Chapter 2: Formal Derivation
Mathematical Formalization of Sθ, σθ, and Time
2.1 The Recursive Entropy Functional
We define Recursive Entropy (Sθ) as the integral of the unbinding scalar over all space and recursion depth:
Sθ = ∫Ω Σn=0nmax σθ(x,n) d³x
Components:
- Ω: Spatial domain (the region of interest)
- n: Discrete recursion depth
- nmax: Maximum recursion depth (Planck ceiling)
- σθ(x,n): Local unbinding scalar at position x, depth n
Continuous form (using recursive time τ):
Sθ = ∫Ω ∫0τmax σθ(x,τ) dτ d³x
2.2 Derivation of σθ from Drift Divergence
The unbinding scalar emerges from the failure of recursive closure:
Step 1: Define the Ideal State
A perfect recursive step satisfies:
R̂(Ψn) = Ψn+1ideal
Step 2: Define the Actual State
In reality, recursive operations produce:
Ψn+1actual = Ψn+1ideal + δΨn+1
Where δΨ represents the deviation from ideal recursion.
Step 3: Drift as Deviation Rate
𝒟(x,n) = αM ‖∂n ℳij‖F + αΦ ‖∂n ∇Φ‖2
Step 4: Lock as Alignment Quality
ℒ(x,n) = ⟨Ψn+1actual | Ψn+1ideal⟩ / ‖Ψn+1ideal‖²
Step 5: Entropy as Residue
σθ(x,n) = 𝒟(x,n) · (1 − ℒ(x,n))
2.3 Time-Linked Interpretation
Entropy Produces Time
The temporal functional from the Time Scroll:
T[Ψ] = ∫Ω σθ d³x · tP
Time Measures Entropy
Inverting the relationship:
T = ∫ dSθ / σθ
Interpretation:
- Time is the “bookkeeping” of entropy production
- Where σθ → 0, time halts
- Where σθ is large, time flows quickly
2.4 The Second Law (ITT Form)
From the definition of σθ and the properties of ℒ:
Claim: dℒ/dn ≤ 0 (lock degrades over recursion)
Consequence:
dℒ/dn ≤ 0 ⟹ d(1−ℒ)/dn ≥ 0 ⟹ dσθ/dn ≥ 0 ⟹ dSθ/dn ≥ 0
This is the ITT Second Law: Entropy tends to increase through recursion, not as a statistical tendency, but as a structural necessity.
2.5 Summary of Key Equations
| Equation | Name | Form |
|---|---|---|
| Unbinding scalar | σθ | 𝒟(1 − ℒ) |
| Drift magnitude | 𝒟 | αM ‖∂n ℳij‖F + αΦ ‖∂n ∇Φ‖2 |
| Recursive entropy | Sθ | ∫Ω Σ σθ(x,n) d³x |
| Time functional | T | ∫ dSθ / σθ |
| Second Law | — | dℒ/dn ≤ 0 ⟹ dSθ/dn ≥ 0 |
| Information residual | I | I0 − Sθ |