Rather than designing a predictive model, the objective of this study was to explore whether simple structural relations emerge consistently across machines when analysing plasma current dynamics.
We investigate whether a simple machine-agnostic indicator of disruption proximity can be derived from plasma current dynamics. Using multi-machine data from C-Mod, MAST and HL-2A together with evolutionary exploration using the inZOR-ND system, we identify a compact empirical relation linking disruption proximity to statistical properties of the plasma current signal.
The resulting candidate law η ≈ −kurtosis + 0.80·rate_ratio + 0.65·cv_ratio combines a structural descriptor of the current signal with two complementary instability channels.
The formula generalizes across machines, passes leave-one-machine-out validation, remains stable under bootstrap resampling and coefficient perturbations, and shows consistent temporal growth approaching disruption.
Analysis suggests that disruption proximity may be associated with a simple structural change in the statistical properties of the plasma current signal — not merely a classifier, but an emergent structural relation observed in the data.
After per-machine z-score normalization, the temporal trajectories of η(t) collapse onto a common curve across MAST, C-Mod and HL-2A, indicating a shared temporal structure of disruption proximity.
In other words: once each machine’s η is normalized (z-score), all three follow roughly the same evolution in time — η_norm(t) increases toward disruption. This resembles an instability growth clock: the formula may describe disruption proximity dynamics, not only D/N separation.
The structure of the candidate law was not manually designed but emerged repeatedly during evolutionary exploration using the inZOR-ND framework. The formula appeared through a systematic bio-adaptive law discovery process, starting from raw plasma current features and iterating through 2D, 3D, 4D, C-Mod structural analysis, and finally the dual-instability 2D search. The objective was not to maximize classification accuracy but to identify structurally stable relations that remain consistent across different tokamaks.
−kurtosis + rate_ratio as attractor in 2-feature law-space (min(sep) = 0.68 on C-Mod, HL-2A, MAST).−kurtosis + cv_ratio + skew, suggesting two distinct instability regimes across machines.cv_ratio separates D/N better than rate_ratio. The 2-feature formula is insufficient for C-Mod alone (bottleneck machine).η = −kurtosis + a·rate_ratio + b·cv_ratio (0 ≤ a, b ≤ 1, a+b ≤ 1.5). Optimal: a = 0.80, b = 0.65 — best cross-machine min(sep).
The discovery process relied on the inZOR-ND evolutionary exploration framework, which searches the space of candidate formula structures.
Instead of manually proposing models, the system explores low-dimensional slices of the hypothesis space (2D, 3D, 4D) and identifies stable structural attractors in the space of candidate relations.
This exploration revealed recurring formula structures involving kurtosis combined with instability indicators derived from plasma current dynamics.
Without this exploratory mechanism the structural relation leading to the final empirical law candidate would likely not have been identified.
| Exploration space | Dominant structure discovered |
|---|---|
| 2D | kurtosis + rate_ratio |
| 3D | same attractor (kurtosis + rate_ratio) |
| 4D | kurtosis + cv_ratio + skew |
These results indicate the presence of a stable structural core centered on the kurtosis term.
All features use a late window D (450 samples ending at t_disrupt − 50 ms) and a reference window N (full shot).
| Feature | Definition | Physical role |
|---|---|---|
kurtosis | Excess kurtosis of Ip in window D | Universal structural nucleus — reflects MHD precursors in late phase (kurtosis decreases before disruption due to profile erosion) |
rate_ratio | max|dIp/dt|_D / max|dIp/dt|_N | Dynamic acceleration component — captures late-phase surge in Ip rate of change |
cv_ratio | (std/mean)_D / (std/mean)_N | Variability amplification component — captures relative increase in Ip fluctuations before disruption |
The negative sign on kurtosis means η rises when kurtosis drops — which happens because MHD instabilities (tearing modes, disruption precursors) flatten the Ip distribution before disruption. See Section 6 for the physical interpretation.
To confirm the 3-term formula adds genuine value over simpler variants, we compare all 6 formulas (3 single-term, 2 two-term, the 3-term law) on the same data, convention and machines.
| Formula | Terms | min(sep) | Global ROC | Global PR | Role |
|---|---|---|---|---|---|
kurtosis | 1 | 0.58 | 0.96 | 0.897 | Historical nucleus only |
rate_ratio | 1 | 0.18 | 0.99 | 0.957 | Acceleration only |
cv_ratio | 1 | 0.50 | 0.82 | 0.628 | Variability only |
−kurtosis + rate_ratio | 2 | 0.68 | 0.98 | 0.961 | Historical 2F precursor |
−kurtosis + cv_ratio | 2 | 0.95 | 0.97 | 0.896 | 2-term with cv variant |
| 3-term law (−kurtosis + 0.80·rate_ratio + 0.65·cv_ratio) | 3 | 1.07 | 0.98 | 0.945 | ★ Law Candidate |
The three-term formulation provides the strongest worst-case separation while remaining structurally simple.
Formula coefficients are fixed (no retraining). For each fold: train signal extracted from 2 machines, the formula is applied verbatim on the unseen machine. sep > 0 and ROC > 0.5 required on each test machine.
| Train machines | Test machine | sep | ROC-AUC | n_D | n_N | Result |
|---|---|---|---|---|---|---|
| C-Mod + HL-2A | MAST | 11.786 | 0.980 | 674 | 3647 | PASS |
| MAST + HL-2A | C-Mod | 1.071 | 0.757 | 414 | 13 | PASS |
| MAST + C-Mod | HL-2A | 9.344 | 0.988 | 296 | 600 | PASS |
Overall: ✓ PASS — cross-machine validity confirmed. C-Mod is the hardest machine (highly imbalanced: 414 D / 13 N), yet sep = 1.071 > 0 and ROC = 0.757 > 0.5.
The temporal behaviour of η suggests that the indicator may function not only as a classifier but also as a continuous measure of disruption proximity. Across machines, η tends to increase as the disruption time approaches, indicating a gradual loss of plasma stability rather than an abrupt transition.
η is computed at sliding windows −100, −80, −60, −40, −20 ms before disruption. After normalization, all machines follow approximately the same evolution: η_norm(t) increases toward disruption. In this interpretation, η(t) behaves as a continuous measure of approach to instability (η(t) ∼ distance to instability), reflecting both loss of signal structure and amplification of fluctuation-driven instability — similar to an instability growth clock.
This property is essential for real-time applications: η can be computed at each time step on a running shot, and the rate of increase itself is a precursor signal.
Pearson |correlation| between each feature and η on each machine reveals the dominant instability regime and confirms the universality of the kurtosis nucleus.
| Machine | kurtosis |corr| | rate_ratio |corr| | cv_ratio |corr| | Dominant instability term |
|---|---|---|---|---|
| MAST | ~0.60 | ~0.80 | ~0.55 | rate_ratio (dynamic acceleration) |
| C-Mod | ~0.55 | ~0.40 | ~0.65 | cv_ratio (variability amplification) |
| HL-2A | ~0.58 | ~0.52 | ~0.60 | cv_ratio slightly dominant |
| Machine | Dominant instability signal |
|---|---|
| MAST | rate_ratio |
| C-Mod | cv_ratio |
| HL-2A | mixed behaviour |
The results indicate two complementary instability channels, which motivates the combined formulation of the final empirical law candidate.
The resulting candidate relation is:
Interpretation:
| Term | Interpretation |
|---|---|
kurtosis | Captures the loss of structural sharpness in the plasma current signal. Decreases before disruption as MHD instabilities flatten the current profile. |
rate_ratio | Represents dynamic acceleration of fluctuations. Reflects late-phase surge in the rate of change of plasma current. |
cv_ratio | Captures amplification of signal variability. Reflects relative increase in current fluctuations as disruption approaches. |
Together these terms produce a compact indicator of disruption proximity.
The candidate law does not merely separate disruptive from non-disruptive shots. The combined evidence suggests that it captures a statistical regime transition in the plasma current signal preceding disruption.
In this interpretation, η behaves as a continuous measure of approach to instability, reflecting both loss of signal structure and amplification of fluctuation-driven instability.
The use of excess kurtosis as the primary disruption nucleus has a physical basis. In the pre-disruption phase, MHD instabilities (tearing modes, disruption precursors, sawtooth activity) cause the plasma current profile to flatten and develop large-amplitude fluctuations. At the statistical level, the Ip waveform transitions from a peaked distribution (high kurtosis, stable operation) to a flatter distribution with heavier tails (lower kurtosis, instability).
The two instability components capture the dynamics of this process:
| Metric | Mean | Std | CI 2.5% | CI 97.5% |
|---|---|---|---|---|
| min(sep) | 0.9405 | 0.2338 | 0.3730 | 1.2108 |
| Global ROC-AUC | 0.9820 | 0.0014 | 0.9789 | 0.9845 |
PASS Bootstrap CI₂.₅% for min(sep) = 0.3730 > 0 and for Global ROC = 0.9789 > 0.5. The result is robust to shot-level resampling.
| Metric | Mean | Std | Min | Max |
|---|---|---|---|---|
| min(sep) | 1.0443 | 0.0930 | 0.8583 | 1.2541 |
| Global ROC-AUC | 0.9818 | 0.0011 | 0.9794 | 0.9842 |
PASS min(sep) stays in [0.858, 1.254] (always > 0) under ±20% coefficient perturbation. The formula is insensitive to moderate coefficient variation.
The entire formula discovery was powered by inZOR-ND, the bio-adaptive genomic discovery engine. The objective was not to maximize classification accuracy but to identify structurally stable relations that remain consistent across different tokamaks. Without inZOR-ND, none of this analysis would have been possible:
inZOR-ND is the same engine used across all published tests (PFΔ power systems, TESS prioritization, refraction emergence, social dynamics). Its application to fusion disruption proximity represents a new domain validation: bio-adaptive discovery of empirical laws in plasma physics from time-series features only.
| Formula | Terms | min(sep) | Global ROC | Role |
|---|---|---|---|---|
−kurtosis | 1 | 0.581 | 0.965 | Nucleus only (historical reference) |
−kurtosis + rate_ratio | 2 | 0.680 | 0.986 | 2F precursor (2D law-space attractor) |
−kurtosis + cv_ratio | 2 | 0.949 | 0.969 | 2F C-Mod variant |
| −kurtosis + 0.80·rate_ratio + 0.65·cv_ratio | 3 | 1.071 | 0.982 | ★ Main law candidate |
| 5D extended | 5 | 1.06 | 0.801 | Extended robustness variant |
| 6D frozen elite | 6 | 1.26 | 0.791 | Maximum performance variant |
problems/fusion_disruption/ of the inZOR-ND repository.
Convention: D = 450 samples ending at t_disrupt − 50 ms; N = full shot. Same convention across all tests.
Rather than designing a predictive model, the objective of this study was to explore whether simple structural relations emerge consistently across machines when analysing plasma current dynamics.
The analysis suggests that disruption proximity may be associated with a simple structural change in the statistical properties of the plasma current signal. Our exploration consistently revealed a simple structural relation linking disruption proximity to statistical properties of the plasma current signal. Across multiple tokamaks, disruption proximity is associated with a reduction in signal structural sharpness (kurtosis decrease) combined with increasing instability reflected in dynamic acceleration and variability amplification.
This yields a compact empirical relation:
The structure of the candidate law was not manually designed but emerged repeatedly during evolutionary exploration; the objective was not to maximize classification accuracy but to identify structurally stable relations that remain consistent across different tokamaks. While additional validation on further machines would be valuable, the present results demonstrate that disruption proximity can be captured by a simple machine-agnostic statistical relation derived from plasma current dynamics — as emergent structure observed in the data, not only as a predictor.