We introduce IGNITE, a generative world foundation model for fusion plasma behavior simulation trained in a self-supervised manner from over a decade of unlabeled experimental data at the DIII-D National Fusion Facility. The core of IGNITE is a dynamics model that can simulate DIII-D discharges from a given set of actuator trajectories. These trajectories can be supplied or generated on-the-fly from a textual prompt or from desired experimental outcomes. The model architecture consists of several spatio-temporal tokenizers that embed the different input modalities, including time-series like spatio-temporal measurement data, image sequences, and high-resolution spectrograms, each of which collected at vastly different time scales. The backbone is composed of an auto-regressive dynamics model that has the capacity to predict entire DIII-D discharges given initial latent plasma states and actuator trajectories over a theoretical infinite horizon. IGNITE paves the way towards efficient AI-driven experimental planning and world modeling for nuclear fusion.
Figures & tables
Figure 1: Main outline of the IGNITE world model.
Figure 2: IGNITE learning curves for different regularization levels and dataset sizes. Figure 2a : A subset of 1000 shots leads to overfitting, despite regularization.
Figure 3: IGNITE predicts the DIII-D discharge 190735 from the held-out validation set.
Appendix figures & tables5 assets
Supplementary material from the paper’s appendix.
Appendix
Diagnostic
Measured properties
Channels
Sampling freq.
Resampled freq.
Modality type
CER
Ion temperature ( Ti ), plasma rotation ( vtor )
2$\times$48
100Hz
–
Slow time series
MSE
Magnetic pitch angle
69
100Hz
–
Slow time series
TS
Electron temperature ( Te ) and density ( ne )
2$\times$44 & 2$\times$10
100Hz
–
Slow time series
Filterscopes
Line emissions
8
10kHz
–
Fast time series
BES
Fluctuations
16
1MHz
500kHz
Spectrogram
ECE
Electron temperature
48
500kHz
–
Spectrogram
Appendix
Table 1: Overview of the diagnostics used for this study.
Table 2: Overview of the actuators used for this study.
Figure 4: Tokenizer for slow time series. The channel-time array is grouped into four channel groups and patched at 5 samples × channels; a shared linear layer projects each patch by Linear →5×128$$ ; a time encoding and a sequence-position encoding are added to each token; the token sequence, each 128-dimensional, is processed by the transformer to produce the model output.
Figure 5: Tokenizer for fast time series. A 50ms window of 8 channels sampled at 10kHz gives 500 samples per channel; a Conv1D front end reduces each channel to 5 frames, patched at 5×8 over frames and channels. A shared Linear →8×256$$ projects each patch, a 256 -wide time encoding is added, and the token sequence is processed by the transformer to produce the model output.
Figure 6: Tokenizer for spectrograms. SEach of the C channels contributes a time-frequency map of 98 frames, cut into 16×16 patches, giving 192 patches per channel. Patches at the same grid position are concatenated across channels and an MLP reduces them to 192$\times$256 . A frequency encoding ( 32$\times$256 ) and a time encoding ( 6×256$$ ) form a 32×6 table whose entries are 256-dimensional vectors, added to the token at that grid position, before the transformer produces the model output.
Inertial confinement fusion (ICF) is a leading pathway toward clean energy, but each shot at the National Ignition Facility costs on the order of one million dollars, making accurate AI surrogates a high-value target. We study exogenous-driven ICF waveform prediction, where a 512-step neutron-rate diagnostic must be inferred directly from a laser pulse and target design parameters, with no historical response observed. The regime stresses standard time-series predictors with temporal sparsity (picosecond peak in a nanosecond window), input-output scale mismatch (under 300 real shots), and peak sensitivity (picosecond timing). We propose ICF-DLM, to our knowledge the first LM-based ICF predictor, combining (i) a physics-typed decomposition into yield YDT, peak timing tpeak, and local waveform wlocal; (ii) bidirectional denoising that defers commitment to peak location; and (iii) a physics-driven PPO reward re-injecting metric structure across numeric tokens. On ICFBench (50K simulations + 232 experimental shots), ICF-DLM cuts peak-timing error from 11.6 to 9.2 steps over a matched autoregressive LLaMA-3-8B and outperforms classical sequence models and LLM-based time-series predictors. Beyond ICF, the recipe shows potential to address science domains with low data and sparse events.
We present TokaMind, to our knowledge the first open-source foundation model for tokamak plasma dynamics, based on a Multi-Modal Transformer (MMT) and pretrained on heterogeneous diagnostics from the publicly available MAST dataset. TokaMind supports multiple data modalities (time-series, 2D profiles, and videos) with different sampling rates, robust missing-signal handling, and efficient task adaptation via selectively loading and freezing four model components. To represent multi-modal signals, we use a lightweight fixed-basis Discrete Cosine Transform embedding (DCT3D) and provide a clean interface for alternative embeddings (e.g., Variational Autoencoders). We evaluate TokaMind on the recently introduced MAST benchmark TokaMark, which comprises 14 tasks with heterogeneous reconstruction and forecasting objectives. Our results show that fine-tuned TokaMind outperforms the strongest benchmark baseline on all but one task. Compared with training the same architecture from scratch under a matched epoch budget, warm-start adaptation is most beneficial on demanding downstream settings, including long-horizon forecasting and high-dimensional equilibrium objectives. These findings highlight the value of multi-modal pretraining for tokamak plasma dynamics and provide a practical, extensible foundation for future fusion modeling tasks. Training code and model weights are publicly available at github.com/UKAEA-IBM-STFC-Fusion-FMs/tokamind and huggingface.co/UKAEA-IBM-STFC, respectively.
Tobia Boschi, Andrea Loreti, Nicola C. Amorisco +13
IBM Research Dublin, Ireland · UK Atomic Energy Authority Abingdon, UK · STFC Hartree Centre Daresbury, UK
World models represent a paradigm shift in generative AI, pursuing predictive understanding and controllable simulation of environments in a structured and generalizable way. We present World Machine, a generative world-modeling architecture for time series. It is a transformer-based architecture with latent states that enables adaptation to different amounts of observed data and contexts. This shows an improvement over traditional transformers, which have a computational and memory cost that scales quadratically with the context. Experiments on a proposed synthetic dataset, Toy1D, validate the approach's feasibility, demonstrate capabilities not found in conventional transformers, and highlight the contributions of each component of the training protocol.
Elton Cardoso do Nascimento, Alexandre da Silva Simões, Esther Luna Colombini +2
Universidade Estadual de Campinas (UNICAMP), {FEEC, IC} · Universidade Estadual Paulista (UNESP), Instituto de Ciˆencia e Tecnologia, Sorocaba