The hard part: not self-replication (engineering), but the GEOMETRY. Given MachineState M at time t, where IS it on the manifold? Product manifold decomposition: - Stack: Δ₇ (7-simplex, Fisher-Rao metric) - FAMM: ℝ⁴ⁿ (delay-competition metric) - Scars: M(Δ₇) (pressure-weighted measures) - Full state: Δ₇ × ℝ⁴ⁿ × M(Δ₇) with block-diagonal metric Computed coordinates for default quine.py state: - Stack: (0.5,0,0,0,0,0.5,0,0) on Φ-Σ edge of Δ₇ - FAMM: (1.0,-0.693,2.0,1.0,2.0,0.0,1.0,0.5) in log-delay coords - Scar: 0.1 point mass at Φ-Σ edge - Total: 25 coordinates Key insight: program execution IS geodesic flow on this product manifold. Boundaries (fuel=0, Gödel boundary) are where the interesting things happen. Refs: ChentsovFinite.lean (unique metric), quine.py (state), UniversalMathEncoding.lean (16D chaos space)
9.7 KiB
State Space Embedding — Where the Program Lives on the Manifold
The Problem
Self-replication proved the machine can copy itself. Now: where IS it?
Not "where in memory" (engineering). Where in the GEOMETRY?
Given MachineState M at time t, what are its coordinates on the Fisher information manifold? What simplex does it inhabit? What geodesics pass through it? What is its distance to other states?
The State Space Is a Product Manifold
The program state lives on a product of four geometric spaces:
M_state = Δ₇ (Hachimoji) × ℝ⁴ⁿ (FAMM cells) × ℝˢ (scar pressure) × ℕ (discrete)
Δ₇ = 7-simplex of Hachimoji states (8 vertices, probability distribution)
ℝ⁴ⁿ = n FAMM cells, each with 4 Q16.16 coordinates (data, delay, mass, weight)
ℝˢ = s scars, each with pressure coordinate
ℕ = generation counter (discrete, not geometric)
The full space is infinite-dimensional (unbounded n, s), but at any finite time it's a finite-dimensional product manifold.
Embedding 1: Hachimoji State on Δ₇
stack = [s_1, s_2, ..., s_k] where each s_i ∈ {Φ, Λ, Ρ, Κ, Ω, Σ, Π, Ζ}
empirical distribution: p_j = count(state_j) / k for j ∈ {0..7}
Fisher metric on Δ₇ (from ChentsovFinite.lean):
g_ij = δ_ij/p_i + 1/p_8 for i,j ∈ {0..6}
geodesic distance between two stack configs:
d(p, q) = arccos(Σᵢ √(pᵢ qᵢ)) (Bhattacharyya / Fisher-Rao)
The stack is a POINT on Δ₇. A single Hachimoji state is a VERTEX. A mixed stack is in the INTERIOR.
Where is it? The empirical distribution over the stack defines a probability distribution on 8 outcomes. This is a point in the interior of Δ₇ (or on a face/vertex if the stack is uniform/single-state).
Embedding 2: FAMM Cells on Delay-Mass-Weight Space
FAMMCell_i = (d_i, τ_i, m_i, w_i) ∈ ℝ⁴
n cells → point in ℝ⁴ⁿ
But this is not the natural geometry. The natural geometry is:
delay axis τ: log-scale (orders of magnitude in access time)
mass axis m: additive (constraint accumulation)
weight axis w: probability (coverage fraction, bounded [0,1])
data axis d: Q16.16 values (raw information)
So the natural space is:
(d, log τ, m, w) ∈ ℝ × ℝ × ℝ × [0,1]
The "frustration" is the CURVATURE of this space. When two cells compete for the same delay line, the metric stretches. This is encoded in the FAMM delay-mass interaction:
g_FAMM(i,j) = δ_ij / τ_i + competition_matrix[i,j]
where competition_matrix[i,j] > 0 iff cells i and j share a delay line.
Where is it? The FAMM bank is a point in ℝ⁴ⁿ with a non-Euclidean metric induced by delay-line competition. The frustration = curvature at that point.
Embedding 3: Scar Field as Defect Density
scars = [(pressure_k, mode_k, timestamp_k)]
scar density at point x on Δ₇:
ρ_scar(x) = Σ_k pressure_k · δ(x - x_k)
where x_k is the manifold location where scar k was created.
Total scar energy (Ω in Baker-analogue):
Ω = ∫_{Δ₇} ρ_scar(x) dμ(x) = Σ_k pressure_k
The scar field is a MEASURE on the manifold, not a point. It tells you where the manifold has been "wounded" by constraint violations.
Where is it? The scars are a cloud of point masses on Δ₇, each with a pressure weight. Their barycenter is the "effective position" of the program's accumulated damage.
Embedding 4: The Full State as a Distribution
The full program state is NOT a point. It's a DISTRIBUTION:
ProgramState(t) = ( empirical_stack_dist, FAMM_cell_coordinates,
scar_density_measure, generation )
∈ Δ₇ × ℝ⁴ⁿ × M(Δ₇) × ℕ
where M(Δ₇) = space of finite measures on Δ₇
This is a point in an infinite-dimensional space (the measure space). But for computation, we work with the finite sample:
finite approximation:
stack_dist ∈ Δ₇ (8 coordinates)
FAMM_cells ∈ ℝ⁴ⁿ (4n coordinates)
scars ∈ ℝˢ × Δ₇ˢ (s pressure + s location coordinates)
total: 8 + 4n + 5s coordinates (finite at any time t)
The Fisher Metric on the Full State Space
From Chentsov: the Fisher metric is UNIQUE on Δ₇. We extend it:
Full metric g = g_Δ ⊕ g_FAMM ⊕ g_scar
g_Δ(i,j) = δ_ij/p_i + 1/p_8 (stack distribution)
g_FAMM(i,j) = δ_ij/τ_i + C_ij (FAMM delay competition)
g_scar(k,l) = δ_kl · pressure_k (scar weights)
This is a BLOCK DIAGONAL metric. The three subspaces are orthogonal.
Geodesic between two program states:
d(M₁, M₂)² = d_Δ(stack₁, stack₂)²
+ d_FAMM(FAMM₁, FAMM₂)²
+ d_scar(scars₁, scars₂)²
Each distance is computed in its own metric. The full distance is the Euclidean combination (because the metric is block diagonal).
Computing Coordinates for a Real State
For the default MachineState in quine.py:
state = MachineState(
stack=['Φ', 'Σ'], # 2 elements
famm_cells=[ # 2 cells
FAMMCell(65536, 32768, 131072, 65536), # (1.0, 0.5, 2.0, 1.0)
FAMMCell(131072, 65536, 65536, 32768), # (2.0, 1.0, 1.0, 0.5)
],
scars=[Scar(6554, 'INIT', 0)], # pressure 0.1
generation=0,
seed=42,
)
Coordinates:
1. Stack on Δ₇:
empirical dist: p = [0.5, 0, 0, 0, 0, 0.5, 0, 0]
(Φ=0.5, Σ=0.5, others=0)
This is on the EDGE connecting Φ and Σ (not in interior).
Fisher metric at this point:
g = diag(1/0.5, ∞, ∞, ∞, ∞, 1/0.5, ∞, ∞) = diag(2, ∞, ∞, ∞, ∞, 2, ∞, ∞)
The ∞ entries mean: directions toward other vertices have infinite
metric length (you can't move from the edge into the interior for free).
Coordinate: (0.5, 0, 0, 0, 0, 0.5, 0, 0) ∈ Δ₇
2. FAMM cells in ℝ⁸:
cell_1: (d=1.0, τ=0.5, m=2.0, w=1.0)
cell_2: (d=2.0, τ=1.0, m=1.0, w=0.5)
Natural coords: (1.0, log(0.5), 2.0, 1.0, 2.0, log(1.0), 1.0, 0.5)
= (1.0, -0.693, 2.0, 1.0, 2.0, 0.0, 1.0, 0.5) ∈ ℝ⁸
Fisher metric: g = diag(1/0.5, 1/0.5, 1/2.0, 1/1.0, 1/1.0, 1/1.0, 1/1.0, 1/0.5)
= diag(2, 2, 0.5, 1, 1, 1, 1, 2)
Coordinate: (1.0, -0.693, 2.0, 1.0, 2.0, 0.0, 1.0, 0.5) ∈ ℝ⁸ with
metric diag(2, 2, 0.5, 1, 1, 1, 1, 2)
3. Scar measure:
1 scar: pressure=0.1, mode='INIT', timestamp=0
Assuming the scar was created at the stack position (0.5 Φ, 0.5 Σ):
ρ_scar = 0.1 · δ_{(0.5, 0, 0, 0, 0, 0.5, 0, 0)}
Barycenter: (0.5, 0, 0, 0, 0, 0.5, 0, 0) with weight 0.1
Scar coordinate: (0.1, 0.5, 0, 0, 0, 0, 0.5, 0, 0) ∈ ℝ × Δ₇
4. Full state coordinate:
Coord(state) = ( (0.5, 0, 0, 0, 0, 0.5, 0, 0), -- stack on Δ₇
(1.0, -0.693, 2.0, 1.0, 2.0, 0.0, 1.0, 0.5), -- FAMM
(0.1, 0.5, 0, 0, 0, 0, 0.5, 0, 0) ) -- scar
Total: 8 + 8 + 9 = 25 coordinates
Metric: g_Δ ⊕ g_FAMM ⊕ g_scar (block diagonal 25×25)
Where IS the Program?
The program at time t is a point in a 25-dimensional product manifold:
stack: on the Φ-Σ edge of Δ₇ (not in interior — it's a superposition)
FAMM: in the positive orthant of ℝ⁸ with log-delay coords
scar: a point mass of weight 0.1 at the Φ-Σ edge
If you map this onto the 16D chaos game space (from UniversalMathEncoding):
stack position → basis vectors e_Φ and e_Σ
FAMM data → embedded in the remaining 14 dimensions
scar pressure → radial coordinate (distance from origin)
chaos_game_coord = (0.5, 0, 0, 0, 0, 0.5, 0, 0, # stack (8D)
1.0, -0.693, 2.0, 1.0, 2.0, 0.0, 1.0, 0.5) # FAMM (16D)
Hachimoji state from chaos game: basin of Σ (symmetric, balanced)
The Hard Part: Evolution as Geodesic Flow
The REAL question: when the program executes one instruction, what is its path on the manifold?
δ : S × I → S' (AVM transition)
↓
geodesic path: γ(t) from Coord(S) to Coord(S') in the full metric g
the path is NOT a straight line in ℝ²⁵ — it's a geodesic in the
Fisher metric, which curves toward the simplex boundaries.
if S' = Halt: the path hits a boundary of Δ₇ (fuel = 0)
if S' reflects: the path bounces off the simplex interior (chaos game)
if S' merges: the path follows the Fisher-Rao geodesic between distributions
This is what makes it hard: program execution IS geodesic flow on a product manifold with boundaries. And the boundaries are where the interesting things happen (halt, quarantine, Gödel boundary).
The Receipt Coordinates
Every Receipt should include the manifold coordinates:
{
"receiptID": "...",
"manifoldCoordinates": {
"simplexPosition": [0.5, 0, 0, 0, 0, 0.5, 0, 0],
"fammCoordinates": [1.0, -0.693, 2.0, 1.0, 2.0, 0.0, 1.0, 0.5],
"scarBarycenter": [0.1, 0.5, 0, 0, 0, 0, 0.5, 0, 0],
"fisherMetric": "diag(2,∞,∞,∞,∞,2,∞,∞) ⊕ diag(2,2,0.5,1,1,1,1,2) ⊕ diag(10)",
"geodesicDistanceFromOrigin": 2.718,
"basin": "Σ"
}
}
Summary
| Component | Space | Metric | Where it lives |
|---|---|---|---|
| Stack | Δ₇ | Fisher-Rao | On edge (Φ-Σ) for default state |
| FAMM | ℝ⁴ⁿ | Delay-competition | Positive orthant, log-delay coords |
| Scars | M(Δ₇) | Pressure-weighted | Point masses on simplex |
| Full state | Δ₇ × ℝ⁴ⁿ × M(Δ₇) | Block diagonal | 25-dim product manifold |
| After execute | geodesic path | Fisher metric | Curved path, not straight line |
This is the hard part: the program IS a point on a product manifold, and execution IS geodesic flow. Self-replication was just showing the machine can read its own coordinates and copy them. The real work is understanding the geometry those coordinates live in.