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projective_asinh |
INFINITY LATTICE RECONSTRUCTION |
source: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\clean_100k_priority |
points: T=10500 weight-dim D=4096 stride=10 |
COMPACT CHART (infinity = origin pole Ω) |
r = ||y|| min=3.688 max=363.8 |
ρ = 1/(1+r) min=0.002741 (near ∞) max=0.2133 |
fraction with ρ<0.05 (near infinity pole): 0.863 |
mean cos⟨u, û_∞⟩: 0.7563 |
mean angle to û_∞: 0.4138 rad |
RECONSTRUCTED WEIGHTS (invert last compact point) |
true log-radius r: 363.468 |
float-safe r used: 40 scale=sinh(r)=1.17693e+17 |
L0 shape=(64, 32) ||W||=7.29482e+15 |
L1 shape=(32, 64) ||W||=1.17466e+17 |
HIDDEN LATTICE DIMS (PCA of relations to Ω) |
component 0: explained_frac=0.8475 |
component 1: explained_frac=0.1506 |
component 2: explained_frac=0.0010 |
component 3: explained_frac=0.0005 |
component 4: explained_frac=0.0003 |
HOW TO READ THIS |
The run-to-infinity is not discarded. Ω is that infinity as a point. |
Every other lattice vertex is a relation to Ω (ρ, angle, C). |
Weights + hidden dims are recovered from that relational geometry. |
arrays: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\clean_100k_priority\infinity_reconstruction\infinity_chart.npz |
weights: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\clean_100k_priority\infinity_reconstruction\reconstructed_weights.npz |
4096 |
projective_asinh_padded_dual |
12288 |
projective_asinh_padded_dual |
12288 |
projective_asinh |
INFINITY LATTICE RECONSTRUCTION |
source: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\fat_first_100k |
points: T=10500 weight-dim D=4096 stride=10 |
COMPACT CHART (infinity = origin pole Ω) |
r = ||y|| min=3.675 max=370.8 |
ρ = 1/(1+r) min=0.002689 (near ∞) max=0.2139 |
fraction with ρ<0.05 (near infinity pole): 0.901 |
mean cos⟨u, û_∞⟩: 0.8349 |
mean angle to û_∞: 0.2953 rad |
RECONSTRUCTED WEIGHTS (invert last compact point) |
true log-radius r: 369.404 |
float-safe r used: 40 scale=sinh(r)=1.17693e+17 |
L0 shape=(64, 32) ||W||=1.14241e+16 |
L1 shape=(32, 64) ||W||=1.17137e+17 |
HIDDEN LATTICE DIMS (PCA of relations to Ω) |
component 0: explained_frac=0.9034 |
component 1: explained_frac=0.0946 |
component 2: explained_frac=0.0007 |
component 3: explained_frac=0.0006 |
component 4: explained_frac=0.0003 |
HOW TO READ THIS |
The run-to-infinity is not discarded. Ω is that infinity as a point. |
Every other lattice vertex is a relation to Ω (ρ, angle, C). |
Weights + hidden dims are recovered from that relational geometry. |
arrays: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\fat_first_100k\infinity_reconstruction\infinity_chart.npz |
weights: C:\Users\User\forward_pc_hebbian\checkpoints\trajectories\fat_first_100k\infinity_reconstruction\reconstructed_weights.npz |
4096 |
Weight trajectory as dynamical medium |
finite_cut (meta) = 18159 |
subsample points kept finite = 1917 |
homogenization (makes explosive path comparable): |
y = asinh(||W||) * W/||W|| |
radial model: dr = a - b*r |
global fit: a=0.0023606511830280663, b=-0.00157853027808433, regime=runaway |
late fit: a=0.0926002317445096, b=-0.00030857114946446955 |
r* = inf |
stop_kind = escape_horizon |
predicted raw ||W|| scale ~ 4.61423555401344e+47 |
t_escape (steps of extra medium sim) = 161 |
last observed radius asinh = 90.42913911208213 |
last observed speed = 100.09837206488785 |
If regime=runaway: free weights do not stop; magenta path is |
continuation until an asinh horizon; red star = horizon point |
along the late direction — completion beyond NaN of the graph. |
If regime=attractor: red star is asymptotic stop in medium space. |
4096 |
projective_asinh_padded_morph |
12288 |
projective_asinh_padded_morph |
12288 |
forward_pc_hebbian lattice dump (full)
Public full dump of dual morphogenetic / free PC-Hebbian work under checkpoints/.
trajectories/morph_A|B— dual morph projective lattices (very large)trajectories/dual_*,clean_100k_priority,fat_first_100k,live_continuousdual_morphogenetic/— net checkpoints + sediment field
Uploaded from a disk-constrained machine; local copies may remain until verified.
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