世界迁移方程 dp/dt 的严格推导(英文版)
From previous appendices, we already have:
Φ = Σ_i A_i e^{iθ_i} Ω_i
World(t) = O(t) ∘ T(Φ)
But a crucial question remains: How does the experienced world shift over time among different possible worlds? This requires a dynamical equation for the probability distribution over worlds:
dp/dt
p_i(t) = Pr( experience lies in world Ω_i )
| Symbol | Meaning |
| p_i(t) | Probability weight of world Ω_i at time t |
| Ω_i | Structural core of world i |
Normalization:
p_i(t) ≥ 0, Σ_i p_i(t) = 1
World‑migration = the evolution of p_i(t) in “world‑space.”
dp_i/dt = Σ_j K_ij p_j(t)
| Symbol | Meaning |
| dp_i/dt | Rate of change of probability for world Ω_i |
| K_ij | Transition rate from world Ω_j to Ω_i |
Probability conservation requires:
Σ_i dp_i/dt = 0 ⇒ Σ_i K_ij = 0 (for all j)
K_ij = Γ · C_ij · D_ij
| Symbol | Meaning |
| Γ | Global migration scale (variability strength) |
| C_ij | Compatibility factor compatibility(O, Ω_i, Ω_j) |
| D_ij | Distance factor f(d(Ω_i, Ω_j)) |
Example distance factor:
D_ij = exp( -α · d(Ω_i, Ω_j) )
| Symbol | Meaning |
| d(Ω_i, Ω_j) | Structural distance between worlds |
| α | Sensitivity to distance |
If worlds are labeled by a continuous parameter λ:
∫ p(λ, t) dμ(λ) = 1
The migration equation becomes:
∂p(λ, t)/∂t
= -∇_λ · ( v(λ) p(λ, t) )
+ ∇_λ² ( D(λ) p(λ, t) )
| Symbol | Meaning |
| p(λ, t) | Probability density at world‑parameter λ |
| v(λ) | Drift field (world‑attractor direction) |
| D(λ) | Diffusion coefficient (random wandering strength) |
| ∇_λ, ∇_λ² | Gradient and Laplacian in world‑parameter space |
Discrete form = jumps; continuous form = flow.
O(t) = O(ν_O(t), θ_O(t), A_O(t), 𝕀(t))
The transition kernel depends on O(t):
K_ij(t) = K_ij( O(t), Ω_i, Ω_j )
The master equation becomes:
dp_i/dt = Σ_j K_ij( O(t), Ω_i, Ω_j ) p_j(t)
| Symbol | Meaning |
| ν_O(t) | Observer frequency |
| θ_O(t) | Observer phase |
| A_O(t) | Awareness amplitude |
| 𝕀(t) | Interpenetration tensor (collective structure) |
As O evolves, the set of “resonant worlds” and “reachable paths” changes.
If O is approximately stable over some time scale:
dp_i/dt = 0 ⇒ Σ_j K_ij p_j* = 0
| Symbol | Meaning |
| p_i* | Steady‑state world distribution under fixed O |
This means: For a relatively stable observer structure, there exists a “world‑attractor distribution” around which the experienced world tends to hover.
0 = 1 + T(Φ)
Φ = Σ_i A_i e^{iθ_i} Ω_i
W = T(Φ)
World(t) = O(t) ∘ T(Φ)
p_i(t) = Pr( experience in world Ω_i )
dp_i/dt = Σ_j K_ij( O(t), Ω_i, Ω_j ) p_j(t)
The Universe Equation provides Φ and T; the observer operator O provides appearance; the world‑migration equation provides the temporal dynamics of appearance.
The world‑migration equation dp/dt does not describe “the universe changing.” It describes how, given Φ and T, the evolving observer operator O(t) causes the probability distribution p_i(t) to flow, drift, and migrate through world‑space, eventually forming steady or quasi‑steady attractor distributions.