Section 8: Mapping Emergent Field Parameters to Fundamental Flow Quantities

Section 8: Mapping Emergent Field Parameters to Fundamental Flow Quantities

8.1 Overview and Motivation

This section establishes explicit functional relationships between emergent field parameters and the discrete flow dynamics of the Temporal Flow Physics (TFP) framework. These parameters are not inputs but arise as coarse-grained outputs of local flow interactions.

Fundamental Inputs:

  • Fi(n): Flow at node i at discrete time n (dimensionless)
  • α(i,j,n): Exchange strength between nodes i and j (dimensionless)
  • Ci: Processing capacity at node i (dimensionless)
  • Vinternal(F): Local internal potential function (dimensionless)

Emergent Field Parameters:

  • vcond: Vacuum expectation amplitude (dimensionless)
  • λpot: Potential curvature (dimensionless)
  • g: Coupling constant (dimensionless)

8.2 Vacuum Expectation Value: vcond from Internal Potential Structure

8.2.1 Origin from Vinternal(F)

The internal potential function has a double-well form:
Vinternal(F) = (F - F0)² × (F - F1 (dimensionless)
Here, F0 and F1 represent attractor flow values.

8.2.2 Link Amplitude from Flow Differences

The local emergent amplitude between connected nodes i and j:
Aij(n) = |Fj(n) − Fi(n)| × Cij(n) (dimensionless)
In stable regimes with node flows near attractors:
Aij(n) → |F1 − F0| × Cij(n) (dimensionless)

8.2.3 Coarse-Grained Order Parameter

Define regional order parameter Φa(n) as:
Φa(n) = Σ(i,j ∈ region a) [wij × Aij(n) × exp(i θij(n))] (complex, dimensionless)
Time-averaged amplitude magnitude approximates:
⟨|Φa(n)|⟩ ≈ ⟨wtotal⟩ × ⟨Aij(n)⟩ (dimensionless)

8.2.4 Explicit Formula for vcond

First-order relation:
vcond = ηgeom × |F1 − F0| × ⟨Cij (dimensionless)
More detailed form:
vcond = |F1 − F0| × sqrt(⟨α⟩ / αcritical) × ⟨coherence_efficiency⟩ (dimensionless)
Where:
ηgeom: geometric averaging factor (dimensionless)
αcritical: threshold for sustained coherence (dimensionless)

8.3 Potential Curvature: λpot from Network Stiffness

8.3.1 Macroscopic Potential Form

The emergent field potential takes the form:
V(Φ) = λpot × (|Φ|² − vcond²)² (dimensionless)
λpot quantifies resistance to deviation from vacuum.

8.3.2 Microscopic Curvature at Minima

Internal potential curvature at minima is:
κinternal = second derivative of Vinternal with respect to F at F = F0 or F1 = 2 × (F1 − F0 (dimensionless)

8.3.3 Amplification from Collective Stiffness

Flow resistance is scaled by condensed node density and link connectivity:
λpot = κinternal × ρeffective × connectivity_factor (dimensionless)
Where:
ρeffective = number of condensed nodes / condensed volume (dimensionless node density)
connectivity_factor = average node degree / max degree (dimensionless)

8.3.4 Explicit Formula for λpot

λpot = 2 × (F1 − F0)² × (Ncondensed / Vcondensed) × (⟨Ci⟩ / Cmax) (dimensionless)
Alternative expression:
λpot = (2 / vcond²) × (F1 − F0)⁴ × ⟨processing_density⟩ × ⟨capacity_utilization⟩ (dimensionless)

8.4 Coupling Constant: g from Exchange Dynamics

8.4.1 Misalignment Resistance

From Section 6, coupling action Scoupling depends on phase misalignment:
Scoupling = −(2 / g²) × Σneighbors ⟨a,b⟩, na(n) − Rabb(n))|² (dimensionless)
g controls resistance to phase misalignment between regions.

8.4.2 Dependence on Exchange Strength

Stronger exchange α and tighter capacity utilization Ci increase coupling rigidity.

8.4.3 Processing Load Ratio

Define processing stress as:
processing_stress = ⟨Σj α(i,j,n)⟩ / ⟨Ci (dimensionless)
Approaching 1 signals nonlinear response increase.

8.4.4 Explicit Formula for g

g² = (⟨Ci⟩ / ⟨Σj α(i,j,n)⟩) × βcoupling × topology_factor (dimensionless)
Simplified proportionality:
g² ∝ ⟨Ci⟩ / ⟨α_total(i,n)⟩ (dimensionless)
Refined formula incorporating fluctuations:
g² = (Cchar / αchar) × (1 + δ_fluctuations) (dimensionless)
Where:
δ_fluctuations = temporal variance in exchange rates (dimensionless)

8.5 Cross-Parameter Relationships

8.5.1 Internal Consistency Constraints

vcond² ∝ (⟨Ci⟩ / ⟨α_total⟩) × |F1 − F0 (dimensionless)
Product of coupling and potential curvature:
g² × λpot = 4 × (F1 − F0)² × network_efficiency (dimensionless)
Emergent mass squared:
m² = λpot × vcond² = 2 × (F1 − F0)⁴ × (ρnodes × ⟨Cij⟩²) (dimensionless)

8.5.2 Scaling Laws

vcond scales linearly: vcond ∝ |F1 − F0|
λpot scales quadratically: λpot ∝ (F1 − F0
Coupling inversely related: g⁻² ∝ ⟨Ci⟩ / ⟨α⟩

8.6 Computational Implementation

8.6.1 Extraction Procedure

Measure from simulations or data:
F0, F1 from internal potential Vinternal(F)
⟨Ci: time-averaged processing capacity
⟨α(i,j,n)⟩: network-wide exchange strengths
Compute parameters:
vcond = |F1 − F0| × sqrt(⟨α⟩ / αcritical) × coherence_factor
λpot = 2 × (F1 − F0)² × ρeffective × (⟨Ci⟩ / Cmax)
g² = (⟨Ci⟩ / ⟨α_total⟩) × βcoupling × topology_factor
Validate consistency:
Check g² × λpot ≈ 4 × (F1 − F0)² × network_efficiency
Confirm m² = λpot × vcond² scales as expected

8.6.2 Time Evolution

Parameter temporal derivatives approximate as:
∂vcond/∂t ∝ ∂(F1 − F0)/∂t + ∂⟨coherence⟩/∂t
∂λpot/∂t ∝ ∂ρnodes/∂t + ∂⟨capacity_utilization⟩/∂t
∂g/∂t ∝ ∂(C/α ratio)/∂t

8.7 Testable Predictions

8.7.1 Parameter Regimes

  • Strong coupling: small → λpot large → sharp phase transitions
  • Weak coupling: large → λpot small → smooth transitions
  • Low capacity: ⟨Ci small → small → high sensitivity to interactions

8.7.2 Network Size Scaling

  • vcond is approximately constant (intensive quantity)
  • λpot scales with node density (N / V)
  • depends on topology, largely independent of node count

8.7.3 Criticality Indicators

  • As ⟨α_total⟩ approaches ⟨Ci:
  • g → ∞ (coupling diverges)
  • λpot → 0 (potential flattens)
  • vcond → 0 (condensate dissolves)

8.8 Summary Table

Parameter Depends On Interpretation
vcond F1 − F0 Vacuum expectation amplitude
λpot (F1 − F0)² × ρ_nodes × ⟨Ci Field stiffness / potential curvature
⟨Ci⟩ / ⟨α_total⟩ × topology_factor Inter-region coupling strength

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