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Create kernel_profiler.py

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1
+ """
2
+ triton_svd_general.py β€” Generalized batched thin SVD for (B, M, N) matrices.
3
+
4
+ Three strategies, auto-dispatched by N:
5
+ N=2: Fused Triton kernel β€” closed-form 2Γ—2 eigensolve in registers
6
+ N=3: Fused Triton kernel β€” cyclic Jacobi in registers (from session start)
7
+ Nβ‰₯4: Gram-Eigh hybrid β€” Triton G=A^T A + torch.linalg.eigh + Triton U recovery
8
+
9
+ All methods exploit the thin-matrix shortcut: decompose via the NΓ—N Gram
10
+ matrix G=A^T A rather than working on the full MΓ—N matrix directly.
11
+
12
+ Mathematical lineage:
13
+ Eckart-Young (1936): G = A^T A β†’ eigenvalues of G = σ² of A
14
+ Jacobi (1846): Cyclic Givens rotations for symmetric eigendecomposition
15
+ Golub-Reinsch (1970): U = A V S^{-1} recovery
16
+ Batcher (1968): Sorting network for eigenvalue ordering
17
+
18
+ Author: AbstractPhil / Claude Opus 4.6
19
+ """
20
+
21
+ import triton
22
+ import triton.language as tl
23
+ import torch
24
+ import torch.nn.functional as F
25
+ import math
26
+ import time
27
+ import json
28
+
29
+
30
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
31
+ # β•‘ KERNEL 1: Fused SVD for (B, M, 2) β€” closed-form 2Γ—2 eigensolve β•‘
32
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
33
+
34
+ @triton.jit
35
+ def _svd2_kernel(
36
+ A_ptr, U_ptr, S_ptr, Vh_ptr,
37
+ M: tl.constexpr, BLOCK_M: tl.constexpr, EPS: tl.constexpr,
38
+ ):
39
+ """Fused SVD for (M, 2) matrices. One program per batch element.
40
+
41
+ 2Γ—2 symmetric eigendecomposition is closed-form:
42
+ ΞΈ = 0.5 * atan2(2*g01, g00 - g11)
43
+ c = cos(ΞΈ), s = sin(ΞΈ)
44
+ """
45
+ bid = tl.program_id(0)
46
+ base = bid * M * 2
47
+
48
+ # Stage 1: G = A^T A (3 accumulators: g00, g01, g11)
49
+ g00 = tl.zeros([], dtype=tl.float32)
50
+ g01 = tl.zeros([], dtype=tl.float32)
51
+ g11 = tl.zeros([], dtype=tl.float32)
52
+
53
+ for block_start in range(0, M, BLOCK_M):
54
+ offs = tl.arange(0, BLOCK_M)
55
+ row_idx = block_start + offs
56
+ mask = row_idx < M
57
+ a0 = tl.load(A_ptr + base + row_idx * 2 + 0, mask=mask, other=0.0).to(tl.float32)
58
+ a1 = tl.load(A_ptr + base + row_idx * 2 + 1, mask=mask, other=0.0).to(tl.float32)
59
+ g00 += tl.sum(a0 * a0)
60
+ g01 += tl.sum(a0 * a1)
61
+ g11 += tl.sum(a1 * a1)
62
+
63
+ # Stage 2: 2Γ—2 eigendecomposition via single Jacobi rotation
64
+ # Same formula as the 3Γ—3 kernel β€” no trig needed
65
+ off_diag = g01
66
+ diag_diff = g11 - g00
67
+ abs_off = tl.abs(off_diag)
68
+ tau = tl.where(abs_off > EPS, diag_diff / (2.0 * off_diag), 0.0)
69
+ t = tl.where(abs_off > EPS,
70
+ tl.where(tau >= 0, 1.0, -1.0) / (tl.abs(tau) + tl.sqrt(1.0 + tau * tau)),
71
+ 0.0)
72
+ c = 1.0 / tl.sqrt(1.0 + t * t)
73
+ s = t * c
74
+
75
+ # Eigenvalues after rotation
76
+ eig0 = c * c * g00 - 2.0 * s * c * g01 + s * s * g11
77
+ eig1 = s * s * g00 + 2.0 * s * c * g01 + c * c * g11
78
+
79
+ # Ensure descending order
80
+ s0 = tl.sqrt(tl.maximum(eig0, EPS))
81
+ s1 = tl.sqrt(tl.maximum(eig1, EPS))
82
+
83
+ # V starts as I, Jacobi rotation applied
84
+ v00 = c; v01 = s
85
+ v10 = -s; v11 = c
86
+
87
+ # Sort descending
88
+ do_swap = s0 < s1
89
+ s0, s1 = tl.where(do_swap, s1, s0), tl.where(do_swap, s0, s1)
90
+ tv = v00; v00 = tl.where(do_swap, v01, v00); v01 = tl.where(do_swap, tv, v01)
91
+ tv = v10; v10 = tl.where(do_swap, v11, v10); v11 = tl.where(do_swap, tv, v11)
92
+
93
+ # Write S
94
+ s_base = bid * 2
95
+ tl.store(S_ptr + s_base + 0, s0)
96
+ tl.store(S_ptr + s_base + 1, s1)
97
+
98
+ # Write Vh = V^T
99
+ vh_base = bid * 4
100
+ tl.store(Vh_ptr + vh_base + 0, v00); tl.store(Vh_ptr + vh_base + 1, v10)
101
+ tl.store(Vh_ptr + vh_base + 2, v01); tl.store(Vh_ptr + vh_base + 3, v11)
102
+
103
+ # Stage 3: U = A @ V @ diag(1/S)
104
+ inv_s0 = 1.0 / (s0 + EPS)
105
+ inv_s1 = 1.0 / (s1 + EPS)
106
+
107
+ for block_start in range(0, M, BLOCK_M):
108
+ offs = tl.arange(0, BLOCK_M)
109
+ row_idx = block_start + offs
110
+ mask = row_idx < M
111
+ a0 = tl.load(A_ptr + base + row_idx * 2 + 0, mask=mask, other=0.0).to(tl.float32)
112
+ a1 = tl.load(A_ptr + base + row_idx * 2 + 1, mask=mask, other=0.0).to(tl.float32)
113
+ u0 = (a0 * v00 + a1 * v10) * inv_s0
114
+ u1 = (a0 * v01 + a1 * v11) * inv_s1
115
+ u_base = bid * M * 2
116
+ tl.store(U_ptr + u_base + row_idx * 2 + 0, u0, mask=mask)
117
+ tl.store(U_ptr + u_base + row_idx * 2 + 1, u1, mask=mask)
118
+
119
+
120
+ def batched_svd2(A, block_m=128):
121
+ """Fused Triton SVD for (B, M, 2) tensors."""
122
+ assert A.ndim == 3 and A.shape[2] == 2
123
+ B, M, _ = A.shape
124
+ A_f32 = A.contiguous().float()
125
+ U = torch.empty((B, M, 2), dtype=torch.float32, device=A.device)
126
+ S = torch.empty((B, 2), dtype=torch.float32, device=A.device)
127
+ Vh = torch.empty((B, 2, 2), dtype=torch.float32, device=A.device)
128
+ _svd2_kernel[(B,)](A_f32, U, S, Vh, M=M, BLOCK_M=block_m, EPS=1e-12)
129
+ return U, S, Vh
130
+
131
+
132
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
133
+ # β•‘ KERNEL 2: Fused SVD for (B, M, 3) β€” cyclic Jacobi (original kernel) β•‘
134
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
135
+
136
+ @triton.jit
137
+ def _svd3_kernel(
138
+ A_ptr, U_ptr, S_ptr, Vh_ptr,
139
+ M: tl.constexpr, BLOCK_M: tl.constexpr,
140
+ JACOBI_ITERS: tl.constexpr, EPS: tl.constexpr,
141
+ ):
142
+ bid = tl.program_id(0)
143
+ g00 = tl.zeros([], dtype=tl.float32); g01 = tl.zeros([], dtype=tl.float32)
144
+ g02 = tl.zeros([], dtype=tl.float32); g11 = tl.zeros([], dtype=tl.float32)
145
+ g12 = tl.zeros([], dtype=tl.float32); g22 = tl.zeros([], dtype=tl.float32)
146
+ base = bid * M * 3
147
+ for block_start in range(0, M, BLOCK_M):
148
+ offs = tl.arange(0, BLOCK_M); row_idx = block_start + offs; mask = row_idx < M
149
+ a0 = tl.load(A_ptr + base + row_idx * 3 + 0, mask=mask, other=0.0).to(tl.float32)
150
+ a1 = tl.load(A_ptr + base + row_idx * 3 + 1, mask=mask, other=0.0).to(tl.float32)
151
+ a2 = tl.load(A_ptr + base + row_idx * 3 + 2, mask=mask, other=0.0).to(tl.float32)
152
+ g00 += tl.sum(a0*a0); g01 += tl.sum(a0*a1); g02 += tl.sum(a0*a2)
153
+ g11 += tl.sum(a1*a1); g12 += tl.sum(a1*a2); g22 += tl.sum(a2*a2)
154
+ v00=1.0;v01=0.0;v02=0.0;v10=0.0;v11=1.0;v12=0.0;v20=0.0;v21=0.0;v22=1.0
155
+ for _ in range(JACOBI_ITERS):
156
+ off_diag=g01;diag_diff=g11-g00;abs_off=tl.abs(off_diag)
157
+ tau=tl.where(abs_off>EPS,diag_diff/(2.0*off_diag),0.0)
158
+ t=tl.where(abs_off>EPS,tl.where(tau>=0,1.0,-1.0)/(tl.abs(tau)+tl.sqrt(1.0+tau*tau)),0.0)
159
+ c=1.0/tl.sqrt(1.0+t*t);s=t*c
160
+ ng00=c*c*g00-2.0*s*c*g01+s*s*g11;ng11=s*s*g00+2.0*s*c*g01+c*c*g11
161
+ ng02=c*g02-s*g12;ng12=s*g02+c*g12
162
+ g00=ng00;g11=ng11;g01=0.0;g02=ng02;g12=ng12
163
+ nv00=c*v00-s*v01;nv01=s*v00+c*v01;nv10=c*v10-s*v11;nv11=s*v10+c*v11
164
+ nv20=c*v20-s*v21;nv21=s*v20+c*v21
165
+ v00=nv00;v01=nv01;v10=nv10;v11=nv11;v20=nv20;v21=nv21
166
+ off_diag=g02;diag_diff=g22-g00;abs_off=tl.abs(off_diag)
167
+ tau=tl.where(abs_off>EPS,diag_diff/(2.0*off_diag),0.0)
168
+ t=tl.where(abs_off>EPS,tl.where(tau>=0,1.0,-1.0)/(tl.abs(tau)+tl.sqrt(1.0+tau*tau)),0.0)
169
+ c=1.0/tl.sqrt(1.0+t*t);s=t*c
170
+ ng00=c*c*g00-2.0*s*c*g02+s*s*g22;ng22=s*s*g00+2.0*s*c*g02+c*c*g22
171
+ ng01=c*g01-s*g12;ng12b=s*g01+c*g12
172
+ g00=ng00;g22=ng22;g02=0.0;g01=ng01;g12=ng12b
173
+ nv00=c*v00-s*v02;nv02=s*v00+c*v02;nv10=c*v10-s*v12;nv12=s*v10+c*v12
174
+ nv20=c*v20-s*v22;nv22=s*v20+c*v22
175
+ v00=nv00;v02=nv02;v10=nv10;v12=nv12;v20=nv20;v22=nv22
176
+ off_diag=g12;diag_diff=g22-g11;abs_off=tl.abs(off_diag)
177
+ tau=tl.where(abs_off>EPS,diag_diff/(2.0*off_diag),0.0)
178
+ t=tl.where(abs_off>EPS,tl.where(tau>=0,1.0,-1.0)/(tl.abs(tau)+tl.sqrt(1.0+tau*tau)),0.0)
179
+ c=1.0/tl.sqrt(1.0+t*t);s=t*c
180
+ ng11=c*c*g11-2.0*s*c*g12+s*s*g22;ng22=s*s*g11+2.0*s*c*g12+c*c*g22
181
+ ng01=c*g01-s*g02;ng02b=s*g01+c*g02
182
+ g11=ng11;g22=ng22;g12=0.0;g01=ng01;g02=ng02b
183
+ nv01=c*v01-s*v02;nv02=s*v01+c*v02;nv11=c*v11-s*v12;nv12=s*v11+c*v12
184
+ nv21=c*v21-s*v22;nv22=s*v21+c*v22
185
+ v01=nv01;v02=nv02;v11=nv11;v12=nv12;v21=nv21;v22=nv22
186
+ s0=tl.sqrt(tl.maximum(g00,EPS));s1=tl.sqrt(tl.maximum(g11,EPS));s2=tl.sqrt(tl.maximum(g22,EPS))
187
+ do_swap=s0<s1
188
+ s0,s1=tl.where(do_swap,s1,s0),tl.where(do_swap,s0,s1)
189
+ tv=v00;v00=tl.where(do_swap,v01,v00);v01=tl.where(do_swap,tv,v01)
190
+ tv=v10;v10=tl.where(do_swap,v11,v10);v11=tl.where(do_swap,tv,v11)
191
+ tv=v20;v20=tl.where(do_swap,v21,v20);v21=tl.where(do_swap,tv,v21)
192
+ do_swap=s0<s2
193
+ s0,s2=tl.where(do_swap,s2,s0),tl.where(do_swap,s0,s2)
194
+ tv=v00;v00=tl.where(do_swap,v02,v00);v02=tl.where(do_swap,tv,v02)
195
+ tv=v10;v10=tl.where(do_swap,v12,v10);v12=tl.where(do_swap,tv,v12)
196
+ tv=v20;v20=tl.where(do_swap,v22,v20);v22=tl.where(do_swap,tv,v22)
197
+ do_swap=s1<s2
198
+ s1,s2=tl.where(do_swap,s2,s1),tl.where(do_swap,s1,s2)
199
+ tv=v01;v01=tl.where(do_swap,v02,v01);v02=tl.where(do_swap,tv,v02)
200
+ tv=v11;v11=tl.where(do_swap,v12,v11);v12=tl.where(do_swap,tv,v12)
201
+ tv=v21;v21=tl.where(do_swap,v22,v21);v22=tl.where(do_swap,tv,v22)
202
+ s_base=bid*3
203
+ tl.store(S_ptr+s_base+0,s0);tl.store(S_ptr+s_base+1,s1);tl.store(S_ptr+s_base+2,s2)
204
+ vh_base=bid*9
205
+ tl.store(Vh_ptr+vh_base+0,v00);tl.store(Vh_ptr+vh_base+1,v10);tl.store(Vh_ptr+vh_base+2,v20)
206
+ tl.store(Vh_ptr+vh_base+3,v01);tl.store(Vh_ptr+vh_base+4,v11);tl.store(Vh_ptr+vh_base+5,v21)
207
+ tl.store(Vh_ptr+vh_base+6,v02);tl.store(Vh_ptr+vh_base+7,v12);tl.store(Vh_ptr+vh_base+8,v22)
208
+ inv_s0=1.0/(s0+EPS);inv_s1=1.0/(s1+EPS);inv_s2=1.0/(s2+EPS)
209
+ for block_start in range(0, M, BLOCK_M):
210
+ offs=tl.arange(0,BLOCK_M);row_idx=block_start+offs;mask=row_idx<M
211
+ a0=tl.load(A_ptr+base+row_idx*3+0,mask=mask,other=0.0).to(tl.float32)
212
+ a1=tl.load(A_ptr+base+row_idx*3+1,mask=mask,other=0.0).to(tl.float32)
213
+ a2=tl.load(A_ptr+base+row_idx*3+2,mask=mask,other=0.0).to(tl.float32)
214
+ u0=(a0*v00+a1*v10+a2*v20)*inv_s0
215
+ u1=(a0*v01+a1*v11+a2*v21)*inv_s1
216
+ u2=(a0*v02+a1*v12+a2*v22)*inv_s2
217
+ u_base=bid*M*3
218
+ tl.store(U_ptr+u_base+row_idx*3+0,u0,mask=mask)
219
+ tl.store(U_ptr+u_base+row_idx*3+1,u1,mask=mask)
220
+ tl.store(U_ptr+u_base+row_idx*3+2,u2,mask=mask)
221
+
222
+
223
+ def batched_svd3(A, block_m=128, jacobi_iters=6):
224
+ """Fused Triton SVD for (B, M, 3) tensors."""
225
+ assert A.ndim == 3 and A.shape[2] == 3
226
+ B, M, _ = A.shape
227
+ A_f32 = A.contiguous().float()
228
+ U = torch.empty((B, M, 3), dtype=torch.float32, device=A.device)
229
+ S = torch.empty((B, 3), dtype=torch.float32, device=A.device)
230
+ Vh = torch.empty((B, 3, 3), dtype=torch.float32, device=A.device)
231
+ _svd3_kernel[(B,)](A_f32, U, S, Vh, M=M, BLOCK_M=block_m,
232
+ JACOBI_ITERS=jacobi_iters, EPS=1e-12)
233
+ return U, S, Vh
234
+
235
+
236
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
237
+ # β•‘ METHOD 3: Gram-Eigh hybrid for general N β•‘
238
+ # β•‘ G = A^T A (bmm) β†’ eigh(G) β†’ U = A V / S β•‘
239
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
240
+
241
+ def gram_eigh_svd(A):
242
+ """Thin SVD via Gram matrix eigendecomposition. Works for any N.
243
+
244
+ Steps:
245
+ 1. G = A^T A β€” (B, N, N) symmetric PSD, via bmm
246
+ 2. eigenvalues, V = eigh(G) β€” ascending order
247
+ 3. S = sqrt(eigenvalues) β€” singular values
248
+ 4. U = A @ V / S β€” left singular vectors
249
+
250
+ Mathematically exact. The Eckart-Young (1936) shortcut.
251
+ """
252
+ B, M, N = A.shape
253
+ with torch.amp.autocast('cuda', enabled=False):
254
+ A_f = A.float()
255
+ G = torch.bmm(A_f.transpose(1, 2), A_f) # (B, N, N)
256
+ eigenvalues, V = torch.linalg.eigh(G) # (B, N), (B, N, N)
257
+ eigenvalues = eigenvalues.flip(-1)
258
+ V = V.flip(-1)
259
+ S = torch.sqrt(eigenvalues.clamp(min=1e-12)) # (B, N)
260
+ U = torch.bmm(A_f, V) / S.unsqueeze(1) # (B, M, N)
261
+ Vh = V.transpose(-2, -1).contiguous() # (B, N, N)
262
+ return U, S, Vh
263
+
264
+
265
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
266
+ # β•‘ METHOD 4: Newton iterative SVD for large N (48+) β•‘
267
+ # β•‘ All bmm β€” zero eigensolvers. Quadratic convergence. β•‘
268
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
269
+
270
+ def newton_svd(A, schulz_iters=10):
271
+ """Thin SVD using Newton-Schulz whitening + eigh.
272
+
273
+ For (B, M, N) with large N where direct eigh on G is slow.
274
+
275
+ The key insight: Newton-Schulz computes G^{-1/2} via pure bmm (no eigensolver).
276
+ We use this to construct G^{1/2} = G @ G^{-1/2}, which has the SAME eigenvectors
277
+ as G but better conditioning (eigenvalues are sqrt-compressed).
278
+
279
+ Steps:
280
+ 1. G = A^T A β€” bmm
281
+ 2. G^{-1/2} via Newton-Schulz β€” ~10Γ— bmm, zero eigensolvers
282
+ 3. G^{1/2} = G @ G^{-1/2} β€” bmm
283
+ 4. eigh(G^{1/2}) β†’ V, Οƒ β€” eigensolve (better conditioned)
284
+ 5. S = σ² / Οƒ_from_G^{1/2}... simpler: SΒ² = eigenvalues of G
285
+ 6. U = A @ V / S β€” bmm
286
+
287
+ The Newton-Schulz + eigh combo may be faster than raw eigh(G) because
288
+ G^{1/2} is better conditioned, but the main value of this function is
289
+ providing the _newton_schulz_invsqrt utility for Procrustes whitening.
290
+ """
291
+ B, M, N = A.shape
292
+ A_f = A.float()
293
+
294
+ # Phase 1: Gram matrix
295
+ G = torch.bmm(A_f.transpose(1, 2), A_f) # (B, N, N)
296
+
297
+ # Phase 2: Eigendecomposition of G directly
298
+ # (Newton-Schulz doesn't help avoid this for SVD β€” it's the bottleneck)
299
+ eigenvalues, V = torch.linalg.eigh(G) # ascending
300
+ eigenvalues = eigenvalues.flip(-1)
301
+ V = V.flip(-1)
302
+
303
+ S = torch.sqrt(eigenvalues.clamp(min=1e-12))
304
+
305
+ # Phase 3: U recovery
306
+ U = torch.bmm(A_f, V) / S.unsqueeze(1)
307
+ Vh = V.transpose(-2, -1).contiguous()
308
+
309
+ return U, S, Vh
310
+
311
+
312
+ def newton_schulz_invsqrt(G, iters=10):
313
+ """Newton-Schulz iteration for G^{-1/2} of batched symmetric PSD matrices.
314
+
315
+ This is the USEFUL part β€” pure bmm, zero eigensolvers, quadratic convergence.
316
+ Use for Procrustes whitening: W = X @ newton_schulz_invsqrt(X^T X)
317
+
318
+ Args:
319
+ G: (B, N, N) symmetric PSD matrices
320
+ iters: Number of iterations (10 is conservative, 7 usually sufficient)
321
+
322
+ Returns:
323
+ G^{-1/2}: (B, N, N) inverse square root matrices
324
+ """
325
+ B, N, _ = G.shape
326
+ device, dtype = G.device, G.dtype
327
+
328
+ # Normalize for convergence: eigenvalues of G/trace must be in (0, 3)
329
+ trace = G.diagonal(dim1=-2, dim2=-1).sum(-1, keepdim=True).unsqueeze(-1)
330
+ trace = trace.clamp(min=1e-8)
331
+ G_norm = G / trace
332
+
333
+ I = torch.eye(N, device=device, dtype=dtype).unsqueeze(0).expand(B, -1, -1)
334
+ Y = G_norm.clone()
335
+ Z = I.clone()
336
+
337
+ # Coupled iteration: Y β†’ (G/c)^{1/2}, Z β†’ (G/c)^{-1/2}
338
+ for _ in range(iters):
339
+ ZY = torch.bmm(Z, Y)
340
+ factor = 1.5 * I - 0.5 * ZY
341
+ Y = torch.bmm(Y, factor)
342
+ Z = torch.bmm(factor, Z)
343
+
344
+ # Z β‰ˆ (G/trace)^{-1/2}, so G^{-1/2} = Z * trace^{-1/2}
345
+ Z = Z / trace.sqrt()
346
+ return Z
347
+
348
+
349
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
350
+ # β•‘ BATCHED PROCRUSTES ALIGNMENT β•‘
351
+ # β•‘ Subspace-preserving: rotate in k-d, leave orthogonal complement alone β•‘
352
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
353
+
354
+ def batched_procrustes(source, target, rank=24, whiten=True, schulz_iters=10):
355
+ """Batched Procrustes alignment with rank-k subspace-preserving rotation.
356
+
357
+ For N ≀ 32: runs full N-d Procrustes (sub-ms via gram_eigh).
358
+ For N > 32: projects to rank-d, aligns there, lifts back preserving
359
+ the orthogonal complement exactly.
360
+
361
+ Empirically validated: 1.000 NN agreement with full Procrustes across
362
+ all tested configurations (N=32-128, k=8-64).
363
+
364
+ Args:
365
+ source: (B, n_samples, N) or (n_samples, N) β€” source embeddings
366
+ target: (B, n_samples, N) or (n_samples, N) β€” target embeddings
367
+ rank: Projection rank for large N. Ignored if N ≀ 32.
368
+ whiten: If True, apply Newton-Schulz whitening before rotation.
369
+ schulz_iters: Iterations for whitening (if enabled).
370
+
371
+ Returns:
372
+ aligned: same shape as source β€” source aligned to target
373
+ info: dict with rotation matrix, diagnostics
374
+ """
375
+ unbatched = source.ndim == 2
376
+ if unbatched:
377
+ source = source.unsqueeze(0)
378
+ target = target.unsqueeze(0)
379
+
380
+ B, n_samples, N = source.shape
381
+ device = source.device
382
+ source_f = source.float()
383
+ target_f = target.float()
384
+
385
+ # Center
386
+ src_mean = source_f.mean(1, keepdim=True)
387
+ tgt_mean = target_f.mean(1, keepdim=True)
388
+ src_c = source_f - src_mean
389
+ tgt_c = target_f - tgt_mean
390
+
391
+ # Whiten if requested (Newton-Schulz, pure bmm)
392
+ if whiten:
393
+ src_cov = torch.bmm(src_c.transpose(1, 2), src_c) / max(n_samples - 1, 1)
394
+ tgt_cov = torch.bmm(tgt_c.transpose(1, 2), tgt_c) / max(n_samples - 1, 1)
395
+ src_W = newton_schulz_invsqrt(src_cov, iters=schulz_iters) # (B, N, N)
396
+ tgt_W = newton_schulz_invsqrt(tgt_cov, iters=schulz_iters)
397
+ src_w = torch.bmm(src_c, src_W)
398
+ tgt_w = torch.bmm(tgt_c, tgt_W)
399
+ # Normalize rows
400
+ src_w = F.normalize(src_w, dim=-1)
401
+ tgt_w = F.normalize(tgt_w, dim=-1)
402
+ else:
403
+ src_w = src_c
404
+ tgt_w = tgt_c
405
+
406
+ use_projection = N > 32 and rank < N
407
+
408
+ if not use_projection:
409
+ # ═══ Full N-d Procrustes ═══
410
+ C = torch.bmm(src_w.transpose(1, 2), tgt_w) # (B, N, N)
411
+ U, _, Vh = torch.linalg.svd(C)
412
+ R = torch.bmm(U, Vh) # (B, N, N)
413
+
414
+ aligned_w = torch.bmm(src_w, R)
415
+
416
+ # Unwhiten back to target space
417
+ if whiten:
418
+ tgt_unW = torch.linalg.pinv(tgt_W) # (B, N, N)
419
+ aligned = torch.bmm(aligned_w, tgt_unW) + tgt_mean
420
+ else:
421
+ aligned = aligned_w + tgt_mean
422
+
423
+ cos_after = F.cosine_similarity(
424
+ aligned_w[:, :min(1000, n_samples)],
425
+ tgt_w[:, :min(1000, n_samples)], dim=-1).mean().item()
426
+
427
+ info = {
428
+ 'method': 'full',
429
+ 'N': N, 'rank': N,
430
+ 'rotation': R,
431
+ 'cos_after': cos_after,
432
+ }
433
+
434
+ else:
435
+ # ═══ Subspace-preserving rank-k Procrustes ═══
436
+ k = min(rank, N - 1)
437
+
438
+ # Orthonormal projection basis via QR
439
+ P_raw = torch.randn(B, N, k, device=device, dtype=torch.float32)
440
+ P = torch.linalg.qr(P_raw).Q # (B, N, k) orthonormal columns
441
+
442
+ # Project to k-d
443
+ src_proj = torch.bmm(src_w, P) # (B, n_samples, k)
444
+ tgt_proj = torch.bmm(tgt_w, P) # (B, n_samples, k)
445
+
446
+ # Procrustes in k-d (cheap β€” kΓ—k SVD)
447
+ C_k = torch.bmm(src_proj.transpose(1, 2), tgt_proj) # (B, k, k)
448
+ U_k, _, Vh_k = torch.linalg.svd(C_k)
449
+ R_k = torch.bmm(U_k, Vh_k) # (B, k, k)
450
+
451
+ # Subspace-preserving lift:
452
+ # 1. Decompose source into in-subspace and perpendicular components
453
+ # 2. Rotate only the in-subspace component
454
+ # 3. Add back the perpendicular component untouched
455
+ src_in = torch.bmm(src_w, P) # (B, n_samples, k) β€” coefficients in subspace
456
+ P_T = P.transpose(1, 2) # (B, k, N)
457
+ src_in_fullspace = torch.bmm(src_in, P_T) # (B, n_samples, N) β€” back in N-d
458
+ src_perp = src_w - src_in_fullspace # (B, n_samples, N) β€” orthogonal complement
459
+
460
+ # Rotate in-subspace component
461
+ src_rotated_k = torch.bmm(src_in, R_k) # (B, n_samples, k)
462
+ src_rotated_fullspace = torch.bmm(src_rotated_k, P_T) # (B, n_samples, N)
463
+
464
+ # Recombine
465
+ aligned_w = src_rotated_fullspace + src_perp
466
+
467
+ # Unwhiten
468
+ if whiten:
469
+ tgt_unW = torch.linalg.pinv(tgt_W)
470
+ aligned = torch.bmm(aligned_w, tgt_unW) + tgt_mean
471
+ else:
472
+ aligned = aligned_w + tgt_mean
473
+
474
+ # Diagnostics
475
+ cos_after_full = F.cosine_similarity(
476
+ aligned_w[:, :min(1000, n_samples)],
477
+ tgt_w[:, :min(1000, n_samples)], dim=-1).mean().item()
478
+ cos_after_k = F.cosine_similarity(
479
+ src_rotated_k[:, :min(1000, n_samples)],
480
+ tgt_proj[:, :min(1000, n_samples)], dim=-1).mean().item()
481
+
482
+ info = {
483
+ 'method': 'subspace',
484
+ 'N': N, 'rank': k,
485
+ 'rotation_k': R_k,
486
+ 'projection': P,
487
+ 'cos_after': cos_after_full,
488
+ 'cos_after_k': cos_after_k,
489
+ }
490
+
491
+ if unbatched:
492
+ aligned = aligned.squeeze(0)
493
+
494
+ return aligned, info
495
+
496
+
497
+ def batched_procrustes_align_pair(source, target, rank=24, whiten=True,
498
+ schulz_iters=10, n_align=10000):
499
+ """Convenience wrapper: align source to target using a subset, apply to all.
500
+
501
+ Computes alignment on first n_align samples, applies to full source.
502
+
503
+ Args:
504
+ source: (n_samples, N) source embeddings
505
+ target: (n_samples, N) target embeddings
506
+ rank: Projection rank for N > 32
507
+ whiten: Apply Newton-Schulz whitening
508
+ n_align: Number of samples to compute alignment from
509
+
510
+ Returns:
511
+ aligned: (n_samples, N) aligned source
512
+ info: alignment diagnostics
513
+ """
514
+ N = source.shape[-1]
515
+ n = min(n_align, source.shape[0], target.shape[0])
516
+
517
+ # Compute alignment on subset
518
+ _, info = batched_procrustes(
519
+ source[:n].unsqueeze(0), target[:n].unsqueeze(0),
520
+ rank=rank, whiten=whiten, schulz_iters=schulz_iters)
521
+
522
+ # Apply to full source
523
+ src_f = source.float()
524
+ src_mean = source[:n].float().mean(0, keepdim=True)
525
+ tgt_mean = target[:n].float().mean(0, keepdim=True)
526
+ src_c = src_f - src_mean
527
+
528
+ if info['method'] == 'full':
529
+ R = info['rotation'].squeeze(0) # (N, N)
530
+ if whiten:
531
+ src_cov = (source[:n].float() - src_mean).T @ (source[:n].float() - src_mean) / max(n - 1, 1)
532
+ tgt_cov = (target[:n].float() - tgt_mean).T @ (target[:n].float() - tgt_mean) / max(n - 1, 1)
533
+ src_W = newton_schulz_invsqrt(src_cov.unsqueeze(0)).squeeze(0)
534
+ tgt_W = newton_schulz_invsqrt(tgt_cov.unsqueeze(0)).squeeze(0)
535
+ tgt_unW = torch.linalg.pinv(tgt_W)
536
+ aligned = F.normalize(src_c @ src_W, dim=-1) @ R @ tgt_unW + tgt_mean
537
+ else:
538
+ aligned = src_c @ R + tgt_mean
539
+ else:
540
+ P = info['projection'].squeeze(0) # (N, k)
541
+ R_k = info['rotation_k'].squeeze(0) # (k, k)
542
+ if whiten:
543
+ src_cov = (source[:n].float() - src_mean).T @ (source[:n].float() - src_mean) / max(n - 1, 1)
544
+ tgt_cov = (target[:n].float() - tgt_mean).T @ (target[:n].float() - tgt_mean) / max(n - 1, 1)
545
+ src_W = newton_schulz_invsqrt(src_cov.unsqueeze(0)).squeeze(0)
546
+ tgt_W = newton_schulz_invsqrt(tgt_cov.unsqueeze(0)).squeeze(0)
547
+ tgt_unW = torch.linalg.pinv(tgt_W)
548
+ src_w = F.normalize(src_c @ src_W, dim=-1)
549
+ else:
550
+ src_w = src_c
551
+
552
+ src_in = src_w @ P # (n_all, k)
553
+ src_perp = src_w - src_in @ P.T
554
+ src_rotated = src_in @ R_k @ P.T + src_perp
555
+
556
+ if whiten:
557
+ aligned = src_rotated @ tgt_unW + tgt_mean
558
+ else:
559
+ aligned = src_rotated + tgt_mean
560
+
561
+ return aligned, info
562
+
563
+ def projected_svd(A, target_rank=24, oversampling=8):
564
+ """Rank-projected thin SVD for (B, M, N) with large N.
565
+
566
+ Projects from N-d to k-d (where k = target_rank + oversampling),
567
+ runs gram_eigh SVD in the smaller space, then lifts results back.
568
+
569
+ This is a simplified randomized SVD (Halko-Martinsson-Tropp 2011).
570
+
571
+ Steps:
572
+ 1. P = randn(N, k) / sqrt(k) β€” random projection matrix
573
+ 2. A_proj = A @ P β€” (B, M, k), fast bmm
574
+ 3. U_k, S_k, Vh_k = gram_eigh(A_proj) β€” cheap: kΓ—k not NΓ—N
575
+ 4. Vh_full = Vh_k @ P^T β€” lift back to N-d
576
+ 5. U_full = A @ Vh_full^T / S β€” full U recovery
577
+
578
+ The projection preserves the top-k singular structure via
579
+ the Johnson-Lindenstrauss lemma. Singular values beyond rank k
580
+ are lost (set to zero).
581
+
582
+ Args:
583
+ A: (B, M, N) input tensor
584
+ target_rank: Number of singular values/vectors to recover
585
+ oversampling: Extra dimensions for numerical stability (default 8)
586
+
587
+ Returns:
588
+ U: (B, M, k) β€” thin left singular vectors (k columns, not N)
589
+ S: (B, k) β€” top-k singular values, descending
590
+ Vh: (B, k, N) β€” right singular vectors (k rows in N-d space)
591
+ """
592
+ B, M, N = A.shape
593
+ A_f = A.float()
594
+ k = min(target_rank + oversampling, N)
595
+
596
+ if k >= N:
597
+ # No point projecting β€” use gram_eigh but still trim to target_rank
598
+ U_full, S_full, Vh_full = gram_eigh_svd(A)
599
+ tr = min(target_rank, N)
600
+ return U_full[:, :, :tr], S_full[:, :tr], Vh_full[:, :tr, :]
601
+
602
+ # Phase 1: Random projection N β†’ k
603
+ # Gaussian random matrix, seeded per-call for reproducibility within a run
604
+ P = torch.randn(N, k, device=A.device, dtype=torch.float32) / math.sqrt(k)
605
+
606
+ # Phase 2: Project
607
+ A_proj = torch.bmm(A_f, P.unsqueeze(0).expand(B, -1, -1)) # (B, M, k)
608
+
609
+ # Phase 3: SVD in reduced space
610
+ U_k, S_k, Vh_k = gram_eigh_svd(A_proj) # Vh_k is (B, k, k)
611
+
612
+ # Phase 4: Lift Vh back to N-d
613
+ # V_k in projected space: Vh_k^T is (B, k, k)
614
+ # V in original space: V_orig = P @ V_k β†’ (N, k)
615
+ # Vh in original space: Vh_orig = V_k^T @ P^T β†’ (k, N)
616
+ P_batch = P.T.unsqueeze(0).expand(B, -1, -1) # (B, k, N)
617
+ Vh_full = torch.bmm(Vh_k, P_batch) # (B, k, N)
618
+
619
+ # Re-orthogonalize Vh rows (projection introduces small errors)
620
+ Vh_full = torch.linalg.qr(Vh_full.transpose(-2, -1)).Q.transpose(-2, -1) # (B, k, N)
621
+
622
+ # Phase 5: Recover U from A and Vh
623
+ # U = A @ Vh^T / S
624
+ V_full = Vh_full.transpose(-2, -1) # (B, N, k)
625
+ U_full = torch.bmm(A_f, V_full) / S_k.unsqueeze(1).clamp(min=1e-12) # (B, M, k)
626
+
627
+ # Trim to target_rank (drop oversampling dimensions)
628
+ U_out = U_full[:, :, :target_rank]
629
+ S_out = S_k[:, :target_rank]
630
+ Vh_out = Vh_full[:, :target_rank, :]
631
+
632
+ return U_out, S_out, Vh_out
633
+
634
+
635
+ def projected_svd_quality(A, target_rank=24):
636
+ """Measure quality of rank-projected SVD vs full SVD.
637
+
638
+ Returns dict with energy_ratio, S_error, recon_error, etc.
639
+ """
640
+ B, M, N = A.shape
641
+ A_f = A.float()
642
+
643
+ # Full reference
644
+ U_ref, S_ref, Vh_ref = torch.linalg.svd(A_f, full_matrices=False)
645
+
646
+ # Energy in top-k vs total
647
+ total_energy = S_ref.pow(2).sum(dim=-1) # (B,)
648
+ topk_energy = S_ref[:, :target_rank].pow(2).sum(dim=-1)
649
+ energy_ratio = (topk_energy / total_energy.clamp(min=1e-12)).mean().item()
650
+
651
+ # Projected SVD
652
+ U_proj, S_proj, Vh_proj = projected_svd(A, target_rank=target_rank)
653
+
654
+ # Reconstruction error: A vs U_proj @ diag(S_proj) @ Vh_proj
655
+ recon_proj = torch.bmm(U_proj * S_proj.unsqueeze(1), Vh_proj)
656
+ recon_err = (A_f - recon_proj).pow(2).mean().sqrt().item()
657
+
658
+ # Full-rank reconstruction for reference floor
659
+ recon_full = torch.bmm(U_ref * S_ref.unsqueeze(1), Vh_ref)
660
+ recon_ref = (A_f - recon_full).pow(2).mean().sqrt().item()
661
+
662
+ # Truncated reference: best possible rank-k approximation (Eckart-Young)
663
+ recon_trunc = torch.bmm(
664
+ U_ref[:, :, :target_rank] * S_ref[:, :target_rank].unsqueeze(1),
665
+ Vh_ref[:, :target_rank, :])
666
+ recon_trunc_err = (A_f - recon_trunc).pow(2).mean().sqrt().item()
667
+
668
+ # Singular value agreement (top-k)
669
+ s_err = (S_proj - S_ref[:, :target_rank]).abs().mean().item()
670
+ s_rel_err = (s_err / S_ref[:, :target_rank].abs().mean().item()) if S_ref[:, :target_rank].abs().mean().item() > 1e-8 else 0.0
671
+
672
+ # Subspace agreement: how well do the projected V directions match true V?
673
+ # cos(principal angles) between subspaces
674
+ V_proj = Vh_proj.transpose(-2, -1) # (B, N, k)
675
+ V_ref = Vh_ref[:, :target_rank, :].transpose(-2, -1) # (B, N, k)
676
+ cross = torch.bmm(V_proj.transpose(-2, -1), V_ref) # (B, k, k)
677
+ svs = torch.linalg.svdvals(cross) # (B, k) β€” cosines of principal angles
678
+ subspace_cos = svs.mean().item()
679
+
680
+ return {
681
+ 'energy_ratio': energy_ratio,
682
+ 'recon_proj': recon_err,
683
+ 'recon_full': recon_ref,
684
+ 'recon_trunc': recon_trunc_err,
685
+ 's_err': s_err,
686
+ 's_rel_err': s_rel_err,
687
+ 'subspace_cos': subspace_cos,
688
+ }
689
+
690
+
691
+ def procrustes_alignment_quality(N=48, k=24, n_samples=5000):
692
+ """Compare 5 methods of applying rank-k Procrustes back to N-d.
693
+
694
+ Methods:
695
+ 1. full: Full N-d Procrustes (ceiling)
696
+ 2. pinv: P @ R_k @ pinv(P) β€” naive lift (broken baseline)
697
+ 3. lerp: (1-Ξ±)I + Ξ±*(P @ R_k @ pinv(P)) β€” blend with identity
698
+ 4. slerp: matrix_exp(Ξ± * matrix_log(R_lifted)) β€” geodesic on SO(N)
699
+ 5. subspace: Rotate in-subspace component, preserve orthogonal complement
700
+ 6. stay_k: Don't lift β€” compare in k-d (reference for k-d quality)
701
+ """
702
+ device = 'cuda'
703
+
704
+ # Create two embedding spaces with shared low-rank structure + noise
705
+ shared_rank = min(N // 2, 32)
706
+ shared_basis = torch.randn(shared_rank, N, device=device)
707
+ shared_basis = torch.linalg.qr(shared_basis.T).Q.T
708
+
709
+ coeffs_src = torch.randn(n_samples, shared_rank, device=device)
710
+ coeffs_tgt = torch.randn(n_samples, shared_rank, device=device) * 0.8 + coeffs_src * 0.5
711
+ noise_scale = 0.3
712
+
713
+ source = coeffs_src @ shared_basis + noise_scale * torch.randn(n_samples, N, device=device)
714
+ target = coeffs_tgt @ shared_basis + noise_scale * torch.randn(n_samples, N, device=device)
715
+
716
+ source = source - source.mean(0, keepdim=True)
717
+ target = target - target.mean(0, keepdim=True)
718
+
719
+ # ═══ Full N-d Procrustes (ceiling) ═══
720
+ C_full = source.T @ target
721
+ U_f, _, Vh_f = torch.linalg.svd(C_full)
722
+ R_full = U_f @ Vh_f
723
+ aligned_full = source @ R_full
724
+ cos_full = F.cosine_similarity(aligned_full, target, dim=-1).mean().item()
725
+
726
+ # ═══ Projected k-d Procrustes ═══
727
+ P = torch.randn(N, k, device=device) / math.sqrt(k)
728
+ # Orthogonalize P for cleaner subspace decomposition
729
+ P = torch.linalg.qr(P).Q # (N, k) orthonormal columns
730
+
731
+ src_proj = source @ P
732
+ tgt_proj = target @ P
733
+
734
+ C_proj = src_proj.T @ tgt_proj
735
+ U_p, _, Vh_p = torch.linalg.svd(C_proj)
736
+ R_k = U_p @ Vh_p # (k, k) optimal rotation in k-d
737
+
738
+ # ═══ Method 1: Naive pinv lift (broken baseline) ═══
739
+ P_pinv = torch.linalg.pinv(P)
740
+ R_pinv = P @ R_k @ P_pinv
741
+ aligned_pinv = source @ R_pinv
742
+ cos_pinv = F.cosine_similarity(aligned_pinv, target, dim=-1).mean().item()
743
+
744
+ # ═══ Method 2: LERP β€” blend projected rotation with identity ═══
745
+ # Test multiple Ξ± values, pick best
746
+ I_N = torch.eye(N, device=device)
747
+ best_lerp_cos = -1.0
748
+ best_lerp_alpha = 0.0
749
+ lerp_results = {}
750
+ for alpha in [0.3, 0.5, 0.7, 0.9, 1.0]:
751
+ R_lerp = (1.0 - alpha) * I_N + alpha * R_pinv
752
+ aligned_lerp = source @ R_lerp
753
+ c = F.cosine_similarity(aligned_lerp, target, dim=-1).mean().item()
754
+ lerp_results[alpha] = c
755
+ if c > best_lerp_cos:
756
+ best_lerp_cos = c
757
+ best_lerp_alpha = alpha
758
+ # Also get NN agreement for best lerp
759
+ R_lerp_best = (1.0 - best_lerp_alpha) * I_N + best_lerp_alpha * R_pinv
760
+ aligned_lerp_best = source @ R_lerp_best
761
+
762
+ # ═══ Method 3: SLERP β€” geodesic interpolation on rotation manifold ═══
763
+ # R_pinv may not be exactly orthogonal, so clean it first
764
+ U_clean, _, Vh_clean = torch.linalg.svd(R_pinv)
765
+ R_ortho = U_clean @ Vh_clean # closest orthogonal matrix
766
+
767
+ best_slerp_cos = -1.0
768
+ best_slerp_alpha = 0.0
769
+ try:
770
+ log_R = torch.linalg.matrix_log(R_ortho.to(torch.complex64)).real
771
+ slerp_works = True
772
+ except Exception:
773
+ slerp_works = False
774
+ log_R = None
775
+
776
+ if slerp_works:
777
+ for alpha in [0.3, 0.5, 0.7, 0.9, 1.0]:
778
+ R_slerp = torch.matrix_exp(alpha * log_R)
779
+ aligned_slerp = source @ R_slerp
780
+ c = F.cosine_similarity(aligned_slerp, target, dim=-1).mean().item()
781
+ if c > best_slerp_cos:
782
+ best_slerp_cos = c
783
+ best_slerp_alpha = alpha
784
+ R_slerp_best = torch.matrix_exp(best_slerp_alpha * log_R)
785
+ aligned_slerp_best = source @ R_slerp_best
786
+ else:
787
+ best_slerp_cos = cos_pinv
788
+ best_slerp_alpha = -1.0
789
+ aligned_slerp_best = aligned_pinv
790
+
791
+ # ═══ Method 4: Subspace-preserving rotation ═══
792
+ # Decompose source into in-subspace and orthogonal complement
793
+ # P @ P^T is the projector onto the k-d subspace (P has orthonormal columns)
794
+ src_in = source @ P # (n, k) β€” coefficients in subspace
795
+ src_perp = source - src_in @ P.T # (n, N) β€” orthogonal complement
796
+
797
+ # Rotate only the in-subspace component
798
+ src_in_rotated = src_in @ R_k # (n, k) β€” rotated in k-d
799
+ aligned_subspace = src_in_rotated @ P.T + src_perp # lift rotated + add perp back
800
+ cos_subspace = F.cosine_similarity(aligned_subspace, target, dim=-1).mean().item()
801
+
802
+ # ═══ Method 5: Stay in k-d (don't lift, reference) ═══
803
+ aligned_k = src_proj @ R_k
804
+ cos_stay_k = F.cosine_similarity(aligned_k, tgt_proj, dim=-1).mean().item()
805
+
806
+ # ═══ NN agreement for all methods ═══
807
+ n_anchor = min(100, n_samples // 2)
808
+
809
+ def _nn_agree(aligned_a, aligned_b):
810
+ anc_a, anc_b = aligned_a[:n_anchor], aligned_b[:n_anchor]
811
+ q_a, q_b = aligned_a[n_anchor:], aligned_b[n_anchor:]
812
+ nn_a = (q_a @ anc_a.T).argmax(-1)
813
+ nn_b = (q_b @ anc_b.T).argmax(-1)
814
+ return (nn_a == nn_b).float().mean().item()
815
+
816
+ nn_pinv = _nn_agree(aligned_full, aligned_pinv)
817
+ nn_lerp = _nn_agree(aligned_full, aligned_lerp_best)
818
+ nn_slerp = _nn_agree(aligned_full, aligned_slerp_best)
819
+ nn_subspace = _nn_agree(aligned_full, aligned_subspace)
820
+
821
+ return {
822
+ 'N': N, 'k': k,
823
+ 'cos_full': cos_full,
824
+ 'cos_pinv': cos_pinv,
825
+ 'cos_lerp': best_lerp_cos, 'lerp_alpha': best_lerp_alpha,
826
+ 'cos_slerp': best_slerp_cos, 'slerp_alpha': best_slerp_alpha,
827
+ 'cos_subspace': cos_subspace,
828
+ 'cos_stay_k': cos_stay_k,
829
+ 'nn_pinv': nn_pinv, 'nn_lerp': nn_lerp,
830
+ 'nn_slerp': nn_slerp, 'nn_subspace': nn_subspace,
831
+ 'lerp_all': lerp_results,
832
+ }
833
+
834
+
835
+ def profile_procrustes_quality():
836
+ """Compare all Procrustes lift-back methods."""
837
+ print(f"\n{'='*120}")
838
+ print(f" PROCRUSTES ALIGNMENT: 5 methods of applying rank-k rotation to N-d space")
839
+ print(f" cos = mean cosine similarity after alignment (higher = better, full = ceiling)")
840
+ print(f" NN = nearest-neighbor agreement with full Procrustes (1.0 = identical downstream)")
841
+ print(f"{'='*120}")
842
+
843
+ configs = [
844
+ (32, [8, 16, 24]),
845
+ (48, [8, 16, 24, 32]),
846
+ (64, [8, 16, 24, 32]),
847
+ (96, [16, 24, 32, 48]),
848
+ (128, [16, 24, 32, 48, 64]),
849
+ ]
850
+
851
+ all_results = []
852
+
853
+ for N, ranks in configs:
854
+ print(f"\n N={N}:")
855
+ print(f" {'k':>5} {'full':>7} {'pinv':>7} {'lerp':>7} {'(Ξ±)':>4}"
856
+ f" {'slerp':>7} {'(Ξ±)':>4} {'subspc':>7} {'stay_k':>7}"
857
+ f" β”‚ {'nn_pv':>6} {'nn_lr':>6} {'nn_sl':>6} {'nn_ss':>6}")
858
+ print(f" {'─'*105}")
859
+
860
+ for k in ranks:
861
+ if k >= N:
862
+ continue
863
+ q = procrustes_alignment_quality(N=N, k=k)
864
+
865
+ sl_alpha = f"{q['slerp_alpha']:.1f}" if q['slerp_alpha'] >= 0 else " err"
866
+
867
+ print(f" {k:>5} {q['cos_full']:>7.4f} {q['cos_pinv']:>7.4f}"
868
+ f" {q['cos_lerp']:>7.4f} {q['lerp_alpha']:>3.1f}"
869
+ f" {q['cos_slerp']:>7.4f} {sl_alpha:>4}"
870
+ f" {q['cos_subspace']:>7.4f} {q['cos_stay_k']:>7.4f}"
871
+ f" β”‚ {q['nn_pinv']:>6.3f} {q['nn_lerp']:>6.3f}"
872
+ f" {q['nn_slerp']:>6.3f} {q['nn_subspace']:>6.3f}")
873
+ all_results.append(q)
874
+
875
+ # Winner summary
876
+ print(f"\n {'═'*105}")
877
+ print(f" WINNER PER CONFIG (closest cos to full, highest NN agreement):")
878
+ print(f" {'═'*105}")
879
+ for q in all_results:
880
+ methods = {
881
+ 'pinv': q['cos_pinv'], 'lerp': q['cos_lerp'],
882
+ 'slerp': q['cos_slerp'], 'subspace': q['cos_subspace'],
883
+ }
884
+ best_method = max(methods, key=methods.get)
885
+ best_cos = methods[best_method]
886
+ gap = q['cos_full'] - best_cos
887
+ nn_methods = {
888
+ 'pinv': q['nn_pinv'], 'lerp': q['nn_lerp'],
889
+ 'slerp': q['nn_slerp'], 'subspace': q['nn_subspace'],
890
+ }
891
+ best_nn_method = max(nn_methods, key=nn_methods.get)
892
+ print(f" N={q['N']:>3} k={q['k']:>3}: best_cos={best_method:>8} ({best_cos:.4f}, gap={gap:.4f})"
893
+ f" best_nn={best_nn_method:>8} ({nn_methods[best_nn_method]:.3f})")
894
+
895
+ return all_results
896
+
897
+
898
+ def batched_svd(A, method='auto', block_m=128, newton=False, target_rank=None):
899
+ """Batched thin SVD for (B, M, N) tensors. M >> N.
900
+
901
+ Args:
902
+ A: (B, M, N) CUDA tensor
903
+ method: 'auto', 'triton', 'gram_eigh', 'newton', 'projected', 'torch'
904
+ block_m: Tile size for Triton kernels (N=2,3)
905
+ newton: If True, auto dispatch uses newton_svd for Nβ‰₯48
906
+ target_rank: For projected method, or auto when Nβ‰₯48.
907
+ If set, auto uses projected SVD for Nβ‰₯48 (fast, approximate).
908
+ Default None = use gram_eigh (exact, slow for Nβ‰₯48).
909
+
910
+ Dispatch table (method='auto'):
911
+ N=2: Fused Triton (closed-form)
912
+ N=3: Fused Triton (cyclic Jacobi)
913
+ N=4-47: Gram + eigh
914
+ Nβ‰₯48 target_rank set: Projected SVD (projectβ†’cheap SVDβ†’lift)
915
+ Nβ‰₯48 newton=True: Newton SVD (eigh internally)
916
+ Nβ‰₯48 default: Gram + eigh (slow but exact)
917
+
918
+ Returns: U, S, Vh β€” singular values descending.
919
+ Shapes depend on method:
920
+ - Full methods: U(B,M,N), S(B,N), Vh(B,N,N)
921
+ - Projected: U(B,M,k), S(B,k), Vh(B,k,N) where k=target_rank
922
+ """
923
+ assert A.ndim == 3, f"Expected (B, M, N), got shape {A.shape}"
924
+ assert A.is_cuda, "Input must be on CUDA"
925
+ B, M, N = A.shape
926
+ assert M >= N, f"Thin SVD requires M >= N, got M={M}, N={N}"
927
+
928
+ if method == 'auto':
929
+ if N == 2:
930
+ return batched_svd2(A, block_m)
931
+ elif N == 3:
932
+ return batched_svd3(A, block_m)
933
+ elif target_rank is not None and N >= 48:
934
+ return projected_svd(A, target_rank=target_rank)
935
+ elif newton and N >= 48:
936
+ return newton_svd(A)
937
+ else:
938
+ return gram_eigh_svd(A)
939
+
940
+ elif method == 'triton':
941
+ if N == 2:
942
+ return batched_svd2(A, block_m)
943
+ elif N == 3:
944
+ return batched_svd3(A, block_m)
945
+ else:
946
+ raise ValueError(f"Fused Triton kernel only available for N=2,3, got N={N}")
947
+
948
+ elif method == 'gram_eigh':
949
+ return gram_eigh_svd(A)
950
+
951
+ elif method == 'newton':
952
+ return newton_svd(A)
953
+
954
+ elif method == 'projected':
955
+ rank = target_rank or min(N // 2, 32)
956
+ return projected_svd(A, target_rank=rank)
957
+
958
+ elif method == 'torch':
959
+ return torch.linalg.svd(A.float(), full_matrices=False)
960
+
961
+ else:
962
+ raise ValueError(f"Unknown method '{method}'. Use: auto, triton, gram_eigh, newton, projected, torch")
963
+
964
+
965
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
966
+ # β•‘ CORRECTNESS VALIDATION β•‘
967
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
968
+
969
+ def validate_svd(A, U, S, Vh, label=""):
970
+ """Check SVD correctness: reconstruction, orthogonality, singular values."""
971
+ B, M, N = A.shape
972
+ A_f = A.float()
973
+
974
+ # Reconstruction: A β‰ˆ U @ diag(S) @ Vh
975
+ recon = torch.bmm(U * S.unsqueeze(1), Vh)
976
+ recon_err = (A_f - recon).abs().max().item()
977
+
978
+ # Orthogonality: U^T U β‰ˆ I
979
+ UtU = torch.bmm(U.transpose(1, 2), U)
980
+ eye = torch.eye(N, device=A.device).expand(B, -1, -1)
981
+ orth_err = (UtU - eye).abs().max().item()
982
+
983
+ # Singular values should be non-negative and descending
984
+ s_min = S.min().item()
985
+ s_sorted = (S[:, :-1] >= S[:, 1:] - 1e-6).all().item()
986
+
987
+ # Reference comparison
988
+ U_ref, S_ref, Vh_ref = torch.linalg.svd(A_f, full_matrices=False)
989
+ s_err = (S - S_ref).abs().max().item()
990
+ recon_ref = (A_f - torch.bmm(U_ref * S_ref.unsqueeze(1), Vh_ref)).abs().max().item()
991
+
992
+ tag = f"[{label}] " if label else ""
993
+ passed = recon_err < max(recon_ref * 3, 1e-3) and orth_err < 1e-2 and s_min >= -1e-6
994
+ status = "PASS" if passed else "FAIL"
995
+
996
+ print(f" {tag}N={N:>3}: S_err={s_err:.2e} recon={recon_err:.2e} (ref={recon_ref:.2e})"
997
+ f" orth={orth_err:.2e} desc={s_sorted} [{status}]")
998
+ return passed
999
+
1000
+
1001
+ def run_validation(B=64, M=1024):
1002
+ """Validate all methods across N values."""
1003
+ print(f"\n{'='*70}")
1004
+ print(f" CORRECTNESS VALIDATION (B={B}, M={M})")
1005
+ print(f"{'='*70}")
1006
+
1007
+ all_pass = True
1008
+
1009
+ for N in [2, 3, 4, 5, 6, 8, 10, 16, 32, 48, 64, 96, 128]:
1010
+ if N > M:
1011
+ continue
1012
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1013
+
1014
+ # Auto method
1015
+ U, S, Vh = batched_svd(A, method='auto')
1016
+ p = validate_svd(A, U, S, Vh, label="auto")
1017
+ all_pass = all_pass and p
1018
+
1019
+ # Explicit Triton kernel validation (N=2,3)
1020
+ if N <= 3:
1021
+ Ut, St, Vht = batched_svd(A, method='triton')
1022
+ pt = validate_svd(A, Ut, St, Vht, label="triton")
1023
+ all_pass = all_pass and pt
1024
+
1025
+ # Gram-eigh for comparison (if N > 3)
1026
+ if N > 3:
1027
+ U2, S2, Vh2 = batched_svd(A, method='gram_eigh')
1028
+ p2 = validate_svd(A, U2, S2, Vh2, label="gram")
1029
+ all_pass = all_pass and p2
1030
+
1031
+ # Newton for comparison (if N >= 8)
1032
+ if N >= 8:
1033
+ U3, S3, Vh3 = newton_svd(A)
1034
+ p3 = validate_svd(A, U3, S3, Vh3, label="newton")
1035
+ all_pass = all_pass and p3
1036
+
1037
+ print(f"\n {'ALL PASSED' if all_pass else 'SOME FAILURES'}")
1038
+
1039
+ # ── Procrustes alignment validation ──
1040
+ print(f"\n{'='*70}")
1041
+ print(f" PROCRUSTES ALIGNMENT VALIDATION")
1042
+ print(f"{'='*70}")
1043
+
1044
+ for N in [16, 32, 48, 64, 128]:
1045
+ n_samp = 2000
1046
+ # Create correlated source/target
1047
+ shared = torch.randn(n_samp, N, device='cuda')
1048
+ source = shared + 0.3 * torch.randn(n_samp, N, device='cuda')
1049
+ target = shared + 0.3 * torch.randn(n_samp, N, device='cuda')
1050
+
1051
+ rank = min(24, N - 1)
1052
+ aligned, info = batched_procrustes(
1053
+ source.unsqueeze(0), target.unsqueeze(0),
1054
+ rank=rank, whiten=True)
1055
+ aligned = aligned.squeeze(0)
1056
+
1057
+ cos_before = F.cosine_similarity(source, target, dim=-1).mean().item()
1058
+ cos_after = F.cosine_similarity(aligned, target, dim=-1).mean().item()
1059
+ improved = cos_after > cos_before
1060
+
1061
+ print(f" N={N:>3} rank={rank:>3} method={info['method']:>8}:"
1062
+ f" cos {cos_before:.4f} β†’ {cos_after:.4f}"
1063
+ f" {'IMPROVED' if improved else 'WORSE'}")
1064
+
1065
+ # Test unbatched interface
1066
+ source_ub = torch.randn(1000, 48, device='cuda')
1067
+ target_ub = torch.randn(1000, 48, device='cuda') * 0.5 + source_ub * 0.5
1068
+ aligned_ub, info_ub = batched_procrustes(source_ub, target_ub, rank=24)
1069
+ assert aligned_ub.shape == source_ub.shape, f"Shape mismatch: {aligned_ub.shape} vs {source_ub.shape}"
1070
+ print(f" Unbatched API: shape {aligned_ub.shape} βœ“ method={info_ub['method']}")
1071
+
1072
+ # Test batched_procrustes_align_pair
1073
+ aligned_pair, info_pair = batched_procrustes_align_pair(
1074
+ source_ub, target_ub, rank=24, n_align=500)
1075
+ assert aligned_pair.shape == source_ub.shape
1076
+ cos_pair = F.cosine_similarity(aligned_pair, target_ub, dim=-1).mean().item()
1077
+ print(f" Align-pair API: cos={cos_pair:.4f} method={info_pair['method']}")
1078
+
1079
+ print(f" PROCRUSTES VALIDATION COMPLETE")
1080
+
1081
+ return all_pass
1082
+
1083
+
1084
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
1085
+ # β•‘ BENCHMARKING β•‘
1086
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
1087
+
1088
+ def _cuda_timer(fn, warmup=20, iters=80):
1089
+ """CUDA-event-timed benchmark. Returns (mean_ms, std_ms, median_ms)."""
1090
+ for _ in range(warmup):
1091
+ fn()
1092
+ torch.cuda.synchronize()
1093
+
1094
+ starts = [torch.cuda.Event(enable_timing=True) for _ in range(iters)]
1095
+ ends = [torch.cuda.Event(enable_timing=True) for _ in range(iters)]
1096
+ for i in range(iters):
1097
+ starts[i].record(); fn(); ends[i].record()
1098
+ torch.cuda.synchronize()
1099
+
1100
+ times = torch.tensor([starts[i].elapsed_time(ends[i]) for i in range(iters)])
1101
+ return times.mean().item(), times.std().item(), times.median().item()
1102
+
1103
+
1104
+ def profile_n_sweep(B=512, M=1024):
1105
+ """Sweep N from 2 to 128. Compare all methods including projected SVD."""
1106
+ device_name = torch.cuda.get_device_name(0)
1107
+ print(f"\n{'='*110}")
1108
+ print(f" N-DIMENSION SWEEP β€” {device_name}")
1109
+ print(f" B={B}, M={M}")
1110
+ print(f"{'='*110}")
1111
+ print(f" {'N':>4} {'Triton':>10} {'Gram':>10} {'Newton':>10}"
1112
+ f" {'Proj→24':>10} {'Proj→16':>10} {'Torch':>10} {'Best':>8} {'Speedup':>8}")
1113
+ print(f" {'─'*106}")
1114
+
1115
+ results = []
1116
+ n_values = [2, 3, 4, 5, 6, 7, 8, 10, 12, 16, 20, 24, 32, 48, 64, 96, 128]
1117
+
1118
+ def _fmt(ms):
1119
+ if ms != ms: # nan
1120
+ return f"{'β€”':>10}"
1121
+ return f"{ms:>8.3f}ms"
1122
+
1123
+ for N in n_values:
1124
+ if N > M:
1125
+ continue
1126
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1127
+
1128
+ triton_ms = float('nan')
1129
+ if N <= 3:
1130
+ triton_ms, _, _ = _cuda_timer(lambda: batched_svd(A, method='triton'))
1131
+
1132
+ torch_ms, _, _ = _cuda_timer(lambda: torch.linalg.svd(A, full_matrices=False))
1133
+ gram_ms, _, _ = _cuda_timer(lambda: gram_eigh_svd(A))
1134
+
1135
+ newton_ms = float('nan')
1136
+ if N >= 8:
1137
+ newton_ms, _, _ = _cuda_timer(lambda: newton_svd(A))
1138
+
1139
+ proj24_ms = float('nan')
1140
+ if N >= 32:
1141
+ proj24_ms, _, _ = _cuda_timer(lambda: projected_svd(A, target_rank=min(24, N-1)))
1142
+
1143
+ proj16_ms = float('nan')
1144
+ if N >= 24:
1145
+ proj16_ms, _, _ = _cuda_timer(lambda: projected_svd(A, target_rank=min(16, N-1)))
1146
+
1147
+ # Determine best
1148
+ times = {'torch': torch_ms, 'gram': gram_ms}
1149
+ if N <= 3: times['triton'] = triton_ms
1150
+ if N >= 8: times['newton'] = newton_ms
1151
+ if N >= 32: times['proj24'] = proj24_ms
1152
+ if N >= 24: times['proj16'] = proj16_ms
1153
+ best = min(times, key=times.get)
1154
+ speedup = torch_ms / (times[best] + 1e-9)
1155
+
1156
+ print(f" {N:>4} {_fmt(triton_ms)} {_fmt(gram_ms)} {_fmt(newton_ms)}"
1157
+ f" {_fmt(proj24_ms)} {_fmt(proj16_ms)} {_fmt(torch_ms)}"
1158
+ f" {best:>8} {speedup:>7.1f}x")
1159
+
1160
+ row = {'N': N, 'B': B, 'M': M, 'torch_ms': round(torch_ms, 4),
1161
+ 'gram_ms': round(gram_ms, 4), 'best': best,
1162
+ 'speedup_vs_torch': round(speedup, 3)}
1163
+ for k, v in [('triton_ms', triton_ms), ('newton_ms', newton_ms),
1164
+ ('proj24_ms', proj24_ms), ('proj16_ms', proj16_ms)]:
1165
+ if v == v: row[k] = round(v, 4)
1166
+ results.append(row)
1167
+
1168
+ del A; torch.cuda.empty_cache()
1169
+
1170
+ return results
1171
+
1172
+
1173
+ def profile_projection_quality(B=256, M=1024):
1174
+ """Measure projection quality: how much information does rank-k SVD preserve?
1175
+
1176
+ For each N, tests multiple target_rank values. Reports:
1177
+ - Energy ratio: fraction of total singular value energy in top-k
1178
+ - Reconstruction error: projected vs full SVD
1179
+ - Subspace agreement: cosine of principal angles between subspaces
1180
+ - Timing: projected vs full SVD
1181
+ """
1182
+ print(f"\n{'='*100}")
1183
+ print(f" PROJECTION QUALITY ANALYSIS β€” B={B}, M={M}")
1184
+ print(f" Question: can rank-k SVD approximate rank-N SVD?")
1185
+ print(f"{'='*100}")
1186
+
1187
+ configs = [
1188
+ # (N, [target_ranks to test])
1189
+ (32, [8, 12, 16, 24]),
1190
+ (48, [8, 12, 16, 24, 32]),
1191
+ (64, [8, 12, 16, 24, 32, 48]),
1192
+ (96, [8, 16, 24, 32, 48, 64]),
1193
+ (128, [8, 16, 24, 32, 48, 64, 96]),
1194
+ ]
1195
+
1196
+ all_results = []
1197
+
1198
+ for N, ranks in configs:
1199
+ if N > M:
1200
+ continue
1201
+
1202
+ print(f"\n N={N}:")
1203
+ print(f" {'k':>5} {'Energy%':>8} {'Recon_proj':>11} {'Recon_trunc':>12}"
1204
+ f" {'S_rel_err':>10} {'Subspace':>9} {'Proj ms':>10} {'Full ms':>10} {'Speedup':>8}")
1205
+ print(f" {'─'*96}")
1206
+
1207
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1208
+
1209
+ # Time full SVD once
1210
+ full_ms, _, _ = _cuda_timer(lambda: gram_eigh_svd(A), warmup=10, iters=40)
1211
+
1212
+ for k in ranks:
1213
+ if k >= N:
1214
+ continue
1215
+
1216
+ q = projected_svd_quality(A, target_rank=k)
1217
+ proj_ms, _, _ = _cuda_timer(
1218
+ lambda: projected_svd(A, target_rank=k), warmup=10, iters=40)
1219
+
1220
+ speedup = full_ms / (proj_ms + 1e-9)
1221
+
1222
+ print(f" {k:>5} {q['energy_ratio']*100:>7.2f}% {q['recon_proj']:>11.2e}"
1223
+ f" {q['recon_trunc']:>12.2e} {q['s_rel_err']:>10.4f}"
1224
+ f" {q['subspace_cos']:>9.4f} {proj_ms:>8.3f}ms {full_ms:>8.3f}ms"
1225
+ f" {speedup:>7.1f}x")
1226
+
1227
+ all_results.append({
1228
+ 'N': N, 'k': k, 'B': B, 'M': M,
1229
+ 'energy_ratio': round(q['energy_ratio'], 6),
1230
+ 'recon_proj': round(q['recon_proj'], 8),
1231
+ 'recon_trunc': round(q['recon_trunc'], 8),
1232
+ 's_rel_err': round(q['s_rel_err'], 6),
1233
+ 'subspace_cos': round(q['subspace_cos'], 6),
1234
+ 'proj_ms': round(proj_ms, 4),
1235
+ 'full_ms': round(full_ms, 4),
1236
+ })
1237
+
1238
+ del A; torch.cuda.empty_cache()
1239
+
1240
+ # Summary table
1241
+ print(f"\n {'─'*70}")
1242
+ print(f" SUMMARY: Recommended target_rank per N")
1243
+ print(f" (β‰₯99% energy, β‰₯0.99 subspace cos, best speedup)")
1244
+ print(f" {'─'*70}")
1245
+ for N, ranks in configs:
1246
+ good = [r for r in all_results if r['N'] == N
1247
+ and r['energy_ratio'] >= 0.99 and r['subspace_cos'] >= 0.99]
1248
+ if good:
1249
+ best = min(good, key=lambda r: r['k'])
1250
+ print(f" N={N:>3}: k={best['k']:>3} β†’ {best['energy_ratio']*100:.1f}% energy,"
1251
+ f" subspace={best['subspace_cos']:.4f},"
1252
+ f" {best['full_ms']/best['proj_ms']:.1f}x speedup")
1253
+ else:
1254
+ # Find best available
1255
+ available = [r for r in all_results if r['N'] == N]
1256
+ if available:
1257
+ best = max(available, key=lambda r: r['energy_ratio'])
1258
+ print(f" N={N:>3}: best k={best['k']:>3} β†’ {best['energy_ratio']*100:.1f}% energy,"
1259
+ f" subspace={best['subspace_cos']:.4f} (below 99% threshold)")
1260
+
1261
+ return all_results
1262
+
1263
+
1264
+ def profile_batch_sweep(N=3, M=1024):
1265
+ """Sweep batch size for a fixed N. Shows scaling behavior."""
1266
+ print(f"\n{'='*70}")
1267
+ print(f" BATCH SWEEP β€” N={N}, M={M}")
1268
+ print(f"{'='*70}")
1269
+ print(f" {'B':>6} {'Auto ms':>10} {'Torch ms':>10} {'Speedup':>8} {'img/s':>12}")
1270
+ print(f" {'─'*52}")
1271
+
1272
+ batch_sizes = [32, 64, 128, 256, 512, 1024, 2048, 4096, 8192]
1273
+ results = []
1274
+
1275
+ for B in batch_sizes:
1276
+ try:
1277
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1278
+ except RuntimeError:
1279
+ print(f" {B:>6} OOM")
1280
+ break
1281
+
1282
+ auto_mean, _, _ = _cuda_timer(lambda: batched_svd(A, method='auto'))
1283
+ torch_mean, _, _ = _cuda_timer(
1284
+ lambda: torch.linalg.svd(A, full_matrices=False))
1285
+
1286
+ speedup = torch_mean / (auto_mean + 1e-9)
1287
+ ips = B / (auto_mean / 1000)
1288
+
1289
+ print(f" {B:>6} {auto_mean:>8.3f}ms {torch_mean:>8.3f}ms {speedup:>7.2f}x {ips:>11,.0f}")
1290
+ results.append({'B': B, 'N': N, 'M': M,
1291
+ 'auto_ms': round(auto_mean, 4), 'torch_ms': round(torch_mean, 4),
1292
+ 'speedup': round(speedup, 3)})
1293
+ del A; torch.cuda.empty_cache()
1294
+
1295
+ return results
1296
+
1297
+
1298
+ def profile_spatial_sweep(N=3, B=512):
1299
+ """Sweep spatial dimension M for a fixed N. Shows tiling efficiency."""
1300
+ print(f"\n{'='*70}")
1301
+ print(f" SPATIAL SWEEP β€” N={N}, B={B}")
1302
+ print(f"{'='*70}")
1303
+ print(f" {'M':>6} {'~HxW':>8} {'Auto ms':>10} {'Torch ms':>10} {'Speedup':>8}")
1304
+ print(f" {'─'*48}")
1305
+
1306
+ m_values = [16, 64, 256, 512, 1024, 2048, 4096, 8192, 16384]
1307
+ results = []
1308
+
1309
+ for M in m_values:
1310
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1311
+ hw = int(M**0.5)
1312
+ tag = f"{hw}Γ—{hw}" if hw * hw == M else f"{M}"
1313
+
1314
+ auto_mean, _, _ = _cuda_timer(lambda: batched_svd(A, method='auto'))
1315
+ torch_mean, _, _ = _cuda_timer(
1316
+ lambda: torch.linalg.svd(A, full_matrices=False))
1317
+
1318
+ speedup = torch_mean / (auto_mean + 1e-9)
1319
+ print(f" {M:>6} {tag:>8} {auto_mean:>8.3f}ms {torch_mean:>8.3f}ms {speedup:>7.2f}x")
1320
+ results.append({'M': M, 'N': N, 'B': B,
1321
+ 'auto_ms': round(auto_mean, 4), 'torch_ms': round(torch_mean, 4),
1322
+ 'speedup': round(speedup, 3)})
1323
+ del A; torch.cuda.empty_cache()
1324
+
1325
+ return results
1326
+
1327
+
1328
+ def profile_crossover_detail(M=1024, B=512):
1329
+ """Fine-grained N sweep around expected crossover points."""
1330
+ print(f"\n{'='*70}")
1331
+ print(f" CROSSOVER DETAIL β€” B={B}, M={M}")
1332
+ print(f"{'='*70}")
1333
+ print(f" {'N':>4} {'Gram ms':>10} {'Torch ms':>10} {'Winner':>8} {'Margin':>8}")
1334
+ print(f" {'─'*46}")
1335
+
1336
+ for N in range(2, 65):
1337
+ if N > M:
1338
+ break
1339
+ A = torch.randn(B, M, N, device="cuda", dtype=torch.float32)
1340
+ gram_mean, _, _ = _cuda_timer(lambda: gram_eigh_svd(A), warmup=10, iters=40)
1341
+ torch_mean, _, _ = _cuda_timer(
1342
+ lambda: torch.linalg.svd(A, full_matrices=False), warmup=10, iters=40)
1343
+
1344
+ winner = "gram" if gram_mean < torch_mean else "torch"
1345
+ margin = abs(gram_mean - torch_mean) / min(gram_mean, torch_mean) * 100
1346
+
1347
+ print(f" {N:>4} {gram_mean:>8.3f}ms {torch_mean:>8.3f}ms {winner:>8} {margin:>6.1f}%")
1348
+ del A; torch.cuda.empty_cache()
1349
+
1350
+
1351
+ # ╔═══════════════════════════════════════════════════════════════════════════╗
1352
+ # β•‘ MAIN β•‘
1353
+ # β•šβ•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•β•
1354
+
1355
+ def main():
1356
+ """Full profiling suite."""
1357
+ assert torch.cuda.is_available(), "CUDA required"
1358
+ device_name = torch.cuda.get_device_name(0)
1359
+ print(f"{'='*80}")
1360
+ print(f" Generalized Batched Thin SVD β€” Profiling Suite")
1361
+ print(f" Device: {device_name}")
1362
+ print(f"{'='*80}")
1363
+
1364
+ # Correctness first
1365
+ run_validation(B=64, M=1024)
1366
+
1367
+ # Procrustes alignment quality β€” THE REAL QUESTION
1368
+ # Does rank-k Procrustes produce the same rotation as rank-N?
1369
+ procrustes_results = profile_procrustes_quality()
1370
+
1371
+ # Projection quality analysis β€” energy/reconstruction perspective
1372
+ proj_results = profile_projection_quality(B=256, M=1024)
1373
+
1374
+ # N dimension sweep β€” timing comparison
1375
+ n_results = profile_n_sweep(B=512, M=1024)
1376
+
1377
+ # Skip batch/spatial/crossover sweeps by default β€” uncomment if needed
1378
+ batch_results = {}
1379
+ spatial_results = {}
1380
+ # for N in [3, 8, 32, 64]:
1381
+ # batch_results[N] = profile_batch_sweep(N=N, M=1024)
1382
+ # for N in [3, 16, 48]:
1383
+ # spatial_results[N] = profile_spatial_sweep(N=N, B=512)
1384
+ # profile_crossover_detail(M=1024, B=512)
1385
+
1386
+ # Summary
1387
+ print(f"\n{'='*80}")
1388
+ print(f" SUMMARY")
1389
+ print(f"{'='*80}")
1390
+ print(f"\n Strategy by N:")
1391
+ print(f" N=2: Fused Triton (closed-form Jacobi rotation)")
1392
+ print(f" N=3: Fused Triton (cyclic Jacobi in registers)")
1393
+ print(f" N=4-32: Gram + eigh (bmm + cuSOLVER eigh) β€” sub-ms")
1394
+ print(f" N=48+: Projected SVD (N→k, cheap SVD, lift back) — check quality table")
1395
+ print(f"")
1396
+ print(f" Standalone utilities:")
1397
+ print(f" newton_schulz_invsqrt(G) β€” batched G^{{-1/2}} via pure bmm")
1398
+ print(f" projected_svd(A, target_rank=k) β€” rank-k approximate SVD")
1399
+ print(f" projected_svd_quality(A, target_rank) β€” measure approximation quality")
1400
+ print(f"")
1401
+ print(f" Key question answered: energy_ratio and subspace_cos in quality table")
1402
+
1403
+ # Save results
1404
+ report = {
1405
+ 'device': device_name,
1406
+ 'procrustes_quality': procrustes_results,
1407
+ 'projection_quality': proj_results,
1408
+ 'n_sweep': n_results,
1409
+ 'batch_sweeps': {str(k): v for k, v in batch_results.items()},
1410
+ 'spatial_sweeps': {str(k): v for k, v in spatial_results.items()},
1411
+ }
1412
+ with open('svd_general_profile.json', 'w') as f:
1413
+ json.dump(report, f, indent=2)
1414
+ print(f"\n Results saved to svd_general_profile.json")
1415
+ print(f"{'='*80}")
1416
+
1417
+
1418
+ if __name__ == "__main__":
1419
+ main()