feat(geometry): State space embedding — where the program lives

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)
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# 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) × (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
= 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) ∈ × × × [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) ×
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:
```python
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) ∈ × 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:
```json
{
"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.