Create pytorch_compiled_kernel.py
Browse files- pytorch_compiled_kernel.py +1049 -0
pytorch_compiled_kernel.py
ADDED
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@@ -0,0 +1,1049 @@
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|
| 1 |
+
"""
|
| 2 |
+
CompiledEigh: torch.compile(fullgraph=True) drop-in for torch.linalg.eigh.
|
| 3 |
+
|
| 4 |
+
Eliminates all graph breaks, device-host syncs, and dynamic allocation.
|
| 5 |
+
Output contract matches torch.linalg.eigh:
|
| 6 |
+
eigenvalues: [*, n] real, ascending
|
| 7 |
+
eigenvectors: [*, n, n] orthonormal columns
|
| 8 |
+
|
| 9 |
+
Author: AbstractPhil / GeoLIP project
|
| 10 |
+
"""
|
| 11 |
+
|
| 12 |
+
import math
|
| 13 |
+
import torch
|
| 14 |
+
import torch.nn as nn
|
| 15 |
+
from torch import Tensor
|
| 16 |
+
from typing import Tuple, Optional
|
| 17 |
+
|
| 18 |
+
|
| 19 |
+
# =============================================================================
|
| 20 |
+
# Constants
|
| 21 |
+
# =============================================================================
|
| 22 |
+
|
| 23 |
+
DEFAULT_MAX_NEWTON: int = 8
|
| 24 |
+
DEFAULT_MAX_JACOBI_SWEEPS: int = 10 # 10 sweeps saturates for n <= 16
|
| 25 |
+
JACOBI_THRESHOLD: int = 16
|
| 26 |
+
|
| 27 |
+
|
| 28 |
+
# =============================================================================
|
| 29 |
+
# Atom: 2x2 Symmetric Eigenproblem
|
| 30 |
+
# =============================================================================
|
| 31 |
+
|
| 32 |
+
def eigh_2x2(a: Tensor, b: Tensor, c: Tensor, eps: float = 1e-30
|
| 33 |
+
) -> Tuple[Tensor, Tensor, Tensor, Tensor]:
|
| 34 |
+
"""
|
| 35 |
+
Closed-form eigendecomposition of batched 2x2 symmetric matrices.
|
| 36 |
+
Returns: (lambda1, lambda2, cos_theta, sin_theta), lambda1 <= lambda2.
|
| 37 |
+
"""
|
| 38 |
+
trace = a + c
|
| 39 |
+
diff = a - c
|
| 40 |
+
two_b = 2.0 * b
|
| 41 |
+
hyp = torch.sqrt(diff * diff + two_b * two_b + eps)
|
| 42 |
+
|
| 43 |
+
lambda1 = 0.5 * (trace - hyp)
|
| 44 |
+
lambda2 = 0.5 * (trace + hyp)
|
| 45 |
+
|
| 46 |
+
vx = two_b
|
| 47 |
+
vy = lambda2 - a
|
| 48 |
+
norm_v = torch.sqrt(vx * vx + vy * vy + eps)
|
| 49 |
+
cos_theta = vy / norm_v
|
| 50 |
+
sin_theta = vx / norm_v
|
| 51 |
+
|
| 52 |
+
return lambda1, lambda2, cos_theta, sin_theta
|
| 53 |
+
|
| 54 |
+
|
| 55 |
+
# =============================================================================
|
| 56 |
+
# Utility: Newton-Schulz Orthogonalization (all-bmm, GPU-native)
|
| 57 |
+
# =============================================================================
|
| 58 |
+
|
| 59 |
+
def orthogonalize_ns(V: Tensor, n_iter: int = 2) -> Tensor:
|
| 60 |
+
"""
|
| 61 |
+
Re-orthogonalize columns of V via Newton-Schulz iteration.
|
| 62 |
+
|
| 63 |
+
Computes V @ (V^T V)^{-1/2} using the coupled iteration:
|
| 64 |
+
X_0 = I, Y_0 = V^T V
|
| 65 |
+
X_{k+1} = 0.5 * X_k @ (3I - Y_k)
|
| 66 |
+
Y_{k+1} = 0.5 * (3I - Y_k) @ Y_k
|
| 67 |
+
|
| 68 |
+
X converges to (V^T V)^{-1/2}, Y converges to I.
|
| 69 |
+
Cubically convergent when V^T V β I.
|
| 70 |
+
|
| 71 |
+
Convergence from ||V^T V - I|| = Ξ΅:
|
| 72 |
+
1 iteration: error β O(Ρ²) β 1e-6 from 1e-3
|
| 73 |
+
2 iterations: error β O(Ξ΅β΄) β 1e-12 from 1e-3
|
| 74 |
+
|
| 75 |
+
All ops are bmm β fully compiled, no sequential column processing.
|
| 76 |
+
|
| 77 |
+
V: [B, n, n] (square, columns are approximate eigenvectors)
|
| 78 |
+
Returns: [B, n, n] with orthonormal columns
|
| 79 |
+
"""
|
| 80 |
+
B, n, m = V.shape
|
| 81 |
+
I_n = torch.eye(m, device=V.device, dtype=V.dtype).unsqueeze(0).expand(B, -1, -1)
|
| 82 |
+
|
| 83 |
+
# Z = V^T V β I
|
| 84 |
+
Y = torch.bmm(V.transpose(-2, -1), V)
|
| 85 |
+
X = I_n.clone()
|
| 86 |
+
|
| 87 |
+
for _ in range(n_iter):
|
| 88 |
+
T = 3.0 * I_n - Y # (3I - Y_k)
|
| 89 |
+
X = 0.5 * torch.bmm(X, T) # X_{k+1}
|
| 90 |
+
Y = 0.5 * torch.bmm(T, Y) # Y_{k+1}
|
| 91 |
+
|
| 92 |
+
return torch.bmm(V, X)
|
| 93 |
+
|
| 94 |
+
|
| 95 |
+
# =============================================================================
|
| 96 |
+
# Phase 1: Householder Tridiagonalization
|
| 97 |
+
# =============================================================================
|
| 98 |
+
|
| 99 |
+
class HouseholderTridiagonalizer(nn.Module):
|
| 100 |
+
"""
|
| 101 |
+
Reduces batched symmetric A to tridiagonal T = Q^T A Q via
|
| 102 |
+
Householder reflections. Fixed loop bounds, compilable.
|
| 103 |
+
"""
|
| 104 |
+
|
| 105 |
+
def __init__(self, max_n: int, eps: float = 1e-30):
|
| 106 |
+
super().__init__()
|
| 107 |
+
self.max_n = max_n
|
| 108 |
+
self.eps = eps
|
| 109 |
+
|
| 110 |
+
def forward(self, A: Tensor, d: Tensor, e: Tensor,
|
| 111 |
+
reflectors: Tensor) -> None:
|
| 112 |
+
B, n, _ = A.shape
|
| 113 |
+
eps = self.eps
|
| 114 |
+
|
| 115 |
+
for k in range(n - 2):
|
| 116 |
+
tail_len = n - k - 1
|
| 117 |
+
x = A[:, k + 1:, k].clone()
|
| 118 |
+
|
| 119 |
+
sigma = torch.sqrt((x * x).sum(dim=-1, keepdim=True) + eps)
|
| 120 |
+
sign_x0 = torch.where(x[:, 0:1] >= 0,
|
| 121 |
+
torch.ones_like(sigma),
|
| 122 |
+
-torch.ones_like(sigma))
|
| 123 |
+
alpha = -sign_x0 * sigma
|
| 124 |
+
|
| 125 |
+
v = x.clone()
|
| 126 |
+
v[:, 0:1] = v[:, 0:1] - alpha
|
| 127 |
+
v_norm = torch.sqrt((v * v).sum(dim=-1, keepdim=True) + eps)
|
| 128 |
+
v = v / v_norm
|
| 129 |
+
|
| 130 |
+
reflectors[k, :, :tail_len] = v
|
| 131 |
+
if tail_len < n:
|
| 132 |
+
reflectors[k, :, tail_len:] = 0.0
|
| 133 |
+
|
| 134 |
+
sub_A = A[:, k + 1:, k + 1:]
|
| 135 |
+
v_col = v.unsqueeze(-1)
|
| 136 |
+
|
| 137 |
+
p = torch.bmm(sub_A, v_col).squeeze(-1)
|
| 138 |
+
vtp = (v * p).sum(dim=-1, keepdim=True)
|
| 139 |
+
q = p - vtp * v
|
| 140 |
+
|
| 141 |
+
q_col = q.unsqueeze(-1)
|
| 142 |
+
q_row = q.unsqueeze(-2)
|
| 143 |
+
v_row = v.unsqueeze(-2)
|
| 144 |
+
|
| 145 |
+
A[:, k + 1:, k + 1:] -= 2.0 * (v_col @ q_row + q_col @ v_row)
|
| 146 |
+
A[:, k, k + 1] = alpha.squeeze(-1)
|
| 147 |
+
A[:, k + 1, k] = alpha.squeeze(-1)
|
| 148 |
+
|
| 149 |
+
for i in range(n):
|
| 150 |
+
d[:, i] = A[:, i, i]
|
| 151 |
+
for i in range(n - 1):
|
| 152 |
+
e[:, i] = A[:, i, i + 1]
|
| 153 |
+
|
| 154 |
+
|
| 155 |
+
# =============================================================================
|
| 156 |
+
# Phase 2a: Secular Equation Newton Solver (Fixed Budget)
|
| 157 |
+
# =============================================================================
|
| 158 |
+
|
| 159 |
+
class SecularNewtonSolver(nn.Module):
|
| 160 |
+
|
| 161 |
+
def __init__(self, max_newton: int = DEFAULT_MAX_NEWTON,
|
| 162 |
+
eps: float = 1e-30, tol: float = 1e-7):
|
| 163 |
+
super().__init__()
|
| 164 |
+
self.max_newton = max_newton
|
| 165 |
+
self.eps = eps
|
| 166 |
+
self.tol = tol
|
| 167 |
+
|
| 168 |
+
def forward(self, delta: Tensor, z_sq: Tensor,
|
| 169 |
+
rho: Tensor, mask: Tensor) -> Tensor:
|
| 170 |
+
B, m = delta.shape
|
| 171 |
+
eps = self.eps
|
| 172 |
+
tol = self.tol
|
| 173 |
+
|
| 174 |
+
z_sq_sum = (z_sq * mask).sum(dim=-1, keepdim=True)
|
| 175 |
+
rho_abs = rho.abs().unsqueeze(-1)
|
| 176 |
+
upper_bound = delta[:, -1:] + z_sq_sum * rho_abs + 1.0
|
| 177 |
+
|
| 178 |
+
lo = delta + eps
|
| 179 |
+
hi = torch.cat([delta[:, 1:], upper_bound], dim=-1) - eps
|
| 180 |
+
lam = 0.5 * (lo + hi)
|
| 181 |
+
rho_exp = rho.unsqueeze(-1)
|
| 182 |
+
|
| 183 |
+
for _step in range(self.max_newton):
|
| 184 |
+
delta_exp = delta.unsqueeze(-1)
|
| 185 |
+
lam_exp = lam.unsqueeze(-2)
|
| 186 |
+
denom = delta_exp - lam_exp
|
| 187 |
+
|
| 188 |
+
denom_safe = torch.where(
|
| 189 |
+
denom.abs() < eps,
|
| 190 |
+
torch.full_like(denom, eps) * denom.sign().clamp(min=0.5),
|
| 191 |
+
denom
|
| 192 |
+
)
|
| 193 |
+
|
| 194 |
+
z_sq_exp = z_sq.unsqueeze(-1)
|
| 195 |
+
mask_exp = mask.unsqueeze(-1)
|
| 196 |
+
masked_z = z_sq_exp * mask_exp
|
| 197 |
+
|
| 198 |
+
terms = masked_z / denom_safe
|
| 199 |
+
f = 1.0 + rho_exp * terms.sum(dim=-2)
|
| 200 |
+
f_prime = rho_exp * (masked_z / (denom_safe * denom_safe)).sum(dim=-2)
|
| 201 |
+
|
| 202 |
+
f_prime_safe = torch.where(
|
| 203 |
+
f_prime.abs() < eps,
|
| 204 |
+
torch.full_like(f_prime, eps),
|
| 205 |
+
f_prime
|
| 206 |
+
)
|
| 207 |
+
delta_lam = -f / f_prime_safe
|
| 208 |
+
lam_new = torch.clamp(lam + delta_lam, lo, hi)
|
| 209 |
+
|
| 210 |
+
f_pos = f > 0
|
| 211 |
+
lo = torch.where(f_pos & mask.bool(), lam, lo)
|
| 212 |
+
hi = torch.where(~f_pos & mask.bool(), lam, hi)
|
| 213 |
+
|
| 214 |
+
converged = (f.abs() < tol) | ~mask.bool()
|
| 215 |
+
lam = torch.where(converged, lam, lam_new)
|
| 216 |
+
|
| 217 |
+
return lam
|
| 218 |
+
|
| 219 |
+
|
| 220 |
+
# =============================================================================
|
| 221 |
+
# Phase 2b: Eigenvectors from Secular Equation
|
| 222 |
+
# =============================================================================
|
| 223 |
+
|
| 224 |
+
def secular_eigenvectors(delta: Tensor, lam: Tensor, z: Tensor,
|
| 225 |
+
mask: Tensor, eps: float = 1e-30) -> Tensor:
|
| 226 |
+
delta_exp = delta.unsqueeze(-1)
|
| 227 |
+
lam_exp = lam.unsqueeze(-2)
|
| 228 |
+
denom = delta_exp - lam_exp
|
| 229 |
+
|
| 230 |
+
denom_safe = torch.where(
|
| 231 |
+
denom.abs() < eps,
|
| 232 |
+
torch.full_like(denom, eps) * denom.sign().clamp(min=0.5),
|
| 233 |
+
denom
|
| 234 |
+
)
|
| 235 |
+
|
| 236 |
+
z_exp = z.unsqueeze(-1)
|
| 237 |
+
mask_exp = mask.unsqueeze(-1)
|
| 238 |
+
V = (z_exp * mask_exp) / denom_safe
|
| 239 |
+
col_norms = torch.sqrt((V * V).sum(dim=-2, keepdim=True) + eps)
|
| 240 |
+
V = V / col_norms
|
| 241 |
+
return V
|
| 242 |
+
|
| 243 |
+
|
| 244 |
+
# =============================================================================
|
| 245 |
+
# Phase 2c: Fixed-Depth Tensor Tree D&C
|
| 246 |
+
# =============================================================================
|
| 247 |
+
|
| 248 |
+
class TensorTreeDC(nn.Module):
|
| 249 |
+
|
| 250 |
+
def __init__(self, max_n: int,
|
| 251 |
+
max_newton: int = DEFAULT_MAX_NEWTON,
|
| 252 |
+
eps: float = 1e-30, tol: float = 1e-7):
|
| 253 |
+
super().__init__()
|
| 254 |
+
self.padded_n = 1 << math.ceil(math.log2(max(max_n, 2)))
|
| 255 |
+
self.depth = int(math.log2(self.padded_n))
|
| 256 |
+
self.max_n = max_n
|
| 257 |
+
self.eps = eps
|
| 258 |
+
self.secular_solver = SecularNewtonSolver(
|
| 259 |
+
max_newton=max_newton, eps=eps, tol=tol
|
| 260 |
+
)
|
| 261 |
+
|
| 262 |
+
def forward(self, d: Tensor, e: Tensor) -> Tuple[Tensor, Tensor]:
|
| 263 |
+
B, n = d.shape
|
| 264 |
+
pn = self.padded_n
|
| 265 |
+
eps = self.eps
|
| 266 |
+
device = d.device
|
| 267 |
+
dtype = d.dtype
|
| 268 |
+
|
| 269 |
+
if n < pn:
|
| 270 |
+
d_max = d.abs().max(dim=-1, keepdim=True).values + 1.0
|
| 271 |
+
pad_diag = d_max + torch.arange(1, pn - n + 1, device=device, dtype=dtype).unsqueeze(0)
|
| 272 |
+
d_padded = torch.cat([d, pad_diag], dim=-1)
|
| 273 |
+
e_padded = torch.zeros(B, pn - 1, device=device, dtype=dtype)
|
| 274 |
+
e_padded[:, :n - 1] = e
|
| 275 |
+
else:
|
| 276 |
+
d_padded = d.clone()
|
| 277 |
+
e_padded = e.clone()
|
| 278 |
+
|
| 279 |
+
# DOWNWARD PASS
|
| 280 |
+
coupling_rho = []
|
| 281 |
+
current_d = d_padded.clone()
|
| 282 |
+
current_e = e_padded.clone()
|
| 283 |
+
|
| 284 |
+
for level in range(self.depth):
|
| 285 |
+
num_sub = 2 ** level
|
| 286 |
+
sub_size = pn // num_sub
|
| 287 |
+
half = sub_size // 2
|
| 288 |
+
|
| 289 |
+
cd = current_d.reshape(B, num_sub, sub_size)
|
| 290 |
+
ce = current_e.reshape(B, num_sub, sub_size - 1)
|
| 291 |
+
|
| 292 |
+
rho = ce[:, :, half - 1].clone()
|
| 293 |
+
coupling_rho.append(rho)
|
| 294 |
+
|
| 295 |
+
cd[:, :, half - 1] = cd[:, :, half - 1] - rho.abs()
|
| 296 |
+
cd[:, :, half] = cd[:, :, half] - rho.abs()
|
| 297 |
+
ce[:, :, half - 1] = 0.0
|
| 298 |
+
|
| 299 |
+
left_d = cd[:, :, :half].reshape(B, num_sub * half)
|
| 300 |
+
right_d = cd[:, :, half:].reshape(B, num_sub * half)
|
| 301 |
+
current_d = torch.stack([left_d.reshape(B, num_sub, half),
|
| 302 |
+
right_d.reshape(B, num_sub, half)],
|
| 303 |
+
dim=2).reshape(B, pn)
|
| 304 |
+
|
| 305 |
+
left_e = ce[:, :, :half - 1].reshape(B, num_sub, half - 1)
|
| 306 |
+
right_e = ce[:, :, half:].reshape(B, num_sub, half - 1)
|
| 307 |
+
current_e = torch.stack([left_e, right_e], dim=2).reshape(
|
| 308 |
+
B, num_sub * 2 * (half - 1))
|
| 309 |
+
expected_e_len = pn - 1
|
| 310 |
+
if current_e.shape[-1] < expected_e_len:
|
| 311 |
+
current_e = torch.nn.functional.pad(
|
| 312 |
+
current_e, (0, expected_e_len - current_e.shape[-1]))
|
| 313 |
+
|
| 314 |
+
# BASE
|
| 315 |
+
base_evals = current_d
|
| 316 |
+
V_current = torch.ones(B, pn, 1, 1, device=device, dtype=dtype)
|
| 317 |
+
|
| 318 |
+
# UPWARD PASS
|
| 319 |
+
current_evals = base_evals
|
| 320 |
+
|
| 321 |
+
for level in range(self.depth - 1, -1, -1):
|
| 322 |
+
num_sub = 2 ** level
|
| 323 |
+
sub_size = pn // num_sub
|
| 324 |
+
half = sub_size // 2
|
| 325 |
+
child_size = half
|
| 326 |
+
|
| 327 |
+
evals_grouped = current_evals.reshape(B, num_sub, 2, child_size)
|
| 328 |
+
left_evals = evals_grouped[:, :, 0, :]
|
| 329 |
+
right_evals = evals_grouped[:, :, 1, :]
|
| 330 |
+
delta = torch.cat([left_evals, right_evals], dim=-1)
|
| 331 |
+
|
| 332 |
+
V_grouped = V_current.reshape(B, num_sub, 2, child_size, child_size)
|
| 333 |
+
V_left = V_grouped[:, :, 0, :, :]
|
| 334 |
+
V_right = V_grouped[:, :, 1, :, :]
|
| 335 |
+
|
| 336 |
+
z_left = V_left[:, :, -1, :]
|
| 337 |
+
z_right = V_right[:, :, 0, :]
|
| 338 |
+
z_cat = torch.cat([z_left, z_right], dim=-1)
|
| 339 |
+
|
| 340 |
+
delta_sorted, sort_idx = delta.sort(dim=-1)
|
| 341 |
+
z_sorted = z_cat.gather(-1, sort_idx)
|
| 342 |
+
|
| 343 |
+
rho = coupling_rho[level]
|
| 344 |
+
mask = torch.ones(B, num_sub, sub_size, device=device, dtype=dtype)
|
| 345 |
+
|
| 346 |
+
gaps = (delta_sorted[:, :, 1:] - delta_sorted[:, :, :-1]).abs()
|
| 347 |
+
degenerate = gaps < (eps * 100)
|
| 348 |
+
avg = 0.5 * (delta_sorted[:, :, :-1] + delta_sorted[:, :, 1:])
|
| 349 |
+
|
| 350 |
+
delta_defl = delta_sorted.clone()
|
| 351 |
+
delta_defl[:, :, :-1] = torch.where(degenerate, avg, delta_sorted[:, :, :-1])
|
| 352 |
+
delta_defl[:, :, 1:] = torch.where(degenerate, avg, delta_sorted[:, :, 1:])
|
| 353 |
+
|
| 354 |
+
z_defl = z_sorted.clone()
|
| 355 |
+
defl_kill = torch.ones_like(z_sorted)
|
| 356 |
+
defl_kill[:, :, 1:] = torch.where(
|
| 357 |
+
degenerate, torch.zeros_like(gaps), torch.ones_like(gaps))
|
| 358 |
+
z_defl = z_defl * defl_kill
|
| 359 |
+
|
| 360 |
+
z_sq = z_defl * z_defl
|
| 361 |
+
Bns = B * num_sub
|
| 362 |
+
new_evals_flat = self.secular_solver(
|
| 363 |
+
delta_defl.reshape(Bns, sub_size),
|
| 364 |
+
z_sq.reshape(Bns, sub_size),
|
| 365 |
+
rho.reshape(Bns),
|
| 366 |
+
mask.reshape(Bns, sub_size),
|
| 367 |
+
)
|
| 368 |
+
new_evals = new_evals_flat.reshape(B, num_sub, sub_size)
|
| 369 |
+
|
| 370 |
+
V_secular_flat = secular_eigenvectors(
|
| 371 |
+
delta_defl.reshape(Bns, sub_size),
|
| 372 |
+
new_evals_flat,
|
| 373 |
+
z_defl.reshape(Bns, sub_size),
|
| 374 |
+
mask.reshape(Bns, sub_size),
|
| 375 |
+
eps=eps
|
| 376 |
+
)
|
| 377 |
+
V_secular = V_secular_flat.reshape(B, num_sub, sub_size, sub_size)
|
| 378 |
+
|
| 379 |
+
inv_sort = sort_idx.argsort(dim=-1)
|
| 380 |
+
inv_exp = inv_sort.unsqueeze(-1).expand_as(V_secular)
|
| 381 |
+
V_unsorted = V_secular.gather(-2, inv_exp)
|
| 382 |
+
|
| 383 |
+
V_block = torch.zeros(B, num_sub, sub_size, sub_size,
|
| 384 |
+
device=device, dtype=dtype)
|
| 385 |
+
V_block[:, :, :half, :half] = V_left
|
| 386 |
+
V_block[:, :, half:, half:] = V_right
|
| 387 |
+
|
| 388 |
+
V_merged = torch.bmm(
|
| 389 |
+
V_block.reshape(Bns, sub_size, sub_size),
|
| 390 |
+
V_unsorted.reshape(Bns, sub_size, sub_size)
|
| 391 |
+
).reshape(B, num_sub, sub_size, sub_size)
|
| 392 |
+
|
| 393 |
+
current_evals = new_evals.reshape(B, pn)
|
| 394 |
+
V_current = V_merged
|
| 395 |
+
|
| 396 |
+
eigenvalues = current_evals
|
| 397 |
+
eigenvectors = V_current.squeeze(1)
|
| 398 |
+
|
| 399 |
+
sorted_evals, sort_perm = eigenvalues.sort(dim=-1)
|
| 400 |
+
sort_exp = sort_perm.unsqueeze(-2).expand_as(eigenvectors)
|
| 401 |
+
sorted_evecs = eigenvectors.gather(-1, sort_exp)
|
| 402 |
+
|
| 403 |
+
if n < pn:
|
| 404 |
+
sorted_evals = sorted_evals[:, :n]
|
| 405 |
+
sorted_evecs = sorted_evecs[:, :n, :n]
|
| 406 |
+
|
| 407 |
+
return sorted_evals, sorted_evecs
|
| 408 |
+
|
| 409 |
+
|
| 410 |
+
# =============================================================================
|
| 411 |
+
# Phase 2 (alternate): Jacobi for small n
|
| 412 |
+
# =============================================================================
|
| 413 |
+
|
| 414 |
+
class JacobiEigh(nn.Module):
|
| 415 |
+
"""
|
| 416 |
+
Jacobi eigenvalue algorithm for small symmetric matrices.
|
| 417 |
+
Fixed sweep count, fully vectorized, zero branches.
|
| 418 |
+
|
| 419 |
+
COMPILE FIX: Pair indices stored as plain Python lists (not tensors).
|
| 420 |
+
Dynamo sees these as constants β no SymInt issues.
|
| 421 |
+
"""
|
| 422 |
+
|
| 423 |
+
def __init__(self, max_n: int,
|
| 424 |
+
max_sweeps: int = DEFAULT_MAX_JACOBI_SWEEPS,
|
| 425 |
+
eps: float = 1e-30):
|
| 426 |
+
super().__init__()
|
| 427 |
+
self.max_n = max_n
|
| 428 |
+
self.max_sweeps = max_sweeps
|
| 429 |
+
self.eps = eps
|
| 430 |
+
|
| 431 |
+
# CRITICAL: plain Python lists, NOT registered buffers.
|
| 432 |
+
# Dynamo traces these as compile-time constants.
|
| 433 |
+
pairs = []
|
| 434 |
+
for p in range(max_n):
|
| 435 |
+
for q in range(p + 1, max_n):
|
| 436 |
+
pairs.append((p, q))
|
| 437 |
+
self._pairs_p: list[int] = [p for p, q in pairs]
|
| 438 |
+
self._pairs_q: list[int] = [q for p, q in pairs]
|
| 439 |
+
self._n_pairs: int = len(pairs)
|
| 440 |
+
|
| 441 |
+
def forward(self, A: Tensor) -> Tuple[Tensor, Tensor]:
|
| 442 |
+
"""
|
| 443 |
+
A: [B, n, n] symmetric
|
| 444 |
+
Returns: (eigenvalues [B, n] ascending, eigenvectors [B, n, n])
|
| 445 |
+
"""
|
| 446 |
+
B, n, _ = A.shape
|
| 447 |
+
eps = self.eps
|
| 448 |
+
|
| 449 |
+
W = A.clone()
|
| 450 |
+
V = torch.eye(n, device=A.device, dtype=A.dtype).unsqueeze(0).expand(B, -1, -1).clone()
|
| 451 |
+
|
| 452 |
+
for _sweep in range(self.max_sweeps):
|
| 453 |
+
for idx in range(self._n_pairs):
|
| 454 |
+
# Plain Python ints β Dynamo sees these as constants
|
| 455 |
+
p: int = self._pairs_p[idx]
|
| 456 |
+
q: int = self._pairs_q[idx]
|
| 457 |
+
|
| 458 |
+
app = W[:, p, p]
|
| 459 |
+
aqq = W[:, q, q]
|
| 460 |
+
apq = W[:, p, q]
|
| 461 |
+
|
| 462 |
+
# Givens rotation angle
|
| 463 |
+
two_apq = 2.0 * apq
|
| 464 |
+
diff = aqq - app
|
| 465 |
+
|
| 466 |
+
# Safe division: sign-preserving eps guard
|
| 467 |
+
abs_two_apq = two_apq.abs().clamp(min=eps)
|
| 468 |
+
sign_two_apq = torch.where(two_apq >= 0,
|
| 469 |
+
torch.ones_like(two_apq),
|
| 470 |
+
-torch.ones_like(two_apq))
|
| 471 |
+
tau = diff / (abs_two_apq * sign_two_apq)
|
| 472 |
+
|
| 473 |
+
tau_sign = torch.where(tau >= 0,
|
| 474 |
+
torch.ones_like(tau),
|
| 475 |
+
-torch.ones_like(tau))
|
| 476 |
+
t = tau_sign / (tau.abs() + torch.sqrt(1.0 + tau * tau))
|
| 477 |
+
|
| 478 |
+
# Zero rotation when off-diagonal is already negligible
|
| 479 |
+
skip = (apq.abs() < eps).float()
|
| 480 |
+
t = t * (1.0 - skip)
|
| 481 |
+
|
| 482 |
+
c = 1.0 / torch.sqrt(1.0 + t * t)
|
| 483 |
+
s = t * c
|
| 484 |
+
|
| 485 |
+
# ββ Rotate W columns p, q ββ
|
| 486 |
+
Wp = W[:, :, p].clone()
|
| 487 |
+
Wq = W[:, :, q].clone()
|
| 488 |
+
c_col = c.unsqueeze(-1)
|
| 489 |
+
s_col = s.unsqueeze(-1)
|
| 490 |
+
W[:, :, p] = c_col * Wp - s_col * Wq
|
| 491 |
+
W[:, :, q] = s_col * Wp + c_col * Wq
|
| 492 |
+
|
| 493 |
+
# ββ Rotate W rows p, q ββ
|
| 494 |
+
Wp = W[:, p, :].clone()
|
| 495 |
+
Wq = W[:, q, :].clone()
|
| 496 |
+
W[:, p, :] = c_col * Wp - s_col * Wq
|
| 497 |
+
W[:, q, :] = s_col * Wp + c_col * Wq
|
| 498 |
+
|
| 499 |
+
# ββ Exact diagonal repair (prevents accumulation drift) ββ
|
| 500 |
+
W[:, p, q] = 0.0
|
| 501 |
+
W[:, q, p] = 0.0
|
| 502 |
+
W[:, p, p] = app - t * apq
|
| 503 |
+
W[:, q, q] = aqq + t * apq
|
| 504 |
+
|
| 505 |
+
# ββ Accumulate eigenvectors ββ
|
| 506 |
+
Vp = V[:, :, p].clone()
|
| 507 |
+
Vq = V[:, :, q].clone()
|
| 508 |
+
V[:, :, p] = c_col * Vp - s_col * Vq
|
| 509 |
+
V[:, :, q] = s_col * Vp + c_col * Vq
|
| 510 |
+
|
| 511 |
+
# ββ Newton-Schulz re-orthogonalization ββ
|
| 512 |
+
# 2 iterations: orth error 1e-3 β ~1e-12 via bmm (GPU-native)
|
| 513 |
+
V = orthogonalize_ns(V, n_iter=2)
|
| 514 |
+
|
| 515 |
+
# ββ Extract and sort ββ
|
| 516 |
+
eigenvalues = torch.diagonal(W, dim1=-2, dim2=-1)
|
| 517 |
+
sorted_evals, sort_perm = eigenvalues.sort(dim=-1)
|
| 518 |
+
sort_exp = sort_perm.unsqueeze(-2).expand_as(V)
|
| 519 |
+
sorted_evecs = V.gather(-1, sort_exp)
|
| 520 |
+
|
| 521 |
+
return sorted_evals, sorted_evecs
|
| 522 |
+
|
| 523 |
+
|
| 524 |
+
# =============================================================================
|
| 525 |
+
# Phase 3: Householder Back-Accumulation
|
| 526 |
+
# =============================================================================
|
| 527 |
+
|
| 528 |
+
class HouseholderBackAccumulate(nn.Module):
|
| 529 |
+
|
| 530 |
+
def __init__(self, max_n: int, eps: float = 1e-30):
|
| 531 |
+
super().__init__()
|
| 532 |
+
self.max_n = max_n
|
| 533 |
+
self.eps = eps
|
| 534 |
+
|
| 535 |
+
def forward(self, reflectors: Tensor, Z: Tensor, n: int) -> Tensor:
|
| 536 |
+
V = Z.clone()
|
| 537 |
+
for k in range(n - 3, -1, -1):
|
| 538 |
+
tail_len = n - k - 1
|
| 539 |
+
v = reflectors[k, :, :tail_len]
|
| 540 |
+
v_col = v.unsqueeze(-1)
|
| 541 |
+
V_sub = V[:, k + 1:, :]
|
| 542 |
+
vtV = torch.bmm(v_col.transpose(-2, -1), V_sub)
|
| 543 |
+
V[:, k + 1:, :] = V_sub - 2.0 * v_col @ vtV
|
| 544 |
+
return V
|
| 545 |
+
|
| 546 |
+
|
| 547 |
+
# =============================================================================
|
| 548 |
+
# Validation
|
| 549 |
+
# =============================================================================
|
| 550 |
+
|
| 551 |
+
class EighValidator(nn.Module):
|
| 552 |
+
|
| 553 |
+
def forward(self, A: Tensor, eigenvalues: Tensor,
|
| 554 |
+
eigenvectors: Tensor) -> Tuple[Tensor, Tensor, Tensor]:
|
| 555 |
+
B, n, _ = A.shape
|
| 556 |
+
AV = torch.bmm(A, eigenvectors)
|
| 557 |
+
VL = eigenvectors * eigenvalues.unsqueeze(-2)
|
| 558 |
+
residual = AV - VL
|
| 559 |
+
A_norm = torch.linalg.norm(A.reshape(B, -1), dim=-1).clamp(min=1e-30)
|
| 560 |
+
residual_norm = torch.linalg.norm(residual.reshape(B, -1), dim=-1) / A_norm
|
| 561 |
+
|
| 562 |
+
VtV = torch.bmm(eigenvectors.transpose(-2, -1), eigenvectors)
|
| 563 |
+
I = torch.eye(n, device=A.device, dtype=A.dtype).unsqueeze(0)
|
| 564 |
+
orth_err = torch.linalg.norm((VtV - I).reshape(B, -1), dim=-1)
|
| 565 |
+
|
| 566 |
+
return residual_norm, orth_err, residual_norm.max()
|
| 567 |
+
|
| 568 |
+
|
| 569 |
+
# =============================================================================
|
| 570 |
+
# Top-Level: CompiledEigh
|
| 571 |
+
# =============================================================================
|
| 572 |
+
|
| 573 |
+
class CompiledEigh(nn.Module):
|
| 574 |
+
"""
|
| 575 |
+
Drop-in replacement for torch.linalg.eigh.
|
| 576 |
+
|
| 577 |
+
Usage:
|
| 578 |
+
solver = CompiledEigh(max_n=6)
|
| 579 |
+
solver = torch.compile(solver, fullgraph=True)
|
| 580 |
+
eigenvalues, eigenvectors = solver(A)
|
| 581 |
+
"""
|
| 582 |
+
|
| 583 |
+
def __init__(self, max_n: int,
|
| 584 |
+
use_jacobi: Optional[bool] = None,
|
| 585 |
+
max_newton: int = DEFAULT_MAX_NEWTON,
|
| 586 |
+
max_jacobi_sweeps: int = DEFAULT_MAX_JACOBI_SWEEPS,
|
| 587 |
+
eps: float = 1e-30, tol: float = 1e-7):
|
| 588 |
+
super().__init__()
|
| 589 |
+
self.max_n = max_n
|
| 590 |
+
self.eps = eps
|
| 591 |
+
|
| 592 |
+
if use_jacobi is None:
|
| 593 |
+
use_jacobi = (max_n <= JACOBI_THRESHOLD)
|
| 594 |
+
self.use_jacobi = use_jacobi
|
| 595 |
+
|
| 596 |
+
if use_jacobi:
|
| 597 |
+
self.jacobi = JacobiEigh(
|
| 598 |
+
max_n=max_n, max_sweeps=max_jacobi_sweeps, eps=eps)
|
| 599 |
+
else:
|
| 600 |
+
self.tridiag = HouseholderTridiagonalizer(max_n=max_n, eps=eps)
|
| 601 |
+
self.dc = TensorTreeDC(
|
| 602 |
+
max_n=max_n, max_newton=max_newton, eps=eps, tol=tol)
|
| 603 |
+
self.back_accum = HouseholderBackAccumulate(max_n=max_n, eps=eps)
|
| 604 |
+
|
| 605 |
+
self.validator = EighValidator()
|
| 606 |
+
|
| 607 |
+
def forward(self, A: Tensor, validate: bool = False
|
| 608 |
+
) -> Tuple[Tensor, Tensor]:
|
| 609 |
+
B, n, _ = A.shape
|
| 610 |
+
|
| 611 |
+
if self.use_jacobi:
|
| 612 |
+
eigenvalues, eigenvectors = self.jacobi(A)
|
| 613 |
+
else:
|
| 614 |
+
A_work = A.clone()
|
| 615 |
+
d = torch.empty(B, n, device=A.device, dtype=A.dtype)
|
| 616 |
+
e = torch.empty(B, n - 1, device=A.device, dtype=A.dtype)
|
| 617 |
+
reflectors = torch.zeros(max(n - 2, 1), B, n,
|
| 618 |
+
device=A.device, dtype=A.dtype)
|
| 619 |
+
self.tridiag(A_work, d, e, reflectors)
|
| 620 |
+
eigenvalues, Z = self.dc(d, e)
|
| 621 |
+
eigenvectors = self.back_accum(reflectors, Z, n)
|
| 622 |
+
# Newton-Schulz re-orthogonalization for D&C path
|
| 623 |
+
eigenvectors = orthogonalize_ns(eigenvectors, n_iter=2)
|
| 624 |
+
|
| 625 |
+
if validate:
|
| 626 |
+
res_norm, orth_err, max_err = self.validator(A, eigenvalues, eigenvectors)
|
| 627 |
+
print(f"[CompiledEigh] max residual: {max_err.item():.2e}, "
|
| 628 |
+
f"mean orth err: {orth_err.mean().item():.2e}")
|
| 629 |
+
|
| 630 |
+
return eigenvalues, eigenvectors
|
| 631 |
+
|
| 632 |
+
|
| 633 |
+
# =============================================================================
|
| 634 |
+
# Functional API
|
| 635 |
+
# =============================================================================
|
| 636 |
+
|
| 637 |
+
_cached_solvers = {}
|
| 638 |
+
|
| 639 |
+
def compiled_eigh(A: Tensor, validate: bool = False) -> Tuple[Tensor, Tensor]:
|
| 640 |
+
B, n, _ = A.shape
|
| 641 |
+
key = (n, A.device, A.dtype)
|
| 642 |
+
if key not in _cached_solvers:
|
| 643 |
+
_cached_solvers[key] = CompiledEigh(max_n=n).to(A.device)
|
| 644 |
+
return _cached_solvers[key](A, validate=validate)
|
| 645 |
+
|
| 646 |
+
|
| 647 |
+
"""
|
| 648 |
+
CompiledEigh β Colab GPU Benchmark v3
|
| 649 |
+
Fixes:
|
| 650 |
+
v2: Jacobi pairs as plain Python lists (Dynamo compile fix), sweeps 6β10
|
| 651 |
+
v3: Replaced Gram-Schmidt with Newton-Schulz orthogonalization (all-bmm),
|
| 652 |
+
disabled TF32 to ensure fp32 precision on Blackwell
|
| 653 |
+
"""
|
| 654 |
+
|
| 655 |
+
import torch
|
| 656 |
+
import time
|
| 657 |
+
import gc
|
| 658 |
+
import sys
|
| 659 |
+
|
| 660 |
+
# ββ Ensure full fp32 precision on Ampere/Hopper/Blackwell ββ
|
| 661 |
+
# TF32 uses 10-bit mantissa for matmul which can degrade orthogonality
|
| 662 |
+
torch.backends.cuda.matmul.allow_tf32 = False
|
| 663 |
+
torch.backends.cudnn.allow_tf32 = False
|
| 664 |
+
torch.set_float32_matmul_precision('highest')
|
| 665 |
+
|
| 666 |
+
|
| 667 |
+
def sync():
|
| 668 |
+
if torch.cuda.is_available():
|
| 669 |
+
torch.cuda.synchronize()
|
| 670 |
+
|
| 671 |
+
|
| 672 |
+
def gpu_timer(fn, warmup=10, repeats=200):
|
| 673 |
+
for _ in range(warmup):
|
| 674 |
+
fn()
|
| 675 |
+
sync()
|
| 676 |
+
start = time.perf_counter()
|
| 677 |
+
for _ in range(repeats):
|
| 678 |
+
fn()
|
| 679 |
+
sync()
|
| 680 |
+
return (time.perf_counter() - start) / repeats
|
| 681 |
+
|
| 682 |
+
|
| 683 |
+
def make_symmetric_batch(B, n, device, dtype=torch.float32):
|
| 684 |
+
R = torch.randn(B, n, n, device=device, dtype=dtype)
|
| 685 |
+
return (R + R.transpose(-2, -1)) / 2.0
|
| 686 |
+
|
| 687 |
+
|
| 688 |
+
def make_cm_like_batch(B, n, device, dtype=torch.float32):
|
| 689 |
+
points = torch.randn(B, n, n, device=device, dtype=dtype)
|
| 690 |
+
points = points / (points.norm(dim=-1, keepdim=True) + 1e-8)
|
| 691 |
+
return torch.bmm(points, points.transpose(-2, -1)) * 0.3
|
| 692 |
+
|
| 693 |
+
|
| 694 |
+
def fmt_time(seconds):
|
| 695 |
+
if seconds < 1e-3:
|
| 696 |
+
return f"{seconds*1e6:.1f} us"
|
| 697 |
+
elif seconds < 1.0:
|
| 698 |
+
return f"{seconds*1e3:.2f} ms"
|
| 699 |
+
return f"{seconds:.3f} s"
|
| 700 |
+
|
| 701 |
+
|
| 702 |
+
# βββ Test 0: Newton-Schulz Diagnostic βββ
|
| 703 |
+
|
| 704 |
+
def test_ns_diagnostic(device):
|
| 705 |
+
"""Verify Newton-Schulz orthogonalization works on GPU independently."""
|
| 706 |
+
print("\n" + "=" * 70)
|
| 707 |
+
print(" TEST 0: NEWTON-SCHULZ DIAGNOSTIC")
|
| 708 |
+
print("=" * 70)
|
| 709 |
+
|
| 710 |
+
for n in [5, 6, 8]:
|
| 711 |
+
B = 1024
|
| 712 |
+
# Create nearly-orthogonal matrix (simulating Jacobi output)
|
| 713 |
+
Q, _ = torch.linalg.qr(torch.randn(B, n, n, device=device))
|
| 714 |
+
# Perturb to ~1e-3 orthogonality error
|
| 715 |
+
noise = torch.randn(B, n, n, device=device) * 1e-3
|
| 716 |
+
V_dirty = Q + noise
|
| 717 |
+
|
| 718 |
+
I_n = torch.eye(n, device=device).unsqueeze(0)
|
| 719 |
+
|
| 720 |
+
# Before NS
|
| 721 |
+
VtV_before = torch.bmm(V_dirty.transpose(-2, -1), V_dirty)
|
| 722 |
+
orth_before = torch.linalg.norm((VtV_before - I_n).reshape(B, -1), dim=-1).max().item()
|
| 723 |
+
|
| 724 |
+
# After NS (2 iterations)
|
| 725 |
+
V_clean = orthogonalize_ns(V_dirty, n_iter=2)
|
| 726 |
+
VtV_after = torch.bmm(V_clean.transpose(-2, -1), V_clean)
|
| 727 |
+
orth_after = torch.linalg.norm((VtV_after - I_n).reshape(B, -1), dim=-1).max().item()
|
| 728 |
+
|
| 729 |
+
# After NS (3 iterations for comparison)
|
| 730 |
+
V_clean3 = orthogonalize_ns(V_dirty, n_iter=3)
|
| 731 |
+
VtV_after3 = torch.bmm(V_clean3.transpose(-2, -1), V_clean3)
|
| 732 |
+
orth_after3 = torch.linalg.norm((VtV_after3 - I_n).reshape(B, -1), dim=-1).max().item()
|
| 733 |
+
|
| 734 |
+
print(f" n={n}: before={orth_before:.2e} "
|
| 735 |
+
f"after(2iter)={orth_after:.2e} "
|
| 736 |
+
f"after(3iter)={orth_after3:.2e}")
|
| 737 |
+
|
| 738 |
+
# Also test with actual Jacobi output
|
| 739 |
+
print(f"\n --- With actual Jacobi output ---")
|
| 740 |
+
for n in [5, 6]:
|
| 741 |
+
B = 2048
|
| 742 |
+
A = make_symmetric_batch(B, n, device)
|
| 743 |
+
solver = JacobiEigh(max_n=n, max_sweeps=10).to(device)
|
| 744 |
+
|
| 745 |
+
# Run Jacobi WITHOUT the NS cleanup
|
| 746 |
+
W = A.clone()
|
| 747 |
+
V = torch.eye(n, device=device).unsqueeze(0).expand(B, -1, -1).clone()
|
| 748 |
+
for _sweep in range(solver.max_sweeps):
|
| 749 |
+
for idx in range(solver._n_pairs):
|
| 750 |
+
p, q = solver._pairs_p[idx], solver._pairs_q[idx]
|
| 751 |
+
app, aqq, apq = W[:, p, p], W[:, q, q], W[:, p, q]
|
| 752 |
+
two_apq = 2.0 * apq
|
| 753 |
+
diff = aqq - app
|
| 754 |
+
abs_2apq = two_apq.abs().clamp(min=1e-30)
|
| 755 |
+
sign_2apq = torch.where(two_apq >= 0,
|
| 756 |
+
torch.ones_like(two_apq), -torch.ones_like(two_apq))
|
| 757 |
+
tau = diff / (abs_2apq * sign_2apq)
|
| 758 |
+
tau_sign = torch.where(tau >= 0,
|
| 759 |
+
torch.ones_like(tau), -torch.ones_like(tau))
|
| 760 |
+
t = tau_sign / (tau.abs() + torch.sqrt(1.0 + tau * tau))
|
| 761 |
+
skip = (apq.abs() < 1e-30).float()
|
| 762 |
+
t = t * (1.0 - skip)
|
| 763 |
+
c = 1.0 / torch.sqrt(1.0 + t * t)
|
| 764 |
+
s = t * c
|
| 765 |
+
c_col, s_col = c.unsqueeze(-1), s.unsqueeze(-1)
|
| 766 |
+
Wp = W[:, :, p].clone(); Wq = W[:, :, q].clone()
|
| 767 |
+
W[:, :, p] = c_col * Wp - s_col * Wq
|
| 768 |
+
W[:, :, q] = s_col * Wp + c_col * Wq
|
| 769 |
+
Wp = W[:, p, :].clone(); Wq = W[:, q, :].clone()
|
| 770 |
+
W[:, p, :] = c_col * Wp - s_col * Wq
|
| 771 |
+
W[:, q, :] = s_col * Wp + c_col * Wq
|
| 772 |
+
W[:, p, q] = 0.0; W[:, q, p] = 0.0
|
| 773 |
+
W[:, p, p] = app - t * apq
|
| 774 |
+
W[:, q, q] = aqq + t * apq
|
| 775 |
+
Vp = V[:, :, p].clone(); Vq = V[:, :, q].clone()
|
| 776 |
+
V[:, :, p] = c_col * Vp - s_col * Vq
|
| 777 |
+
V[:, :, q] = s_col * Vp + c_col * Vq
|
| 778 |
+
|
| 779 |
+
I_n = torch.eye(n, device=device).unsqueeze(0)
|
| 780 |
+
VtV = torch.bmm(V.transpose(-2, -1), V)
|
| 781 |
+
orth_raw = torch.linalg.norm((VtV - I_n).reshape(B, -1), dim=-1).max().item()
|
| 782 |
+
|
| 783 |
+
V_ns = orthogonalize_ns(V, n_iter=2)
|
| 784 |
+
VtV_ns = torch.bmm(V_ns.transpose(-2, -1), V_ns)
|
| 785 |
+
orth_ns = torch.linalg.norm((VtV_ns - I_n).reshape(B, -1), dim=-1).max().item()
|
| 786 |
+
|
| 787 |
+
print(f" Jacobi raw n={n}: orth={orth_raw:.2e} after NS(2)={orth_ns:.2e}")
|
| 788 |
+
|
| 789 |
+
|
| 790 |
+
# βββ Test 1: Accuracy βββ
|
| 791 |
+
|
| 792 |
+
def test_accuracy(device):
|
| 793 |
+
print("\n" + "=" * 70)
|
| 794 |
+
print(" TEST 1: ACCURACY vs torch.linalg.eigh")
|
| 795 |
+
print("=" * 70)
|
| 796 |
+
|
| 797 |
+
validator = EighValidator()
|
| 798 |
+
configs = [
|
| 799 |
+
(3, 4096, "3x3 small"),
|
| 800 |
+
(5, 4096, "5x5 CM matrix size"),
|
| 801 |
+
(6, 4096, "6x6 pentachoron bordered"),
|
| 802 |
+
(8, 2048, "8x8 padded CM"),
|
| 803 |
+
(12, 1024, "12x12 medium"),
|
| 804 |
+
(16, 512, "16x16 Jacobi boundary"),
|
| 805 |
+
]
|
| 806 |
+
|
| 807 |
+
all_pass = True
|
| 808 |
+
for n, B, label in configs:
|
| 809 |
+
A = make_symmetric_batch(B, n, device)
|
| 810 |
+
ref_vals, ref_vecs = torch.linalg.eigh(A)
|
| 811 |
+
|
| 812 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 813 |
+
our_vals, our_vecs = solver(A)
|
| 814 |
+
|
| 815 |
+
val_err = (our_vals - ref_vals).abs().max().item()
|
| 816 |
+
val_mean = (our_vals - ref_vals).abs().mean().item()
|
| 817 |
+
|
| 818 |
+
dots = torch.bmm(ref_vecs.transpose(-2, -1), our_vecs)
|
| 819 |
+
alignment = dots.abs().max(dim=-1).values.min().item()
|
| 820 |
+
|
| 821 |
+
res_norm, orth_err, max_res = validator(A, our_vals, our_vecs)
|
| 822 |
+
max_orth = orth_err.max().item()
|
| 823 |
+
|
| 824 |
+
# Thresholds: eigenval 1e-3, alignment 0.999, orth 1e-4
|
| 825 |
+
ok = val_err < 1e-3 and alignment > 0.999 and max_orth < 1e-4
|
| 826 |
+
if not ok:
|
| 827 |
+
all_pass = False
|
| 828 |
+
|
| 829 |
+
print(f"\n [{'PASS' if ok else 'FAIL'}] {label} (n={n}, B={B})")
|
| 830 |
+
print(f" eigenvalue err max={val_err:.2e} mean={val_mean:.2e}")
|
| 831 |
+
print(f" eigvec alignment min={alignment:.8f}")
|
| 832 |
+
print(f" residual norm max={max_res.item():.2e}")
|
| 833 |
+
print(f" orthogonality max={max_orth:.2e}")
|
| 834 |
+
|
| 835 |
+
print(f"\n --- CM-like spectral distribution ---")
|
| 836 |
+
for n in [5, 6]:
|
| 837 |
+
A = make_cm_like_batch(2048, n, device)
|
| 838 |
+
ref_vals, _ = torch.linalg.eigh(A)
|
| 839 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 840 |
+
our_vals, our_vecs = solver(A)
|
| 841 |
+
val_err = (our_vals - ref_vals).abs().max().item()
|
| 842 |
+
res_norm, orth_err, max_res = validator(A, our_vals, our_vecs)
|
| 843 |
+
print(f" CM-like n={n}: val_err={val_err:.2e} "
|
| 844 |
+
f"res={max_res.item():.2e} orth={orth_err.max().item():.2e}")
|
| 845 |
+
|
| 846 |
+
return all_pass
|
| 847 |
+
|
| 848 |
+
|
| 849 |
+
# βββ Test 2: torch.compile fullgraph βββ
|
| 850 |
+
|
| 851 |
+
def test_compile(device):
|
| 852 |
+
print("\n" + "=" * 70)
|
| 853 |
+
print(" TEST 2: torch.compile(fullgraph=True)")
|
| 854 |
+
print("=" * 70)
|
| 855 |
+
|
| 856 |
+
results = {}
|
| 857 |
+
for n, B, label in [(5, 1024, "5x5"), (6, 1024, "6x6"), (8, 512, "8x8")]:
|
| 858 |
+
A = make_symmetric_batch(B, n, device)
|
| 859 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 860 |
+
|
| 861 |
+
try:
|
| 862 |
+
compiled_solver = torch.compile(solver, fullgraph=True)
|
| 863 |
+
vals, vecs = compiled_solver(A)
|
| 864 |
+
sync()
|
| 865 |
+
ref_vals, _ = torch.linalg.eigh(A)
|
| 866 |
+
err = (vals - ref_vals).abs().max().item()
|
| 867 |
+
results[label] = ("PASS", err)
|
| 868 |
+
print(f" [{label}] fullgraph=True SUCCESS (val_err={err:.2e})")
|
| 869 |
+
except Exception as e:
|
| 870 |
+
results[label] = ("FAIL", str(e)[:200])
|
| 871 |
+
print(f" [{label}] COMPILE FAILED: {str(e)[:200]}")
|
| 872 |
+
|
| 873 |
+
return all(v[0] == "PASS" for v in results.values())
|
| 874 |
+
|
| 875 |
+
|
| 876 |
+
# βββ Test 3: Throughput βββ
|
| 877 |
+
|
| 878 |
+
def test_benchmark(device):
|
| 879 |
+
print("\n" + "=" * 70)
|
| 880 |
+
print(" TEST 3: GPU THROUGHPUT BENCHMARK")
|
| 881 |
+
print("=" * 70)
|
| 882 |
+
print(f" Device: {torch.cuda.get_device_name(0)}")
|
| 883 |
+
print(f" Timing: 10 warmup + 200 repeats\n")
|
| 884 |
+
|
| 885 |
+
configs = [
|
| 886 |
+
(5, 1024, "CM 5x5 B=1024"),
|
| 887 |
+
(5, 4096, "CM 5x5 B=4096"),
|
| 888 |
+
(5, 8192, "CM 5x5 B=8192"),
|
| 889 |
+
(6, 1024, "CM 6x6 B=1024"),
|
| 890 |
+
(6, 4096, "CM 6x6 B=4096"),
|
| 891 |
+
(6, 8192, "CM 6x6 B=8192"),
|
| 892 |
+
(8, 2048, "8x8 B=2048"),
|
| 893 |
+
(16, 1024, "16x16 B=1024"),
|
| 894 |
+
]
|
| 895 |
+
|
| 896 |
+
print(f" {'Config':<22} {'eigh ref':>10} {'ours eager':>12} "
|
| 897 |
+
f"{'ours compiled':>14} {'vs ref':>8}")
|
| 898 |
+
print(f" {'-'*22} {'-'*10} {'-'*12} {'-'*14} {'-'*8}")
|
| 899 |
+
|
| 900 |
+
for n, B, label in configs:
|
| 901 |
+
A = make_symmetric_batch(B, n, device)
|
| 902 |
+
|
| 903 |
+
ref_time = gpu_timer(lambda: torch.linalg.eigh(A))
|
| 904 |
+
|
| 905 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 906 |
+
eager_time = gpu_timer(lambda: solver(A))
|
| 907 |
+
|
| 908 |
+
try:
|
| 909 |
+
compiled_solver = torch.compile(solver, fullgraph=True)
|
| 910 |
+
for _ in range(5):
|
| 911 |
+
compiled_solver(A)
|
| 912 |
+
sync()
|
| 913 |
+
compiled_time = gpu_timer(lambda: compiled_solver(A))
|
| 914 |
+
compiled_str = fmt_time(compiled_time)
|
| 915 |
+
speedup = ref_time / compiled_time
|
| 916 |
+
speedup_str = f"{speedup:.2f}x"
|
| 917 |
+
except Exception:
|
| 918 |
+
compiled_str = "FAIL"
|
| 919 |
+
speedup_str = "N/A"
|
| 920 |
+
|
| 921 |
+
print(f" {label:<22} {fmt_time(ref_time):>10} "
|
| 922 |
+
f"{fmt_time(eager_time):>12} {compiled_str:>14} {speedup_str:>8}")
|
| 923 |
+
|
| 924 |
+
print(f"\n --- High batch stress test ---")
|
| 925 |
+
for n in [5, 6]:
|
| 926 |
+
for B in [16384, 32768]:
|
| 927 |
+
try:
|
| 928 |
+
A = make_symmetric_batch(B, n, device)
|
| 929 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 930 |
+
compiled_solver = torch.compile(solver, fullgraph=True)
|
| 931 |
+
for _ in range(3):
|
| 932 |
+
compiled_solver(A)
|
| 933 |
+
sync()
|
| 934 |
+
t = gpu_timer(lambda: compiled_solver(A), warmup=5, repeats=100)
|
| 935 |
+
ref_t = gpu_timer(lambda: torch.linalg.eigh(A), warmup=5, repeats=100)
|
| 936 |
+
print(f" n={n} B={B}: compiled={fmt_time(t)} ref={fmt_time(ref_t)} "
|
| 937 |
+
f"ratio={ref_t/t:.2f}x throughput={B/t:.0f}/sec")
|
| 938 |
+
except RuntimeError as e:
|
| 939 |
+
if "out of memory" in str(e).lower():
|
| 940 |
+
print(f" n={n} B={B}: OOM")
|
| 941 |
+
torch.cuda.empty_cache()
|
| 942 |
+
else:
|
| 943 |
+
raise
|
| 944 |
+
|
| 945 |
+
|
| 946 |
+
# βββ Test 4: Autograd βββ
|
| 947 |
+
|
| 948 |
+
def test_autograd(device):
|
| 949 |
+
print("\n" + "=" * 70)
|
| 950 |
+
print(" TEST 4: AUTOGRAD BACKWARD")
|
| 951 |
+
print("=" * 70)
|
| 952 |
+
|
| 953 |
+
for n, B in [(5, 512), (6, 512)]:
|
| 954 |
+
A_ref = make_symmetric_batch(B, n, device).requires_grad_(True)
|
| 955 |
+
vals_ref, vecs_ref = torch.linalg.eigh(A_ref)
|
| 956 |
+
(vals_ref.sum() + (vecs_ref ** 2).sum()).backward()
|
| 957 |
+
grad_ref = A_ref.grad.clone()
|
| 958 |
+
|
| 959 |
+
# Eager backward
|
| 960 |
+
A_e = A_ref.detach().clone().requires_grad_(True)
|
| 961 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 962 |
+
try:
|
| 963 |
+
vals_e, vecs_e = solver(A_e)
|
| 964 |
+
(vals_e.sum() + (vecs_e ** 2).sum()).backward()
|
| 965 |
+
err_e = (A_e.grad - grad_ref).abs().max().item()
|
| 966 |
+
rel_e = err_e / (grad_ref.abs().max().item() + 1e-30)
|
| 967 |
+
print(f" [{'PASS' if rel_e < 0.1 else 'WARN'}] n={n} eager backward: "
|
| 968 |
+
f"grad_err={err_e:.2e} rel={rel_e:.2e}")
|
| 969 |
+
except Exception as e:
|
| 970 |
+
print(f" [FAIL] n={n} eager backward: {e}")
|
| 971 |
+
|
| 972 |
+
# Compiled backward (may break β forward fullgraph is the key win)
|
| 973 |
+
A_c = A_ref.detach().clone().requires_grad_(True)
|
| 974 |
+
try:
|
| 975 |
+
compiled_solver = torch.compile(solver)
|
| 976 |
+
vals_c, vecs_c = compiled_solver(A_c)
|
| 977 |
+
(vals_c.sum() + (vecs_c ** 2).sum()).backward()
|
| 978 |
+
err_c = (A_c.grad - grad_ref).abs().max().item()
|
| 979 |
+
rel_c = err_c / (grad_ref.abs().max().item() + 1e-30)
|
| 980 |
+
print(f" [{'PASS' if rel_c < 0.1 else 'WARN'}] n={n} compiled backward: "
|
| 981 |
+
f"grad_err={err_c:.2e} rel={rel_c:.2e}")
|
| 982 |
+
except Exception as e:
|
| 983 |
+
print(f" [INFO] n={n} compiled backward: {str(e)[:150]}")
|
| 984 |
+
print(f" (forward fullgraph is the main win)")
|
| 985 |
+
|
| 986 |
+
|
| 987 |
+
# βββ Test 5: VRAM βββ
|
| 988 |
+
|
| 989 |
+
def test_vram(device):
|
| 990 |
+
print("\n" + "=" * 70)
|
| 991 |
+
print(" TEST 5: VRAM USAGE")
|
| 992 |
+
print("=" * 70)
|
| 993 |
+
|
| 994 |
+
for n, B in [(5, 4096), (6, 4096), (6, 8192), (5, 8192)]:
|
| 995 |
+
torch.cuda.empty_cache()
|
| 996 |
+
gc.collect()
|
| 997 |
+
torch.cuda.reset_peak_memory_stats()
|
| 998 |
+
base_mem = torch.cuda.memory_allocated()
|
| 999 |
+
|
| 1000 |
+
A = make_symmetric_batch(B, n, device)
|
| 1001 |
+
solver = CompiledEigh(max_n=n).to(device)
|
| 1002 |
+
vals, vecs = solver(A)
|
| 1003 |
+
|
| 1004 |
+
peak_mem = torch.cuda.max_memory_allocated()
|
| 1005 |
+
delta_mb = (peak_mem - base_mem) / (1024 ** 2)
|
| 1006 |
+
print(f" n={n} B={B}: peak delta = {delta_mb:.1f} MB")
|
| 1007 |
+
|
| 1008 |
+
del A, solver, vals, vecs
|
| 1009 |
+
torch.cuda.empty_cache()
|
| 1010 |
+
gc.collect()
|
| 1011 |
+
|
| 1012 |
+
|
| 1013 |
+
# βββ Main βββ
|
| 1014 |
+
|
| 1015 |
+
def main():
|
| 1016 |
+
print("=" * 70)
|
| 1017 |
+
print(" CompiledEigh v3 β GPU Benchmark Suite")
|
| 1018 |
+
print("=" * 70)
|
| 1019 |
+
|
| 1020 |
+
if not torch.cuda.is_available():
|
| 1021 |
+
print("\n No CUDA. Run on Colab with A100/H100.")
|
| 1022 |
+
sys.exit(1)
|
| 1023 |
+
|
| 1024 |
+
device = torch.device('cuda')
|
| 1025 |
+
print(f"\n GPU: {torch.cuda.get_device_name(0)}")
|
| 1026 |
+
print(f" CUDA: {torch.version.cuda}")
|
| 1027 |
+
print(f" PyTorch: {torch.__version__}")
|
| 1028 |
+
mem_gb = torch.cuda.get_device_properties(0).total_memory / (1024**3)
|
| 1029 |
+
print(f" VRAM: {mem_gb:.1f} GB")
|
| 1030 |
+
print(f" TF32 matmul: {torch.backends.cuda.matmul.allow_tf32}")
|
| 1031 |
+
print(f" float32 precision: {torch.get_float32_matmul_precision()}")
|
| 1032 |
+
|
| 1033 |
+
test_ns_diagnostic(device)
|
| 1034 |
+
acc_ok = test_accuracy(device)
|
| 1035 |
+
compile_ok = test_compile(device)
|
| 1036 |
+
test_benchmark(device)
|
| 1037 |
+
test_autograd(device)
|
| 1038 |
+
test_vram(device)
|
| 1039 |
+
|
| 1040 |
+
print("\n" + "=" * 70)
|
| 1041 |
+
print(" SUMMARY")
|
| 1042 |
+
print("=" * 70)
|
| 1043 |
+
print(f" Accuracy: {'PASS' if acc_ok else 'FAIL'}")
|
| 1044 |
+
print(f" Compile: {'PASS' if compile_ok else 'FAIL'}")
|
| 1045 |
+
print("=" * 70)
|
| 1046 |
+
|
| 1047 |
+
|
| 1048 |
+
if __name__ == '__main__':
|
| 1049 |
+
main()
|