choudhary et al., 2021, Hsu et al., 2021).

3. Input Encoding, Representation, and Expressive Power

Atomic Features:

Typically one-hot encoding of atomic number augmented by a vector of elemental properties (group, period, electronegativity, covalent radius, mass, valence electron count) (Beaver et al., 11 Sep 2024). Features are processed via embedding layers.

Bond Features:

Radial basis function (RBF) expansions (Gaussian or Bessel) of distances dijd_{ij}, e.g.,

RBFn(d)=exp[γn(dμn)2]\mathrm{RBF}_n(d) = \exp[-\gamma_n (d-\mu_n)^2]

with n=1Nrbfn=1\dots N_\text{rbf}, centers μn\mu_n, and widths γn\gamma_n (Hsu et al., 2021). The choice of NrbfN_\text{rbf} is architecture-dependent (e.g., 32–80) (Choudhary et al., 2021).

Angle and Dihedral Features:

  • Bond Angles αijk\alpha_{ijk}: Encoded via Gaussian expansion of either angle or its cosine, populating part of the edge embedding vector.
  • Dihedral Angles αijkl\alpha'_{ijkl} (ALIGNN-d): Each angle is mapped to (cosα,sinα)(\cos\alpha', \sin\alpha') for periodicity, with each component RBF-expanded into a dedicated region of the embedding vector, with explicit separation from bond-angle channels (Hsu et al., 2021).

Such encoding ensures that directional or chiral distinctions are preserved, overcoming degeneracies in 2-body representations.

The use of dual-graph (and higher-order) propagation in conjunction with these featurizations allows ALIGNN to match the expressive power of fully-connected (maximal) graphs with significantly fewer edges, retaining computational efficiency (Hsu et al., 2021).

4. Training Regimens, Loss Functions, and Optimization

Loss Functions:

  • Regression of Physical Quantities: Usual mean squared error (MSE) between predictions and targets for scalar properties (e.g., formation energy, band gap, adsorption capacity, SHG coefficients).
  • Force-Field Training (ALIGNN-FF): Weighted sum of energy-MSE and force-MSE, i.e.,

L=λE1Ni(EipredEiDFT)2+λF13Natomsi,α(Fi,αpredFi,αDFT)2L = \lambda_E\,\frac{1}{N}\sum_{i}(E_i^\text{pred} - E_i^\text{DFT})^2 + \lambda_F\,\frac{1}{3N_\text{atoms}}\sum_{i,\alpha}(F_{i,\alpha}^\text{pred} - F_{i,\alpha}^\text{DFT})^2

Optimization is typically performed via AdamW, with layer normalization and residual connections supporting stability and convergence; learning rate schedules and early stopping control overfitting.

Data and Validation:

  • Training Sets: Large-scale datasets such as JARVIS-DFT (~55,000 crystals; ~1.2M structures for force fields), hypothetical MOFs, and specialty property-specific databases (e.g., NOEMD for SHG) (Choudhary et al., 2021, Choudhary et al., 2022, Alkabakibi et al., 28 Apr 2025).
  • Split Protocols: Standard practice is 80/10/10 (train/val/test), with cross-validation for small or imbalanced datasets.

5. Evaluated Tasks and Domain Applications

ALIGNN’s architecture has proven effective across multiple application areas:

  • Materials Property Prediction: Scalar and spectral targets including formation energy, electronic band gap, density of states (DOS), phonon spectra, and nonlinear optical (e.g., SHG Kurtz–Perry coefficient) (Choudhary et al., 2021, Kaundinya et al., 2022, Alkabakibi et al., 28 Apr 2025).
  • Adsorption in Metal–Organic Frameworks (MOFs): Rapid prediction of CO2_2 uptakes, isotherms, pore geometries, and bandgaps in hMOF and CoREMOF databases, enabling high-throughput virtual screening (Choudhary et al., 2021).
  • Force-Field and Surrogate Modeling (ALIGNN-FF): Unified accurate prediction of energies and forces across a chemically diverse periodic table, supporting pre-optimization, structure search, and large-scale dynamical simulation (Choudhary et al., 2022, Beaver et al., 11 Sep 2024).
  • Optical and Thermodynamic Spectra: Efficient learning of full electron and phonon DOS, enabling computation of derived quantities like heat capacities, vibrational entropies, and SHG intensities (Kaundinya et al., 2022, Gurunathan et al., 2022).
  • High-Entropy Alloy Stability: Screening of structural phases (FCC, BCC) via surrogate modeling, with experimental validation in new alloy systems (Beaver et al., 11 Sep 2024).

ALIGNN-d specifically enables interpretability and chemical insight in angularly-sensitive optical phenomena, such as distinguishing the contributions of bond and dihedral angles to IR absorption in disordered metal–aqua complexes (Hsu et al., 2021).

6. Architectural Advantages, Memory Efficiency, and Interpretability

ALIGNN achieves a balance between expressivity and computational cost by making selectivity over explicit geometric interactions:

  • Memory Efficiency: By using only nearest-neighbor bonds (O(N)) and a controlled number of line-graph edges, ALIGNN-d achieves the same geometric expressivity as a maximally connected graph (O(N2^2)) but with far fewer edges (e.g., 135 vs. 120 edges for a five-coordinated Cu(II) aqua complex, yet capturing all three/four-body invariants) (Hsu et al., 2021).
  • Interpretability: The network structure allows per-component decomposition of predictions. Final scalar outputs for each atom, bond, angle, and dihedral are accessible, enabling attributions and visualization of the structural origins of target properties. This facility has facilitated tractable insight into the geometric motifs underlying spectral features or structure-function relationships (Hsu et al., 2021).

7. Extensions, Limitations, and Future Directions

While ALIGNN and its variants have demonstrated leading performance, certain limitations and active research directions remain:

  • Higher-Order Interactions: ALIGNN-d extends explicitly to four-body (dihedral) terms; further higher-order correlations may require additional graphical constructs, potentially with added complexity (Hsu et al., 2021).
  • Transferability and Data Coverage: Pretraining on broad datasets enables generalization but may impose systematic biases when deployed on out-of-distribution chemistries (e.g., high-entropy alloys not seen during force-field training). Fine-tuning or active learning can mitigate such effects (Beaver et al., 11 Sep 2024, Choudhary et al., 2022).
  • Lattice and Phase Diversity: Application beyond binary phase stability (e.g., to hexagonal or multiphase systems) requires extending sampling strategies or candidate generation (Beaver et al., 11 Sep 2024).
  • Long-range Interactions: Cutoff-based edge construction may miss physically relevant long-range effects in certain porous or extended systems (Choudhary et al., 2021).
  • Interpretability Frontier: While component attributions are enabled, hidden-layer interpretations and the mapping from learned features to chemical causality are still limited in their transparency.

Proposed future approaches include integration of coordinate relaxation loops, direct modeling of phase separation in alloys, active data acquisition for underrepresented chemistries, and deeper exploitation of componentwise interpretability, as well as applications in closed-loop materials discovery platforms (Hsu et al., 2021, Beaver et al., 11 Sep 2024, Alkabakibi et al., 28 Apr 2025).


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