Theory

Core Ideas

• No particles: Stable interference nodes emerge from recursively superposed spherical waves.
• Residual fields: Observable structure arises from Ψ_M − α(r)·Ψ_A with radial damping α(r).
• Spin modulation on Yin: Spin(t) = A·sin(2π f t)·sin(θ) applied to harmonics j = 3, 4 controls asymmetry.
• Fibonacci sphere sampling: Sources distributed on a Fibonacci sphere; harmonics j = 1…5 with A_j = Z / 2^j, k_j = 2π·2^j·√Z.

Example (Z = 2, Helium — standard config)

• Δφ = 0.85π; r ∈ [1.10, 1.25]; threshold: 50% of max(|Ψ_res|); cluster ≥ 5 voxels.
• Result: 3 clusters detected, 2 valence-plausible.

Detection Logic (evolving)

• Outer-shell scanning with adaptive cluster thresholds; for low Z, clusters ≥ 1 voxel may be considered valence-relevant if within r-window and below field threshold.
• For higher Z, min cluster size grows with Z (empirical adaptation).

From Yin–Yang to ASFM

The Yin–Yang metaphor motivates the destructive–constructive field balance; ASFM implements it with explicit damping and spin asymmetry on neutron fields, delivering a reproducible simulation framework.

Planned Formal Write-up

• Full derivations and parameter sweeps for Z = 1–118.
• Molecular binding pilot (O–O distance/orientation → standing-wave node formation).
• Fission SC-analyses (SC‑1/SC‑2 windows by voxel radius).