Free SKILL.md scraped from GitHub. Clone the repo or copy the file directly into your Claude Code skills directory.
npx versuz@latest install hiyenwong-ai-collection-collection-skills-kuramoto-oscillatory-phase-encodinggit clone https://github.com/hiyenwong/ai_collection.gitcp ai_collection/SKILL.MD ~/.claude/skills/hiyenwong-ai-collection-collection-skills-kuramoto-oscillatory-phase-encoding/SKILL.md---
name: kuramoto-oscillatory-phase-encoding
description: "Kuramoto Oscillatory Phase Encoding for Vision Transformers - neuro-inspired synchronization-based phase encoding that mimics biological oscillatory neural dynamics. Uses Kuramoto model to encode spatial information through phase relationships for efficient vision transformers. Activation: kuramoto phase encoding, oscillatory encoding, vision transformer phase, biological synchronization, neural oscillator encoding."
---
# Kuramoto Oscillatory Phase Encoding for Vision Transformers
> Kuramoto Oscillatory Phase Encoding (KOPE) - neuro-inspired approach using coupled oscillator synchronization dynamics to encode spatial information through phase relationships in Vision Transformers, achieving biological plausibility and computational efficiency.
## Metadata
- **Source**: arXiv:2604.07904v1
- **Authors**: Vision and neuroscience research team
- **Published**: 2026-04-09
- **Category**: Computer Vision, Neuroscience-Inspired AI, Vision Transformers
## Core Methodology
### Key Innovation
Traditional positional encodings in Vision Transformers rely on static sinusoidal functions or learned embeddings, lacking biological plausibility and dynamic adaptability. KOPE introduces:
1. **Biologically-grounded encoding**: Mimics oscillatory synchronization patterns observed in neural populations
2. **Dynamic phase relationships**: Coupled oscillators naturally encode relative spatial positions through phase differences
3. **Emergent spatial structure**: Global synchronization patterns emerge from local oscillator interactions
### Technical Framework
#### Kuramoto Model for Spatial Encoding
The Kuramoto model describes synchronization in coupled oscillators:
```
dθᵢ/dt = ωᵢ + Σⱼ Kᵢⱼ sin(θⱼ - θᵢ)
```
Where:
- θᵢ: Phase of oscillator at spatial position i
- ωᵢ: Natural frequency
- Kᵢⱼ: Coupling strength between positions i and j
#### Vision Transformer Integration
**Phase Encoding Layer**:
```python
class KuramotoPhaseEncoding(nn.Module):
def __init__(self, num_patches, embed_dim, coupling_strength=1.0):
super().__init__()
self.num_patches = num_patches
self.embed_dim = embed_dim
self.grid_size = int(num_patches ** 0.5)
# Natural frequencies (learnable per patch)
self.omega = nn.Parameter(torch.randn(num_patches, embed_dim))
# Coupling matrix based on spatial proximity
self.K = self._build_coupling_matrix(coupling_strength)
# Initial phases
self.theta_0 = nn.Parameter(torch.zeros(num_patches, embed_dim))
def _build_coupling_matrix(self, strength):
"""Build spatial coupling based on 2D grid distance"""
positions = torch.arange(self.num_patches)
row = positions // self.grid_size
col = positions % self.grid_size
# Pairwise distances
dist = ((row.unsqueeze(1) - row.unsqueeze(0)) ** 2 +
(col.unsqueeze(1) - col.unsqueeze(0)) ** 2) ** 0.5
# Gaussian coupling: stronger for nearby patches
K = strength * torch.exp(-dist / (self.grid_size / 2))
return K
def forward(self, x):
"""
x: [batch, num_patches, embed_dim]
Returns: phase-encoded features
"""
batch_size = x.shape[0]
# Solve Kuramoto dynamics (simplified: assume steady state)
# In practice, use iterative solver or analytical approximation
theta = self._solve_kuramoto(batch_size)
# Encode position via phase
phase_encoding = torch.cos(theta) + 1j * torch.sin(theta)
# Combine with patch embeddings
return x * phase_encoding.real + x * phase_encoding.imag * 0.1
def _solve_kuramoto(self, batch_size):
"""Iterative solver for Kuramoto steady state"""
theta = self.theta_0.unsqueeze(0).expand(batch_size, -1, -1)
omega = self.omega.unsqueeze(0).expand(batch_size, -1, -1)
# Fixed-point iteration
for _ in range(10): # convergence steps
# Compute phase differences
dtheta = theta.unsqueeze(2) - theta.unsqueeze(1) # [B, N, N, D]
# Coupling term
coupling = (self.K.unsqueeze(-1) * torch.sin(dtheta)).sum(dim=1)
# Update
theta = theta + 0.1 * (omega + coupling)
return theta
```
**Multi-Frequency Encoding**:
```python
class MultiFrequencyKuramotoEncoding(nn.Module):
"""Multiple frequency bands for rich phase representation"""
def __init__(self, num_patches, embed_dim, n_bands=4):
super().__init__()
self.n_bands = n_bands
assert embed_dim % n_bands == 0
self.dim_per_band = embed_dim // n_bands
self.encoders = nn.ModuleList([
KuramotoPhaseEncoding(num_patches, self.dim_per_band)
for _ in range(n_bands)
])
# Different base frequencies for each band
for i, encoder in enumerate(self.encoders):
encoder.omega.data = encoder.omega.data * (2 ** i)
def forward(self, x):
# Split into frequency bands
x_bands = x.chunk(self.n_bands, dim=-1)
# Apply band-specific encoding
encoded = [enc(xb) for enc, xb in zip(self.encoders, x_bands)]
# Concatenate
return torch.cat(encoded, dim=-1)
```
#### Attention with Phase-Aware Position
```python
class PhaseAwareAttention(nn.Module):
"""Self-attention incorporating phase-based position encoding"""
def __init__(self, embed_dim, num_heads):
super().__init__()
self.num_heads = num_heads
self.head_dim = embed_dim // num_heads
self.scale = self.head_dim ** -0.5
self.qkv = nn.Linear(embed_dim, embed_dim * 3)
self.proj = nn.Linear(embed_dim, embed_dim)
# Phase coupling in attention
self.phase_attention = KuramotoPhaseEncoding(
num_patches=196, # for 14x14 patches
embed_dim=self.head_dim
)
def forward(self, x):
B, N, C = x.shape
# Standard QKV
qkv = self.qkv(x).reshape(B, N, 3, self.num_heads, self.head_dim)
qkv = qkv.permute(2, 0, 3, 1, 4) # [3, B, H, N, D]
q, k, v = qkv[0], qkv[1], qkv[2]
# Phase encoding
q_phase = self.phase_attention(q)
k_phase = self.phase_attention(k)
# Attention with phase
attn = (q_phase @ k_phase.transpose(-2, -1)) * self.scale
attn = attn.softmax(dim=-1)
x = (attn @ v).transpose(1, 2).reshape(B, N, C)
x = self.proj(x)
return x
```
## Implementation Guide
### Prerequisites
- PyTorch 2.0+
- NumPy for oscillator dynamics
- einops for tensor manipulation
### Step-by-Step
1. **Patch Embedding with KOPE**
```python
class KOPETokenizer(nn.Module):
def __init__(self, img_size=224, patch_size=16, embed_dim=768):
super().__init__()
self.patch_embed = nn.Conv2d(3, embed_dim, patch_size, patch_size)
num_patches = (img_size // patch_size) ** 2
self.position_encoding = KuramotoPhaseEncoding(
num_patches, embed_dim
)
def forward(self, x):
# Extract patches
x = self.patch_embed(x) # [B, embed_dim, H', W']
x = x.flatten(2).transpose(1, 2) # [B, N, embed_dim]
# Add KOPE
x = self.position_encoding(x)
return x
```
2. **Training Configuration**
```python
config = {
"model": {
"embed_dim": 768,
"depth": 12,
"num_heads": 12,
"patch_size": 16,
"img_size": 224
},
"kuramoto": {
"coupling_strength": 1.0,
"convergence_steps": 10,
"frequency_bands": 4
},
"training": {
"learning_rate": 1e-3,
"weight_decay": 0.05,
"warmup_epochs": 5
}
}
```
3. **Efficiency Optimizations**
```python
class EfficientKuramotoSolver:
"""Approximate fast solver for Kuramoto steady state"""
@staticmethod
def analytical_approximation(omega, K, iterations=5):
"""
Fast approximation using mean-field assumption
Assumes all oscillators synchronize to mean phase
"""
N = omega.shape[0]
# Mean field order parameter
r = torch.ones(N, 1) * 0.5 # initial coherence
psi = torch.zeros(N, 1) # mean phase
for _ in range(iterations):
# Update order parameter
r_new = torch.abs((r * torch.exp(1j * psi)).mean())
psi_new = torch.angle((r * torch.exp(1j * psi)).mean())
# Update local phases
local_phase = torch.atan2(omega, K.sum(dim=1, keepdim=True) * r_new)
theta = psi_new + local_phase
r = r_new.expand_as(r)
psi = theta
return theta
```
### Code Example: Complete KOPE-ViT
```python
class KOPEVisionTransformer(nn.Module):
"""
Vision Transformer with Kuramoto Oscillatory Phase Encoding
"""
def __init__(
self,
img_size=224,
patch_size=16,
embed_dim=768,
depth=12,
num_heads=12,
mlp_ratio=4.0,
num_classes=1000
):
super().__init__()
self.patch_size = patch_size
self.num_patches = (img_size // patch_size) ** 2
# Patch embedding
self.patch_embed = nn.Conv2d(
3, embed_dim, kernel_size=patch_size, stride=patch_size
)
# KOPE position encoding
self.pos_encoding = MultiFrequencyKuramotoEncoding(
num_patches=self.num_patches,
embed_dim=embed_dim,
n_bands=4
)
# Transformer blocks
self.blocks = nn.ModuleList([
PhaseAwareTransformerBlock(
embed_dim=embed_dim,
num_heads=num_heads,
mlp_ratio=mlp_ratio
)
for _ in range(depth)
])
# Classification head
self.norm = nn.LayerNorm(embed_dim)
self.head = nn.Linear(embed_dim, num_classes)
def forward(self, x):
# Patch embedding
x = self.patch_embed(x)
x = x.flatten(2).transpose(1, 2) # [B, N, embed_dim]
# Add KOPE
x = self.pos_encoding(x)
# Transformer layers
for block in self.blocks:
x = block(x)
# Classification
x = self.norm(x.mean(dim=1)) # Global average pooling
x = self.head(x)
return x
```
## Applications
- **Vision Transformers with Biological Plausibility**: Image classification with neuroscience-inspired position encoding
- **Oscillatory Neural Networks**: Building networks that mimic brain oscillation patterns
- **Spatial Reasoning Tasks**: Tasks requiring understanding of relative spatial positions
- **Multi-Scale Feature Learning**: Multiple frequency bands capture different spatial scales
## Pitfalls
- **Convergence Speed**: Kuramoto solver requires iterative computation; approximation needed for efficiency
- **Hyperparameter Sensitivity**: Coupling strength and frequency bands need careful tuning
- **Limited Long-Range**: Kuramoto coupling favors local synchronization
- **Computational Cost**: Phase dynamics more expensive than static positional encodings
## Related Skills
- kuramoto-brain-network
- brain-inspired-attention-mechanisms
- adaptive-spiking-neuron-asn
- vision-smolmamba-token-pruning
## References
```bibtex
@article{kope2026,
title={Kuramoto Oscillatory Phase Encoding: Neuro-inspired Synchronization for Vision Transformers},
author={[Authors]},
journal={arXiv preprint arXiv:2604.07904},
year={2026}
}
```