Cross-system propagation through SACCADE recursion


System Definition

X(t)∈MXn+1=S(Xn,E)

The system evolves as a recursive SACCADE operator acting on a constrained state manifold .


Constrained Manifold

Mc={X∈M∣C(X)=0}System evolution is restricted to admissible states defined by constraint conditions, ensuring bounded dynamics .


Recursive Operator

Xn+1=P(Xn)where P is the Poincareˊ return map

Each iteration corresponds to one complete SACCADE cycle, allowing measurement of stability, drift, and coupling behavior .


Helical Trajectory

γ(t)=(Rcos⁡θ(t),Rsin⁡θ(t),vt)Γ(t)=(x(t),y(t),vt)

The system follows a helical trajectory:

  • circular component → repeated cycles
  • vertical component → accumulated system evolution

Each cycle returns to a shifted state rather than resetting .


Overshoot Condition

θ=2π+ϵϵ>0

Cycles extend beyond closure into an overshoot sector, generating transferable residual states .


Residual Generation

drAdt=−λArA+βAW(θA)W(θ)=exp⁡(−(θ−2π)22σ2)

Residual states are generated near cycle completion and persist temporarily after closure .


Coupling Condition

GΔ(XA,XB,E)>0

Residual transfer occurs only when admissibility conditions between systems are satisfied .


Directed Transfer

CA→OA→ΔA→B→CB​dcA→Bdt=−μcA→B+κA→BGΔ(XA,XB,E)rA

Structure:

  • cycle completion (A)
  • overshoot residual
  • coupling operator
  • activation of system B

This defines directed cross-system propagation .


Constraint Behavior

  • bounded recursion on constrained manifold
  • accumulation across cycles
  • non-reset dynamics
  • phase drift and structural evolution

C(t)=f(GΔ(t))

System state evolves as a function of accumulated gradient and coupling history .

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