inZOR-ND — FUSION DISRUPTION PROXIMITY

inZOR-ND: Empirical Law Candidate for Machine-Agnostic Disruption Proximity

Derived from Plasma Current Dynamics Alone · Validated on MAST, C-Mod, HL-2A · 3-Machine Cross-Validation
Dumitru Novic · March 2026 · 1,384 disruptive windows · 4,260 non-disruptive windows · 3 tokamaks

Abstract

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.

Main Empirical Law Candidate (3-term, dual-instability)
η ≈ −kurtosis + 0.80 · rate_ratio + 0.65 · cv_ratio
η increases as plasma approaches disruption  ·  Derived from Ip only  ·  No machine-specific tuning
1.071
min(sep) cross-machine
0.982
Global ROC-AUC
LOMO Pass (all 3 folds)
3
Tokamaks validated
1,384
Disruptive windows
>0
Bootstrap CI₉₅ min(sep)
How to read this result

Shared temporal structure: collapse test

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.

Cross-machine collapse: z-score and min-max normalized η(t)
Fig — Cross-machine collapse test. Left: z-score normalization per machine. Right: min-max [0,1] per machine. After z-score, the three machines follow a common temporal curve; the shared evolution supports a single machine-agnostic temporal structure of the indicator.

1. How We Got Here — Discovery Path with inZOR-ND

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.

1
2D exploration: inZOR-ND converges to −kurtosis + rate_ratio as attractor in 2-feature law-space (min(sep) = 0.68 on C-Mod, HL-2A, MAST).
2
3D extension: A second valley emerges: −kurtosis + cv_ratio + skew, suggesting two distinct instability regimes across machines.
3
C-Mod structural analysis: On C-Mod, cv_ratio separates D/N better than rate_ratio. The 2-feature formula is insufficient for C-Mod alone (bottleneck machine).
4
Dual-instability test: 2D grid search (a, b) in 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).
5
Validation: LOMO, temporal trajectory η(t), per-machine structural analysis, bootstrap (300 replicas), sensitivity (±20%, 300 replicas). All pass.
Discovery path from single features to 3-term law
Fig 0 — Discovery path: min(sep) staircase from 1-term < 2-term < 3-term. The 3-term law achieves the largest cross-machine robustness (min(sep) = 1.071), discovered by inZOR-ND without manual formula design.

Evolutionary exploration with inZOR-ND

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.

Dimensional exploration results

Exploration spaceDominant structure discovered
2Dkurtosis + rate_ratio
3Dsame attractor (kurtosis + rate_ratio)
4Dkurtosis + cv_ratio + skew

These results indicate the presence of a stable structural core centered on the kurtosis term.

2. Feature Definitions (Derived from Ip Only)

All features use a late window D (450 samples ending at t_disrupt − 50 ms) and a reference window N (full shot).

FeatureDefinitionPhysical role
kurtosisExcess kurtosis of Ip in window DUniversal structural nucleus — reflects MHD precursors in late phase (kurtosis decreases before disruption due to profile erosion)
rate_ratiomax|dIp/dt|_D / max|dIp/dt|_NDynamic acceleration component — captures late-phase surge in Ip rate of change
cv_ratio(std/mean)_D / (std/mean)_NVariability 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.

3. Validation — Formula Comparison

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.

Ablation comparison
Fig 1 — Baseline / Ablation Test. Left: min(sep) increases monotonically: 1-term < 2-term < 3-term. Right: Global ROC-AUC. The 3-term law candidate achieves the highest cross-machine robustness.
FormulaTermsmin(sep)Global ROCGlobal PRRole
kurtosis10.580.960.897Historical nucleus only
rate_ratio10.180.990.957Acceleration only
cv_ratio10.500.820.628Variability only
−kurtosis + rate_ratio20.680.980.961Historical 2F precursor
−kurtosis + cv_ratio20.950.970.8962-term with cv variant
3-term law (−kurtosis + 0.80·rate_ratio + 0.65·cv_ratio)31.070.980.945★ Law Candidate

The three-term formulation provides the strongest worst-case separation while remaining structurally simple.

4. Leave-One-Machine-Out (LOMO) Validation

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.

LOMO validation
Fig 2 — LOMO Validation: sep and ROC-AUC for each test machine (left-out machine). All 3 folds PASS. The formula generalises without retraining across MAST, C-Mod, HL-2A.
Train machinesTest machinesepROC-AUCn_Dn_NResult
C-Mod + HL-2AMAST11.7860.9806743647PASS
MAST + HL-2AC-Mod1.0710.75741413PASS
MAST + C-ModHL-2A9.3440.988296600PASS

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.

5. Temporal Trajectory η(t) — Continuous Measure of Disruption Proximity

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.

Temporal η(t) trajectory
Fig 3 — Temporal trajectory of η(t) for C-Mod, HL-2A and MAST. Mean η (solid line) ± std (shaded). η increases monotonically in all three machines as plasma approaches disruption, confirming the clock-like behaviour of the indicator.

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.

6. Per-Machine Structural Analysis

Pearson |correlation| between each feature and η on each machine reveals the dominant instability regime and confirms the universality of the kurtosis nucleus.

Per-machine structural analysis
Fig 4 — Per-machine structural analysis: |Pearson correlation| between kurtosis, rate_ratio, cv_ratio and η. kurtosis is a common nucleus across all machines. rate_ratio dominates on MAST; cv_ratio dominates on C-Mod and HL-2A.
Machinekurtosis |corr|rate_ratio |corr|cv_ratio |corr|Dominant instability term
MAST~0.60~0.80~0.55rate_ratio (dynamic acceleration)
C-Mod~0.55~0.40~0.65cv_ratio (variability amplification)
HL-2A~0.58~0.52~0.60cv_ratio slightly dominant

Structural dominance per machine

MachineDominant instability signal
MASTrate_ratio
C-Modcv_ratio
HL-2Amixed behaviour

The results indicate two complementary instability channels, which motivates the combined formulation of the final empirical law candidate.

6b. Main Empirical Law Candidate

The resulting candidate relation is:

η ≈ −kurtosis + 0.80 · rate_ratio + 0.65 · cv_ratio

Interpretation:

TermInterpretation
kurtosisCaptures the loss of structural sharpness in the plasma current signal. Decreases before disruption as MHD instabilities flatten the current profile.
rate_ratioRepresents dynamic acceleration of fluctuations. Reflects late-phase surge in the rate of change of plasma current.
cv_ratioCaptures amplification of signal variability. Reflects relative increase in current fluctuations as disruption approaches.

Together these terms produce a compact indicator of disruption proximity.

Interpretation: statistical regime transition

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.

Summary of disruption proximity law candidate
Figure: Summary of the disruption proximity law candidate and its validation across machines.

7. Physical Interpretation — Why kurtosis Decreases

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:

Scope statement:
  • This is an empirical candidate law derived from Ip features on three machines. It is not a first-principles physical law.
  • The formula does not use magnetic equilibrium, temperature, density, or other diagnostic signals.
  • Performance on unseen machines, higher-dimensional diagnostics, or real-time deployment may differ.
  • The inZOR-ND discovery engine discovered the formula structure; the physical grounding is offered as post-hoc interpretation.

8. Robustness & Sensitivity

Robustness and sensitivity analysis
Fig 5 — Left: Bootstrap per-machine sep (mean ± std, 300 replicas with replacement). Centre: Global ROC-AUC bootstrap CI₉₅. Right: min(sep) distribution under ±20% coefficient perturbation (sensitivity, 300 replicas). All min > 0; all ROC CI₉₅ > 0.5.

A. Bootstrap Robustness (shot-level resampling, 300 replicas)

MetricMeanStdCI 2.5%CI 97.5%
min(sep)0.94050.23380.37301.2108
Global ROC-AUC0.98200.00140.97890.9845

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.

B. Sensitivity (coefficients ±20%, 300 replicas)

MetricMeanStdMinMax
min(sep)1.04430.09300.85831.2541
Global ROC-AUC0.98180.00110.97940.9842

PASS min(sep) stays in [0.858, 1.254] (always > 0) under ±20% coefficient perturbation. The formula is insensitive to moderate coefficient variation.

9. Role of inZOR-ND in This Discovery

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.

10. Complete Formula Hierarchy

FormulaTermsmin(sep)Global ROCRole
−kurtosis10.5810.965Nucleus only (historical reference)
−kurtosis + rate_ratio20.6800.9862F precursor (2D law-space attractor)
−kurtosis + cv_ratio20.9490.9692F C-Mod variant
−kurtosis + 0.80·rate_ratio + 0.65·cv_ratio31.0710.982★ Main law candidate
5D extended51.060.801Extended robustness variant
6D frozen elite61.260.791Maximum performance variant

11. Data, Code & Reproducibility

Data used: MAST (Mega Amp Spherical Tokamak), C-Mod (Alcator C-Mod / Zindi competition), HL-2A — all open/public datasets in HDF5 format.
Code: All scripts available in problems/fusion_disruption/ of the inZOR-ND repository.
PDF: Preprint v1 (Zenodo)  ·  Extended report (law candidate)
# Reproduce all validation results: python3 run_dual_instability_law_test.py # formula + temporal η(t) python3 run_priority_tests.py # LOMO + per-machine structural python3 run_robustness_sensitivity.py # bootstrap + sensitivity python3 run_baseline_ablation_test.py # ablation comparison python3 generate_publication_figures.py # all publication figures

Convention: D = 450 samples ending at t_disrupt − 50 ms; N = full shot. Same convention across all tests.

Disclaimer: This study uses empirical data from 3 tokamaks. Real-time deployment, transfer to unseen machines (EAST, JET, ITER), and physics-based validation would require additional diagnostics, engineering tests, and collaboration with tokamak operators. This work is intended as a scientific baseline and inZOR-ND capability demonstration.

12. Conclusion

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:

η ≈ −kurtosis + 0.80 · rate_ratio + 0.65 · cv_ratio

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.