| # ChaosBench-Logic Ontology |
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| ## Overview |
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| 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. |
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| --- |
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| ## Core Predicate Set (15) |
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| 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`. |
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| ### 1. Chaotic |
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| **Definition:** The system exhibits deterministic chaos — long-term unpredictable behavior arising from sensitive dependence on initial conditions, despite being governed by deterministic equations. |
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| **Formal properties:** |
| - Has positive Lyapunov exponent |
| - Exhibits sensitive dependence on initial conditions |
| - Deterministic (not stochastic) |
| - Aperiodic dynamics |
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| **Example:** Lorenz-63 system, Hénon map, logistic map at r=4 |
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| --- |
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| ### 2. Deterministic |
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| **Definition:** The system's future state is uniquely determined by its current state and the governing equations, with no random or stochastic components. |
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| **Formal properties:** |
| - Evolution described by deterministic equations (ODEs, maps, PDEs) |
| - No noise terms or random variables |
| - Same initial conditions always produce the same trajectory |
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| **Example:** All non-stochastic ODEs, discrete maps without noise |
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| **Counter-example:** Ornstein-Uhlenbeck process (has stochastic term) |
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| --- |
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| ### 3. PosLyap (Positive Lyapunov Exponent) |
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| **Definition:** The system has at least one positive Lyapunov exponent, meaning nearby trajectories diverge exponentially on average. |
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| **Formal properties:** |
| - Largest Lyapunov exponent λ₁ > 0 |
| - Quantifies exponential divergence rate: d(t) ≈ d₀ e^(λ₁t) |
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| **Example:** Lorenz-63 (λ₁ ≈ 0.9), Hénon map (λ₁ ≈ 0.42) |
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| **Note:** Positive Lyapunov exponent is necessary but not sufficient for chaos (needs bounded dynamics). |
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| --- |
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| ### 4. Sensitive (Sensitive Dependence on Initial Conditions) |
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| **Definition:** Arbitrarily small differences in initial conditions lead to large differences in trajectories after sufficient time. |
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| **Formal properties:** |
| - Related to positive Lyapunov exponent |
| - Makes long-term prediction impossible in practice |
| - Butterfly effect |
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| **Example:** Weather systems, double pendulum |
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| --- |
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| ### 5. StrangeAttr (Strange Attractor) |
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| **Definition:** The system's long-term behavior is confined to an attractor with fractal structure and non-integer dimension. |
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| **Formal properties:** |
| - Fractal dimension (not integer) |
| - Self-similar structure at different scales |
| - Bounded in phase space |
| - Attracts nearby trajectories |
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| **Example:** Lorenz attractor (dimension ≈ 2.06), Hénon attractor |
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| **Note:** Strange attractor is *sufficient* but *not necessary* for chaos. Some chaotic systems lack attractors (e.g., Arnold cat map is area-preserving). |
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| --- |
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| ### 6. PointUnpredictable (Pointwise Unpredictable) |
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| **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. |
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| **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 |
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| **Example:** Weather (can't predict specific temperature two weeks ahead) |
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| --- |
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| ### 7. StatPredictable (Statistically Predictable) |
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| **Definition:** While individual trajectories are unpredictable, statistical properties (ensemble averages, distributions, moments) remain predictable over long times. |
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| **Formal properties:** |
| - Ergodicity: time averages equal ensemble averages |
| - Invariant measure and attractor statistics are stable |
| - Climate vs. weather distinction |
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| **Example:** Can predict average summer temperature (climate) but not specific day's weather |
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| **Note:** Chaotic systems are pointwise unpredictable but statistically predictable. |
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| --- |
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| ### 8. QuasiPeriodic |
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| **Definition:** The system exhibits motion that is almost periodic but never exactly repeats, typically characterized by multiple incommensurate frequencies. |
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| **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 |
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| **Example:** Circle map (quasiperiodic regime), coupled oscillators with incommensurate frequencies |
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| **Counter-example:** Chaotic systems (not quasiperiodic) |
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| --- |
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| ### 9. Random (Stochastic) |
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| **Definition:** The system includes intrinsic randomness or noise in its governing equations. |
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| **Formal properties:** |
| - Contains stochastic terms (Wiener process, random variables) |
| - Described by stochastic differential equations (SDEs) |
| - Multiple realizations from same initial conditions differ |
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| **Example:** Ornstein-Uhlenbeck process, Brownian motion, systems with thermal noise |
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| **Counter-example:** All deterministic systems |
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| --- |
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| ### 10. FixedPointAttr (Fixed-Point Attractor) |
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| **Definition:** The system's long-term behavior converges to a single equilibrium point in phase space. |
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| **Formal properties:** |
| - Attractor is a 0-dimensional point |
| - All trajectories approach the fixed point asymptotically |
| - All Lyapunov exponents are negative |
| - Stable equilibrium |
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| **Example:** Damped harmonic oscillator, systems below bifurcation threshold |
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| **Counter-example:** Chaotic, periodic, or quasiperiodic systems |
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| --- |
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| ### 11. Periodic |
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| **Definition:** The system exhibits perfectly repeating behavior with a fixed period. |
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| **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 |
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| **Example:** Limit cycles, periodic orbits in maps, undamped harmonic oscillator |
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| **Counter-example:** Chaotic or quasiperiodic systems |
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| --- |
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| ### 12. Dissipative |
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| **Definition:** The system's phase space volume contracts over time (div(v) < 0). |
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| **Formal properties:** |
| - Volume contraction → trajectories converge to lower-dimensional attractor |
| - Distinguishes dissipative chaos from Hamiltonian (conservative) chaos |
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| **Example:** Lorenz system (dissipative), Rössler system, Hénon map (area-contracting) |
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| **Counter-example:** Standard map (conservative/area-preserving), Arnold cat map |
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| --- |
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| ### 13. Bounded |
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| **Definition:** All trajectories remain in a bounded region of phase space. |
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| **Formal properties:** |
| - Attractors are bounded by definition |
| - Statistical predictability requires bounded ensemble |
| - Required for physical realizability of chaotic dynamics |
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| **Example:** Lorenz system (bounded attractor), logistic map (bounded on [0,1]) |
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| --- |
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| ### 14. Mixing |
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| **Definition:** The system has the strong mixing property: correlation functions decay to zero. |
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| **Formal properties:** |
| - Mixing is stronger than ergodicity (mixing ⊂ ergodic) |
| - Essential for statistical mechanics interpretation of chaos |
| - Hyperbolic chaotic systems typically exhibit mixing |
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| **Example:** Lorenz system, Arnold cat map (hyperbolic mixing) |
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| **Counter-example:** Periodic orbits, quasi-periodic tori |
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| --- |
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| ### 15. Ergodic |
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| **Definition:** Time averages along typical trajectories equal ensemble averages (Birkhoff ergodic theorem). |
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| **Formal properties:** |
| - Foundation of statistical mechanics |
| - Weaker than mixing but essential for statistical predictability |
| - Enables long-time statistical forecasting |
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| **Example:** Lorenz system (ergodic on attractor), quasi-periodic torus |
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| **Counter-example:** Periodic orbits, multi-attractor systems |
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| --- |
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| ## First-Order Logic (FOL) Axioms |
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| The predicates are not independent — they obey logical constraints formalized as FOL axioms. |
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| ### Axiom Structure |
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| 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 |
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| ### Axiom 1: Chaotic Systems |
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| ``` |
| Chaotic(s) → Deterministic(s) ∧ PosLyap(s) ∧ Sensitive(s) ∧ PointUnpredictable(s) ∧ StatPredictable(s) |
| Chaotic(s) → ¬Random(s) ∧ ¬Periodic(s) ∧ ¬QuasiPeriodic(s) ∧ ¬FixedPointAttr(s) |
| ``` |
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| **Interpretation:** Chaos requires determinism, positive Lyapunov exponent, sensitivity, pointwise unpredictability, and statistical predictability. Chaos excludes randomness, periodicity, quasiperiodicity, and fixed-point attractors. |
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| **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). |
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| --- |
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| ### Axiom 2: Random Systems |
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| ``` |
| Random(s) → ¬Deterministic(s) ∧ ¬Chaotic(s) ∧ ¬QuasiPeriodic(s) ∧ ¬Periodic(s) |
| ``` |
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| **Interpretation:** Stochastic systems are not deterministic and cannot be chaotic, quasiperiodic, or periodic (which require determinism). |
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| --- |
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| ### Axiom 3: QuasiPeriodic Systems |
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| ``` |
| QuasiPeriodic(s) → Deterministic(s) |
| QuasiPeriodic(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬Periodic(s) ∧ ¬FixedPointAttr(s) |
| ``` |
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| **Interpretation:** Quasiperiodicity requires determinism and excludes chaos, randomness, periodicity, and fixed-point attractors. |
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| --- |
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| ### Axiom 4: Periodic Systems |
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| ``` |
| Periodic(s) → Deterministic(s) |
| Periodic(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬QuasiPeriodic(s) ∧ ¬StrangeAttr(s) |
| ``` |
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| **Interpretation:** Periodicity requires determinism and excludes chaos, randomness, quasiperiodicity, and strange attractors. |
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| --- |
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| ### Axiom 5: Fixed-Point Attractors |
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| ``` |
| FixedPointAttr(s) → Deterministic(s) |
| FixedPointAttr(s) → ¬Chaotic(s) ∧ ¬Random(s) ∧ ¬QuasiPeriodic(s) ∧ ¬Periodic(s) ∧ ¬StrangeAttr(s) |
| ``` |
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| **Interpretation:** Fixed-point attractors require determinism and exclude chaos, randomness, quasiperiodicity, periodicity, and strange attractors. |
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| --- |
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| ### Axiom 6: Deterministic Systems |
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| ``` |
| Deterministic(s) → ¬Random(s) |
| ``` |
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| **Interpretation:** Determinism and randomness are mutually exclusive. |
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| --- |
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| ## Design Choices & Rationale |
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| ### 1. Unidirectional Implications |
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| Axioms are **one-way implications**. For example: |
| - `Chaotic → Deterministic` (chaos implies determinism) |
| - But NOT: `Deterministic → Chaotic` (determinism doesn't imply chaos) |
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| **Rationale:** Many deterministic systems are not chaotic (e.g., simple harmonic motion). |
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| --- |
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| ### 2. StrangeAttr Not Required for Chaos |
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| `StrangeAttr` is **not** in the `requires` list for `Chaotic`. |
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| **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) |
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| This design allows the ontology to handle both dissipative and conservative chaotic systems. |
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| --- |
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| ### 3. Symmetric Exclusions |
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| If A excludes B, then B excludes A. For example: |
| - `Chaotic → ¬Random` |
| - `Random → ¬Chaotic` |
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| **Rationale:** Exclusion is inherently symmetric. This ensures logical consistency. |
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| --- |
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| ### 4. Incomplete Specification |
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| The axioms specify **necessary conditions** and **exclusions** but do not fully constrain all relationships. |
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| **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) |
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| **Rationale:** This reflects the mathematical reality — determinism alone doesn't determine the type of dynamics. |
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| --- |
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| ## Validation & Consistency |
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| ### Logical Consistency Checks |
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| The evaluation pipeline (`eval_chaosbench.py`) checks model predictions against these axioms to detect **FOL violations**. |
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| Example violation: |
| ``` |
| Model predicts: Chaotic=YES, Deterministic=NO |
| Violation: Chaotic → Deterministic |
| ``` |
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| 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). |
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| ### Ground Truth Assignment |
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| Each system in `systems/*.json` has a `truth_assignment` field with boolean values for the predicates (11 core required, 4 extension optional): |
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| ```json |
| { |
| "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 |
| } |
| } |
| ``` |
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| All truth assignments are verified to satisfy the FOL axioms. |
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| --- |
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| ## Predicate Extraction from Questions |
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| The evaluation pipeline maps natural language questions to predicates using keyword matching: |
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| | 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` | |
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| See `chaosbench/logic/ontology.py:KEYWORD_MAP` for implementation. |
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| --- |
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| ## Example System Definitions |
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| ### Chaotic System: Lorenz-63 |
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| ```json |
| { |
| "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 |
| } |
| } |
| ``` |
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| **Satisfies:** All Chaotic axioms — deterministic, positive Lyapunov, sensitive, etc. |
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| --- |
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| ### Stochastic System: Ornstein-Uhlenbeck Process |
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| ```json |
| { |
| "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 |
| } |
| } |
| ``` |
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| **Satisfies:** Random axioms — not deterministic, not chaotic, etc. |
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| --- |
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| ### QuasiPeriodic System: Circle Map |
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| ```json |
| { |
| "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 |
| } |
| } |
| ``` |
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| **Satisfies:** QuasiPeriodic axioms — deterministic but not chaotic, periodic, or random. |
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| --- |
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| ## References |
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| 1. **Chaos Theory:** Strogatz, S. H. (2015). *Nonlinear Dynamics and Chaos*. Westview Press. |
| 2. **Lyapunov Exponents:** Wolf, A., et al. (1985). "Determining Lyapunov exponents from a time series." *Physica D*. |
| 3. **Strange Attractors:** Ott, E. (2002). *Chaos in Dynamical Systems*. Cambridge University Press. |
| 4. **Ergodic Theory:** Walters, P. (1982). *An Introduction to Ergodic Theory*. Springer. |
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| --- |
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| ## Citation |
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| If you use this ontology in your research, please cite: |
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| ```bibtex |
| @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} |
| } |
| ``` |
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| --- |
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| ## Contact |
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| For questions about the ontology or to report errors: |
| - Open an issue on [GitHub](https://github.com/11NOel11/ChaosBench-Logic/issues) |
| - Contact: Noel Thomas (MBZUAI) |
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