ChaosBench-Logic Ontology
Overview
This document defines the formal ontology used in ChaosBench-Logic: a 27-predicate logical ontology (15 core predicates plus structural extensions) and the First-Order Logic (FOL) axioms that govern their relationships.
Core Predicate Set (15)
Each dynamical system in ChaosBench-Logic is characterized by a predicate inventory that includes a core 15-predicate set plus additional structural predicates used for extended reasoning. The original 11 predicates (1-11) are required for system eligibility; the 4 extension predicates (12-15) were added in v2 for deeper reasoning chains. The full 27-predicate inventory is defined in chaosbench/logic/ontology.py.
1. Chaotic
Definition: The system exhibits deterministic chaos — long-term unpredictable behavior arising from sensitive dependence on initial conditions, despite being governed by deterministic equations.
Formal properties:
- Has positive Lyapunov exponent
- Exhibits sensitive dependence on initial conditions
- Deterministic (not stochastic)
- Aperiodic dynamics
Example: Lorenz-63 system, Hénon map, logistic map at r=4
2. Deterministic
Definition: The system's future state is uniquely determined by its current state and the governing equations, with no random or stochastic components.
Formal properties:
- Evolution described by deterministic equations (ODEs, maps, PDEs)
- No noise terms or random variables
- Same initial conditions always produce the same trajectory
Example: All non-stochastic ODEs, discrete maps without noise
Counter-example: Ornstein-Uhlenbeck process (has stochastic term)
3. PosLyap (Positive Lyapunov Exponent)
Definition: The system has at least one positive Lyapunov exponent, meaning nearby trajectories diverge exponentially on average.
Formal properties:
- Largest Lyapunov exponent λ₁ > 0
- Quantifies exponential divergence rate: d(t) ≈ d₀ e^(λ₁t)
Example: Lorenz-63 (λ₁ ≈ 0.9), Hénon map (λ₁ ≈ 0.42)
Note: Positive Lyapunov exponent is necessary but not sufficient for chaos (needs bounded dynamics).
4. Sensitive (Sensitive Dependence on Initial Conditions)
Definition: Arbitrarily small differences in initial conditions lead to large differences in trajectories after sufficient time.
Formal properties:
- Related to positive Lyapunov exponent
- Makes long-term prediction impossible in practice
- Butterfly effect
Example: Weather systems, double pendulum
5. StrangeAttr (Strange Attractor)
Definition: The system's long-term behavior is confined to an attractor with fractal structure and non-integer dimension.
Formal properties:
- Fractal dimension (not integer)
- Self-similar structure at different scales
- Bounded in phase space
- Attracts nearby trajectories
Example: Lorenz attractor (dimension ≈ 2.06), Hénon attractor
Note: Strange attractor is sufficient but not necessary for chaos. Some chaotic systems lack attractors (e.g., Arnold cat map is area-preserving).
6. PointUnpredictable (Pointwise Unpredictable)
Definition: Precise point prediction of the system state at a specific future time is impossible beyond a finite horizon, even with arbitrarily accurate initial conditions.
Formal properties:
- Due to sensitive dependence and finite-precision measurements
- Lyapunov time: τ = 1/λ₁ (time scale for losing one bit of information)
- Individual trajectories cannot be predicted long-term
Example: Weather (can't predict specific temperature two weeks ahead)
7. StatPredictable (Statistically Predictable)
Definition: While individual trajectories are unpredictable, statistical properties (ensemble averages, distributions, moments) remain predictable over long times.
Formal properties:
- Ergodicity: time averages equal ensemble averages
- Invariant measure and attractor statistics are stable
- Climate vs. weather distinction
Example: Can predict average summer temperature (climate) but not specific day's weather
Note: Chaotic systems are pointwise unpredictable but statistically predictable.
8. QuasiPeriodic
Definition: The system exhibits motion that is almost periodic but never exactly repeats, typically characterized by multiple incommensurate frequencies.
Formal properties:
- Dynamics on a torus in phase space
- Multiple independent frequencies: ω₁, ω₂, ..., ωₙ
- Ratios ωᵢ/ωⱼ are irrational (incommensurate)
- All Lyapunov exponents are zero or negative
Example: Circle map (quasiperiodic regime), coupled oscillators with incommensurate frequencies
Counter-example: Chaotic systems (not quasiperiodic)
9. Random (Stochastic)
Definition: The system includes intrinsic randomness or noise in its governing equations.
Formal properties:
- Contains stochastic terms (Wiener process, random variables)
- Described by stochastic differential equations (SDEs)
- Multiple realizations from same initial conditions differ
Example: Ornstein-Uhlenbeck process, Brownian motion, systems with thermal noise
Counter-example: All deterministic systems
10. FixedPointAttr (Fixed-Point Attractor)
Definition: The system's long-term behavior converges to a single equilibrium point in phase space.
Formal properties:
- Attractor is a 0-dimensional point
- All trajectories approach the fixed point asymptotically
- All Lyapunov exponents are negative
- Stable equilibrium
Example: Damped harmonic oscillator, systems below bifurcation threshold
Counter-example: Chaotic, periodic, or quasiperiodic systems
11. Periodic
Definition: The system exhibits perfectly repeating behavior with a fixed period.
Formal properties:
- Attractor is a closed orbit (limit cycle)
- State returns exactly to starting point after period T
- One Lyapunov exponent is zero, others negative
- All Lyapunov exponents ≤ 0
Example: Limit cycles, periodic orbits in maps, undamped harmonic oscillator
Counter-example: Chaotic or quasiperiodic systems
12. Dissipative
Definition: The system's phase space volume contracts over time (div(v) < 0).
Formal properties:
- Volume contraction → trajectories converge to lower-dimensional attractor
- Distinguishes dissipative chaos from Hamiltonian (conservative) chaos
Example: Lorenz system (dissipative), Rössler system, Hénon map (area-contracting)
Counter-example: Standard map (conservative/area-preserving), Arnold cat map
13. Bounded
Definition: All trajectories remain in a bounded region of phase space.
Formal properties:
- Attractors are bounded by definition
- Statistical predictability requires bounded ensemble
- Required for physical realizability of chaotic dynamics
Example: Lorenz system (bounded attractor), logistic map (bounded on [0,1])
14. Mixing
Definition: The system has the strong mixing property: correlation functions decay to zero.
Formal properties:
- Mixing is stronger than ergodicity (mixing ⊂ ergodic)
- Essential for statistical mechanics interpretation of chaos
- Hyperbolic chaotic systems typically exhibit mixing
Example: Lorenz system, Arnold cat map (hyperbolic mixing)
Counter-example: Periodic orbits, quasi-periodic tori
15. Ergodic
Definition: Time averages along typical trajectories equal ensemble averages (Birkhoff ergodic theorem).
Formal properties:
- Foundation of statistical mechanics
- Weaker than mixing but essential for statistical predictability
- Enables long-time statistical forecasting
Example: Lorenz system (ergodic on attractor), quasi-periodic torus
Counter-example: Periodic orbits, multi-attractor systems
First-Order Logic (FOL) Axioms
The predicates are not independent — they obey logical constraints formalized as FOL axioms.
Axiom Structure
Each axiom has two components:
- Requires: If predicate A is true, these predicates must also be true
- Excludes: If predicate A is true, these predicates must be false
Axiom 1: Chaotic Systems
Chaotic(s) → Deterministic(s) ∧ PosLyap(s) ∧ Sensitive(s) ∧ PointUnpredictable(s) ∧ StatPredictable(s)
Chaotic(s) → ¬Random(s) ∧ ¬Periodic(s) ∧ ¬QuasiPeriodic(s) ∧ ¬FixedPointAttr(s)
Interpretation: Chaos requires determinism, positive Lyapunov exponent, sensitivity, pointwise unpredictability, and statistical predictability. Chaos excludes randomness, periodicity, quasiperiodicity, and fixed-point attractors.
Design choice: StrangeAttr is not in the requires list because strange attractors are sufficient but not necessary for chaos (e.g., Arnold cat map is chaotic without an attractor).
Axiom 2: Random Systems
Random(s) → ¬Deterministic(s) ∧ ¬Chaotic(s) ∧ ¬QuasiPeriodic(s) ∧ ¬Periodic(s)
Interpretation: Stochastic systems are not deterministic and cannot be chaotic, quasiperiodic, or periodic (which require determinism).
Axiom 3: QuasiPeriodic Systems
QuasiPeriodic(s) → Deterministic(s)
QuasiPeriodic(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬Periodic(s) ∧ ¬FixedPointAttr(s)
Interpretation: Quasiperiodicity requires determinism and excludes chaos, randomness, periodicity, and fixed-point attractors.
Axiom 4: Periodic Systems
Periodic(s) → Deterministic(s)
Periodic(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬QuasiPeriodic(s) ∧ ¬StrangeAttr(s)
Interpretation: Periodicity requires determinism and excludes chaos, randomness, quasiperiodicity, and strange attractors.
Axiom 5: Fixed-Point Attractors
FixedPointAttr(s) → Deterministic(s)
FixedPointAttr(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬QuasiPeriodic(s) ∧ ¬Periodic(s) ∧ ¬StrangeAttr(s)
Interpretation: Fixed-point attractors require determinism and exclude chaos, randomness, quasiperiodicity, periodicity, and strange attractors.
Axiom 6: Deterministic Systems
Deterministic(s) → ¬Random(s)
Interpretation: Determinism and randomness are mutually exclusive.
Design Choices & Rationale
1. Unidirectional Implications
Axioms are one-way implications. For example:
Chaotic → Deterministic(chaos implies determinism)- But NOT:
Deterministic → Chaotic(determinism doesn't imply chaos)
Rationale: Many deterministic systems are not chaotic (e.g., simple harmonic motion).
2. StrangeAttr Not Required for Chaos
StrangeAttr is not in the requires list for Chaotic.
Rationale:
- Strange attractors are sufficient for chaos (if you have a strange attractor, the system is chaotic)
- But they are not necessary (some chaotic systems lack attractors)
- Example: Arnold cat map is chaotic but area-preserving (no attractor)
This design allows the ontology to handle both dissipative and conservative chaotic systems.
3. Symmetric Exclusions
If A excludes B, then B excludes A. For example:
Chaotic → ¬RandomRandom → ¬Chaotic
Rationale: Exclusion is inherently symmetric. This ensures logical consistency.
4. Incomplete Specification
The axioms specify necessary conditions and exclusions but do not fully constrain all relationships.
Example: Deterministic has no requires list (only excludes Random). A deterministic system could be:
- Chaotic (Lorenz)
- Periodic (limit cycle)
- Quasiperiodic (torus)
- Fixed-point (damped oscillator)
Rationale: This reflects the mathematical reality — determinism alone doesn't determine the type of dynamics.
Validation & Consistency
Logical Consistency Checks
The evaluation pipeline (eval_chaosbench.py) checks model predictions against these axioms to detect FOL violations.
Example violation:
Model predicts: Chaotic=YES, Deterministic=NO
Violation: Chaotic → Deterministic
This is counted as a logical inconsistency even if the model doesn't contradict itself (didn't give both YES and NO to the same question).
Ground Truth Assignment
Each system in systems/*.json has a truth_assignment field with boolean values for the predicates (11 core required, 4 extension optional):
{
"system_id": "lorenz63",
"truth_assignment": {
"Chaotic": true,
"Deterministic": true,
"PosLyap": true,
"Sensitive": true,
"StrangeAttr": true,
"PointUnpredictable": true,
"StatPredictable": true,
"QuasiPeriodic": false,
"Random": false,
"FixedPointAttr": false,
"Periodic": false
}
}
All truth assignments are verified to satisfy the FOL axioms.
Predicate Extraction from Questions
The evaluation pipeline maps natural language questions to predicates using keyword matching:
| Keywords | Predicate |
|---|---|
| "chaotic", "chaos" | Chaotic |
| "deterministic" | Deterministic |
| "positive lyapunov", "lyapunov exponent" | PosLyap |
| "sensitive dependence", "sensitivity" | Sensitive |
| "strange attractor" | StrangeAttr |
| "pointwise prediction", "point-wise predictable" | PointUnpredictable |
| "statistically predictable", "statistical prediction" | StatPredictable |
| "quasi-periodic", "quasiperiodic" | QuasiPeriodic |
| "random", "randomness", "stochastic" | Random |
| "fixed point", "fixedpoint" | FixedPointAttr |
| "periodic" | Periodic |
| "dissipative", "volume-contracting" | Dissipative |
| "bounded", "bounded attractor" | Bounded |
| "mixing", "topological mixing" | Mixing |
| "ergodic", "ergodicity" | Ergodic |
See chaosbench/logic/ontology.py:KEYWORD_MAP for implementation.
Example System Definitions
Chaotic System: Lorenz-63
{
"system_id": "lorenz63",
"name": "Lorenz-63 system",
"category": "chaotic",
"equations": "dx/dt = σ (y - x); dy/dt = x (ρ - z) - y; dz/dt = x y - β z",
"parameters": {
"sigma": 10.0,
"rho": 28.0,
"beta": 2.6666666667
},
"truth_assignment": {
"Chaotic": true,
"Deterministic": true,
"PosLyap": true,
"Sensitive": true,
"StrangeAttr": true,
"PointUnpredictable": true,
"StatPredictable": true,
"QuasiPeriodic": false,
"Random": false,
"FixedPointAttr": false,
"Periodic": false
}
}
Satisfies: All Chaotic axioms — deterministic, positive Lyapunov, sensitive, etc.
Stochastic System: Ornstein-Uhlenbeck Process
{
"system_id": "stochastic_ou",
"name": "Ornstein-Uhlenbeck process",
"category": "stochastic",
"equations": "dX = θ(μ - X)dt + σ dW",
"truth_assignment": {
"Random": true,
"Deterministic": false,
"Chaotic": false,
"PosLyap": false,
"Sensitive": false,
"StrangeAttr": false,
"PointUnpredictable": false,
"StatPredictable": false,
"QuasiPeriodic": false,
"FixedPointAttr": false,
"Periodic": false
}
}
Satisfies: Random axioms — not deterministic, not chaotic, etc.
QuasiPeriodic System: Circle Map
{
"system_id": "circle_map_quasiperiodic",
"name": "Circle map (quasiperiodic regime)",
"category": "quasiperiodic",
"equations": "θₙ₊₁ = θₙ + Ω - (K/2π) sin(2π θₙ) mod 1",
"truth_assignment": {
"QuasiPeriodic": true,
"Deterministic": true,
"Chaotic": false,
"Random": false,
"PosLyap": false,
"Sensitive": false,
"StrangeAttr": false,
"PointUnpredictable": false,
"StatPredictable": false,
"FixedPointAttr": false,
"Periodic": false
}
}
Satisfies: QuasiPeriodic axioms — deterministic but not chaotic, periodic, or random.
References
- Chaos Theory: Strogatz, S. H. (2015). Nonlinear Dynamics and Chaos. Westview Press.
- Lyapunov Exponents: Wolf, A., et al. (1985). "Determining Lyapunov exponents from a time series." Physica D.
- Strange Attractors: Ott, E. (2002). Chaos in Dynamical Systems. Cambridge University Press.
- Ergodic Theory: Walters, P. (1982). An Introduction to Ergodic Theory. Springer.
Citation
If you use this ontology in your research, please cite:
@software{thomas2025chaosbench,
author = {Thomas, Noel},
title = {ChaosBench-Logic: A Benchmark for Evaluating Large Language Models on Complex Reasoning about Dynamical Systems},
year = {2025},
url = {https://github.com/11NOel11/ChaosBench-Logic}
}
Contact
For questions about the ontology or to report errors:
- Open an issue on GitHub
- Contact: Noel Thomas (MBZUAI)