Upload training_validation/fdra_oscillators_with_routing.py with huggingface_hub
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training_validation/fdra_oscillators_with_routing.py
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| 1 |
+
"""
|
| 2 |
+
FDRA Oscillator Implementation with Explicit Decay Parameters
|
| 3 |
+
|
| 4 |
+
This implements the core FDRA oscillator dynamics where each oscillator has:
|
| 5 |
+
- A decay parameter λ_i ∈ (0, 1)
|
| 6 |
+
- Half-life τ_i = ln(0.5) / ln(λ_i)
|
| 7 |
+
|
| 8 |
+
The key problem this addresses (from Melanie/Tiago's discovery):
|
| 9 |
+
- During training at GPT-2 scale, all λ_i collapse to near 1.0 (very short half-lives)
|
| 10 |
+
- This means oscillators only attend to ~10 tokens instead of full context length
|
| 11 |
+
- The model works for short-context tasks but fails on long-context reasoning
|
| 12 |
+
|
| 13 |
+
Solution: Half-life regularization to maintain diversity across temporal scales.
|
| 14 |
+
|
| 15 |
+
Authors: FDRA Half-Life Regularization Implementation
|
| 16 |
+
Date: 2026-01-22
|
| 17 |
+
"""
|
| 18 |
+
|
| 19 |
+
import numpy as np
|
| 20 |
+
from typing import Dict, List, Tuple, Optional, Any
|
| 21 |
+
from dataclasses import dataclass
|
| 22 |
+
import json
|
| 23 |
+
from pathlib import Path
|
| 24 |
+
|
| 25 |
+
|
| 26 |
+
@dataclass
|
| 27 |
+
class OscillatorConfig:
|
| 28 |
+
"""Configuration for FDRA oscillator bank."""
|
| 29 |
+
num_oscillators: int = 32 # Number of oscillators
|
| 30 |
+
state_dim: int = 16 # Dimension per oscillator
|
| 31 |
+
sequence_length: int = 4096 # Max sequence length (L)
|
| 32 |
+
tau_min: float = 1.0 # Minimum half-life
|
| 33 |
+
tau_max: float = 4096.0 # Maximum half-life (typically = L)
|
| 34 |
+
|
| 35 |
+
# Initialization
|
| 36 |
+
init_method: str = "log_uniform" # "log_uniform" or "random"
|
| 37 |
+
|
| 38 |
+
|
| 39 |
+
@dataclass
|
| 40 |
+
class OscillatorState:
|
| 41 |
+
"""State of an oscillator bank."""
|
| 42 |
+
h: np.ndarray # Hidden states: (num_oscillators, state_dim)
|
| 43 |
+
lambdas: np.ndarray # Decay parameters: (num_oscillators,)
|
| 44 |
+
|
| 45 |
+
def copy(self) -> 'OscillatorState':
|
| 46 |
+
return OscillatorState(
|
| 47 |
+
h=self.h.copy(),
|
| 48 |
+
lambdas=self.lambdas.copy()
|
| 49 |
+
)
|
| 50 |
+
|
| 51 |
+
|
| 52 |
+
class FDRAOscillatorBank:
|
| 53 |
+
"""
|
| 54 |
+
FDRA Oscillator Bank with explicit decay parameters.
|
| 55 |
+
|
| 56 |
+
Each oscillator i has:
|
| 57 |
+
h_i(t+1) = λ_i * h_i(t) + u_i(t)
|
| 58 |
+
|
| 59 |
+
Where:
|
| 60 |
+
λ_i ∈ (0, 1) is the decay parameter
|
| 61 |
+
τ_i = ln(0.5) / ln(λ_i) is the half-life
|
| 62 |
+
|
| 63 |
+
Half-life interpretation:
|
| 64 |
+
τ_i = number of steps for oscillator state to decay to 50%
|
| 65 |
+
|
| 66 |
+
The goal of half-life regularization:
|
| 67 |
+
Maintain log-uniform distribution of τ_i across [τ_min, τ_max]
|
| 68 |
+
This ensures oscillators can attend to both short and long contexts.
|
| 69 |
+
"""
|
| 70 |
+
|
| 71 |
+
def __init__(self, config: OscillatorConfig):
|
| 72 |
+
self.config = config
|
| 73 |
+
self.n = config.num_oscillators
|
| 74 |
+
self.d = config.state_dim
|
| 75 |
+
self.L = config.sequence_length
|
| 76 |
+
|
| 77 |
+
# Initialize decay parameters
|
| 78 |
+
self.lambdas = self._init_lambdas()
|
| 79 |
+
|
| 80 |
+
# Initialize hidden states
|
| 81 |
+
self.h = np.zeros((self.n, self.d))
|
| 82 |
+
|
| 83 |
+
# Track history for analysis
|
| 84 |
+
self.history: List[Dict[str, Any]] = []
|
| 85 |
+
|
| 86 |
+
def _init_lambdas(self) -> np.ndarray:
|
| 87 |
+
"""
|
| 88 |
+
Initialize decay parameters λ_i.
|
| 89 |
+
|
| 90 |
+
For log-uniform half-lives, we want:
|
| 91 |
+
τ_i ~ LogUniform(τ_min, τ_max)
|
| 92 |
+
|
| 93 |
+
Since τ = ln(0.5) / ln(λ), we have:
|
| 94 |
+
λ = 0.5^(1/τ)
|
| 95 |
+
|
| 96 |
+
So for log-uniform τ:
|
| 97 |
+
log(τ) ~ Uniform(log(τ_min), log(τ_max))
|
| 98 |
+
τ = exp(log_τ)
|
| 99 |
+
λ = 0.5^(1/τ)
|
| 100 |
+
"""
|
| 101 |
+
if self.config.init_method == "log_uniform":
|
| 102 |
+
# Log-uniform distribution of half-lives
|
| 103 |
+
log_tau_min = np.log(self.config.tau_min)
|
| 104 |
+
log_tau_max = np.log(self.config.tau_max)
|
| 105 |
+
|
| 106 |
+
# Evenly spaced in log space
|
| 107 |
+
log_taus = np.linspace(log_tau_min, log_tau_max, self.n)
|
| 108 |
+
taus = np.exp(log_taus)
|
| 109 |
+
|
| 110 |
+
# Convert half-lives to decay parameters
|
| 111 |
+
# λ = exp(ln(0.5) / τ) = 0.5^(1/τ)
|
| 112 |
+
lambdas = np.power(0.5, 1.0 / taus)
|
| 113 |
+
|
| 114 |
+
else:
|
| 115 |
+
# Random initialization (not recommended)
|
| 116 |
+
lambdas = np.random.uniform(0.5, 0.99, self.n)
|
| 117 |
+
|
| 118 |
+
return lambdas
|
| 119 |
+
|
| 120 |
+
def get_half_lives(self) -> np.ndarray:
|
| 121 |
+
"""
|
| 122 |
+
Compute half-lives from decay parameters.
|
| 123 |
+
|
| 124 |
+
τ_i = ln(0.5) / ln(λ_i)
|
| 125 |
+
"""
|
| 126 |
+
# Clamp lambdas to avoid log(1) = 0
|
| 127 |
+
safe_lambdas = np.clip(self.lambdas, 1e-10, 1.0 - 1e-10)
|
| 128 |
+
taus = np.log(0.5) / np.log(safe_lambdas)
|
| 129 |
+
return taus
|
| 130 |
+
|
| 131 |
+
def get_log_half_lives(self) -> np.ndarray:
|
| 132 |
+
"""Get log of half-lives: z_i = log(τ_i)."""
|
| 133 |
+
return np.log(self.get_half_lives())
|
| 134 |
+
|
| 135 |
+
def forward(self, u: np.ndarray) -> np.ndarray:
|
| 136 |
+
"""
|
| 137 |
+
One step of oscillator dynamics.
|
| 138 |
+
|
| 139 |
+
h_i(t+1) = λ_i * h_i(t) + u_i(t)
|
| 140 |
+
|
| 141 |
+
Args:
|
| 142 |
+
u: Input signal, shape (num_oscillators, state_dim)
|
| 143 |
+
|
| 144 |
+
Returns:
|
| 145 |
+
Updated hidden states, shape (num_oscillators, state_dim)
|
| 146 |
+
"""
|
| 147 |
+
# Broadcast lambdas across state dimensions
|
| 148 |
+
lambdas_broadcast = self.lambdas[:, np.newaxis] # (n, 1)
|
| 149 |
+
|
| 150 |
+
# Apply dynamics
|
| 151 |
+
self.h = lambdas_broadcast * self.h + u
|
| 152 |
+
|
| 153 |
+
return self.h.copy()
|
| 154 |
+
|
| 155 |
+
def reset(self):
|
| 156 |
+
"""Reset oscillator states to zero."""
|
| 157 |
+
self.h = np.zeros((self.n, self.d))
|
| 158 |
+
|
| 159 |
+
def get_half_life_statistics(self) -> Dict[str, float]:
|
| 160 |
+
"""
|
| 161 |
+
Compute statistics of half-life distribution.
|
| 162 |
+
|
| 163 |
+
Returns:
|
| 164 |
+
Dictionary with mean, std, min, max in log space.
|
| 165 |
+
"""
|
| 166 |
+
taus = self.get_half_lives()
|
| 167 |
+
z = np.log(taus)
|
| 168 |
+
|
| 169 |
+
return {
|
| 170 |
+
"tau_min": float(np.min(taus)),
|
| 171 |
+
"tau_max": float(np.max(taus)),
|
| 172 |
+
"tau_mean": float(np.mean(taus)),
|
| 173 |
+
"tau_median": float(np.median(taus)),
|
| 174 |
+
"log_tau_mean": float(np.mean(z)),
|
| 175 |
+
"log_tau_std": float(np.std(z)),
|
| 176 |
+
"log_tau_min": float(np.min(z)),
|
| 177 |
+
"log_tau_max": float(np.max(z)),
|
| 178 |
+
}
|
| 179 |
+
|
| 180 |
+
def get_state(self) -> OscillatorState:
|
| 181 |
+
"""Get current oscillator state."""
|
| 182 |
+
return OscillatorState(
|
| 183 |
+
h=self.h.copy(),
|
| 184 |
+
lambdas=self.lambdas.copy()
|
| 185 |
+
)
|
| 186 |
+
|
| 187 |
+
def set_state(self, state: OscillatorState):
|
| 188 |
+
"""Set oscillator state."""
|
| 189 |
+
self.h = state.h.copy()
|
| 190 |
+
self.lambdas = state.lambdas.copy()
|
| 191 |
+
|
| 192 |
+
|
| 193 |
+
class FDRAWithOscillators:
|
| 194 |
+
"""
|
| 195 |
+
Full FDRA agent with oscillator bank for memory.
|
| 196 |
+
|
| 197 |
+
This extends the basic FDRA agent to use an oscillator bank
|
| 198 |
+
with explicit decay parameters that can be regularized.
|
| 199 |
+
|
| 200 |
+
Architecture:
|
| 201 |
+
Input → [Oscillator Bank] → Slow State → Output
|
| 202 |
+
↑ ↓
|
| 203 |
+
Fast State ←──────────────
|
| 204 |
+
|
| 205 |
+
Routing Modes (validated in routing ablation):
|
| 206 |
+
- "uniform": Equal weight to all oscillators (baseline)
|
| 207 |
+
- "tau_weighted": Weight ∝ τ (soft routing to slow modes)
|
| 208 |
+
- "tau_gated": Only write to τ > threshold oscillators
|
| 209 |
+
"""
|
| 210 |
+
|
| 211 |
+
def __init__(
|
| 212 |
+
self,
|
| 213 |
+
osc_config: Optional[OscillatorConfig] = None,
|
| 214 |
+
wlc_threshold: float = 1.0,
|
| 215 |
+
routing_mode: str = "uniform" # "uniform", "tau_weighted", or "tau_gated"
|
| 216 |
+
):
|
| 217 |
+
self.config = osc_config or OscillatorConfig()
|
| 218 |
+
self.oscillators = FDRAOscillatorBank(self.config)
|
| 219 |
+
self.wlc_threshold = wlc_threshold
|
| 220 |
+
self.routing_mode = routing_mode
|
| 221 |
+
|
| 222 |
+
# Routing config
|
| 223 |
+
self.routing_min = 0.25 # Minimum routing weight
|
| 224 |
+
self.routing_max = 4.0 # Maximum routing weight
|
| 225 |
+
self.gating_threshold = 0.25 # Fraction of L for gating threshold
|
| 226 |
+
|
| 227 |
+
# Fast state (reactive, for computation)
|
| 228 |
+
self.fast = np.zeros(self.config.state_dim)
|
| 229 |
+
|
| 230 |
+
# Energy tracking
|
| 231 |
+
self.energy = 0.0
|
| 232 |
+
|
| 233 |
+
self.history: List[Dict[str, Any]] = []
|
| 234 |
+
|
| 235 |
+
def _compute_routing_weights(self) -> np.ndarray:
|
| 236 |
+
"""
|
| 237 |
+
Compute routing weights based on routing mode.
|
| 238 |
+
|
| 239 |
+
Returns:
|
| 240 |
+
Routing weights, shape (num_oscillators,)
|
| 241 |
+
"""
|
| 242 |
+
taus = self.oscillators.get_half_lives()
|
| 243 |
+
|
| 244 |
+
if self.routing_mode == "uniform":
|
| 245 |
+
# Equal weight to all oscillators
|
| 246 |
+
return np.ones(self.config.num_oscillators)
|
| 247 |
+
|
| 248 |
+
elif self.routing_mode == "tau_weighted":
|
| 249 |
+
# Weight ∝ τ, normalized by mean
|
| 250 |
+
weights = taus / np.mean(taus)
|
| 251 |
+
# Clamp for stability
|
| 252 |
+
weights = np.clip(weights, self.routing_min, self.routing_max)
|
| 253 |
+
return weights
|
| 254 |
+
|
| 255 |
+
elif self.routing_mode == "tau_gated":
|
| 256 |
+
# Hard gating: only oscillators with τ > threshold
|
| 257 |
+
threshold = self.gating_threshold * self.config.sequence_length
|
| 258 |
+
mask = (taus > threshold).astype(float)
|
| 259 |
+
if np.sum(mask) == 0:
|
| 260 |
+
# Fallback to uniform if no oscillators pass
|
| 261 |
+
return np.ones(self.config.num_oscillators)
|
| 262 |
+
# Normalize so total weight is same as uniform
|
| 263 |
+
return mask * (self.config.num_oscillators / np.sum(mask))
|
| 264 |
+
|
| 265 |
+
else:
|
| 266 |
+
raise ValueError(f"Unknown routing mode: {self.routing_mode}")
|
| 267 |
+
|
| 268 |
+
def get_slow_state(self) -> np.ndarray:
|
| 269 |
+
"""
|
| 270 |
+
Aggregate slow state from oscillator bank.
|
| 271 |
+
|
| 272 |
+
The slow state is a weighted sum of oscillator states,
|
| 273 |
+
with weights proportional to half-life.
|
| 274 |
+
"""
|
| 275 |
+
taus = self.oscillators.get_half_lives()
|
| 276 |
+
weights = taus / np.sum(taus) # Normalize
|
| 277 |
+
|
| 278 |
+
# Weighted sum across oscillators
|
| 279 |
+
weighted_h = self.oscillators.h * weights[:, np.newaxis]
|
| 280 |
+
slow = np.sum(weighted_h, axis=0) # (state_dim,)
|
| 281 |
+
|
| 282 |
+
return slow
|
| 283 |
+
|
| 284 |
+
def forward_dynamics(self, action: np.ndarray) -> np.ndarray:
|
| 285 |
+
"""
|
| 286 |
+
Forward dynamics with oscillator bank.
|
| 287 |
+
|
| 288 |
+
1. Compute routing weights based on mode
|
| 289 |
+
2. Distribute action across oscillators (weighted by routing)
|
| 290 |
+
3. Update oscillator bank
|
| 291 |
+
4. Compute slow state from oscillators
|
| 292 |
+
5. Update fast state
|
| 293 |
+
"""
|
| 294 |
+
# Compute routing weights (the key change for τ-routing)
|
| 295 |
+
routing_weights = self._compute_routing_weights() # (n,)
|
| 296 |
+
|
| 297 |
+
# Distribute action to oscillators WITH ROUTING WEIGHTS
|
| 298 |
+
u = np.tile(action, (self.config.num_oscillators, 1)) # (n, d)
|
| 299 |
+
|
| 300 |
+
# Apply routing weights (scale each oscillator's input by its weight)
|
| 301 |
+
u = u * routing_weights[:, np.newaxis] # (n, d)
|
| 302 |
+
|
| 303 |
+
# Scale by base factor
|
| 304 |
+
u = u * 0.1
|
| 305 |
+
|
| 306 |
+
# Update oscillators
|
| 307 |
+
self.oscillators.forward(u)
|
| 308 |
+
|
| 309 |
+
# Get slow state from oscillators
|
| 310 |
+
slow = self.get_slow_state()
|
| 311 |
+
|
| 312 |
+
# Update fast state (reactive)
|
| 313 |
+
self.fast = 0.9 * self.fast + action
|
| 314 |
+
|
| 315 |
+
# Energy
|
| 316 |
+
self.energy += np.linalg.norm(action) * 0.1
|
| 317 |
+
|
| 318 |
+
return slow
|
| 319 |
+
|
| 320 |
+
def get_coherence(self) -> float:
|
| 321 |
+
"""Coherence between slow and fast states."""
|
| 322 |
+
slow = self.get_slow_state()
|
| 323 |
+
slow_norm = np.linalg.norm(slow)
|
| 324 |
+
fast_norm = np.linalg.norm(self.fast)
|
| 325 |
+
|
| 326 |
+
if slow_norm < 1e-10 or fast_norm < 1e-10:
|
| 327 |
+
return 0.0
|
| 328 |
+
|
| 329 |
+
return float(np.dot(slow, self.fast) / (slow_norm * fast_norm))
|
| 330 |
+
|
| 331 |
+
def step(self, action: np.ndarray) -> Dict[str, Any]:
|
| 332 |
+
"""Execute one step and return diagnostics."""
|
| 333 |
+
slow = self.forward_dynamics(action)
|
| 334 |
+
coherence = self.get_coherence()
|
| 335 |
+
|
| 336 |
+
stats = self.oscillators.get_half_life_statistics()
|
| 337 |
+
|
| 338 |
+
result = {
|
| 339 |
+
"slow_norm": float(np.linalg.norm(slow)),
|
| 340 |
+
"fast_norm": float(np.linalg.norm(self.fast)),
|
| 341 |
+
"coherence": coherence,
|
| 342 |
+
"energy": self.energy,
|
| 343 |
+
**stats
|
| 344 |
+
}
|
| 345 |
+
|
| 346 |
+
self.history.append(result)
|
| 347 |
+
return result
|
| 348 |
+
|
| 349 |
+
def reset(self):
|
| 350 |
+
"""Reset all state."""
|
| 351 |
+
self.oscillators.reset()
|
| 352 |
+
self.fast = np.zeros(self.config.state_dim)
|
| 353 |
+
self.energy = 0.0
|
| 354 |
+
self.history = []
|
| 355 |
+
|
| 356 |
+
|
| 357 |
+
def demo_oscillators():
|
| 358 |
+
"""Demonstrate oscillator bank behavior."""
|
| 359 |
+
print("=" * 60)
|
| 360 |
+
print("FDRA OSCILLATOR BANK DEMONSTRATION")
|
| 361 |
+
print("=" * 60)
|
| 362 |
+
|
| 363 |
+
config = OscillatorConfig(
|
| 364 |
+
num_oscillators=16,
|
| 365 |
+
state_dim=8,
|
| 366 |
+
sequence_length=4096,
|
| 367 |
+
tau_min=1.0,
|
| 368 |
+
tau_max=4096.0
|
| 369 |
+
)
|
| 370 |
+
|
| 371 |
+
bank = FDRAOscillatorBank(config)
|
| 372 |
+
|
| 373 |
+
print("\n1. Initial Half-Life Distribution")
|
| 374 |
+
print("-" * 40)
|
| 375 |
+
stats = bank.get_half_life_statistics()
|
| 376 |
+
print(f" τ range: [{stats['tau_min']:.1f}, {stats['tau_max']:.1f}]")
|
| 377 |
+
print(f" τ mean: {stats['tau_mean']:.1f}")
|
| 378 |
+
print(f" log(τ) mean: {stats['log_tau_mean']:.3f}")
|
| 379 |
+
print(f" log(τ) std: {stats['log_tau_std']:.3f}")
|
| 380 |
+
|
| 381 |
+
print("\n2. Half-Lives per Oscillator")
|
| 382 |
+
print("-" * 40)
|
| 383 |
+
taus = bank.get_half_lives()
|
| 384 |
+
for i, tau in enumerate(taus):
|
| 385 |
+
bar = "█" * int(np.log(tau) * 3)
|
| 386 |
+
print(f" Osc {i:2d}: τ = {tau:7.1f} steps {bar}")
|
| 387 |
+
|
| 388 |
+
print("\n3. Simulating Input Sequence")
|
| 389 |
+
print("-" * 40)
|
| 390 |
+
|
| 391 |
+
# Pulse input at t=0
|
| 392 |
+
u = np.random.randn(config.num_oscillators, config.state_dim)
|
| 393 |
+
bank.forward(u)
|
| 394 |
+
initial_norms = np.linalg.norm(bank.h, axis=1)
|
| 395 |
+
|
| 396 |
+
# Decay for 100 steps with zero input
|
| 397 |
+
decay_steps = [10, 50, 100, 500, 1000]
|
| 398 |
+
zero_input = np.zeros((config.num_oscillators, config.state_dim))
|
| 399 |
+
|
| 400 |
+
step = 0
|
| 401 |
+
for target in decay_steps:
|
| 402 |
+
while step < target:
|
| 403 |
+
bank.forward(zero_input)
|
| 404 |
+
step += 1
|
| 405 |
+
|
| 406 |
+
current_norms = np.linalg.norm(bank.h, axis=1)
|
| 407 |
+
retention = current_norms / (initial_norms + 1e-10)
|
| 408 |
+
|
| 409 |
+
print(f"\n After {step} steps:")
|
| 410 |
+
for i, (tau, ret) in enumerate(zip(taus, retention)):
|
| 411 |
+
if tau < step * 0.5:
|
| 412 |
+
expected = "✗ (should be < 50%)"
|
| 413 |
+
else:
|
| 414 |
+
expected = "✓ (should be > 50%)"
|
| 415 |
+
print(f" Osc {i:2d}: τ={tau:7.1f}, retention={ret:.1%} {expected}")
|
| 416 |
+
if i >= 3:
|
| 417 |
+
print(f" ... ({len(taus) - 4} more)")
|
| 418 |
+
break
|
| 419 |
+
|
| 420 |
+
print("\n" + "=" * 60)
|
| 421 |
+
print("OBSERVATION: Oscillators with τ > t retain more than 50% of signal")
|
| 422 |
+
print("This is the desired behavior for long-context modeling.")
|
| 423 |
+
print("=" * 60)
|
| 424 |
+
|
| 425 |
+
|
| 426 |
+
if __name__ == "__main__":
|
| 427 |
+
demo_oscillators()
|