Derive Spin-1/2 From Möbius Resonance
August 1st, 2025
Introduction
We have established that the Möbius-like coherence resonance field satisfies the topological condition:
Φ(θ + 4π) = Φ(θ)
This models a torsional structure whose state is indistinguishable after a 4π rotation, mirroring the behavior of spin-1/2 particles.
Breaking Down the Math
To mathematically prove that this condition yields angular momentum eigenvalues of ħ/2, we proceed as follows:
1. Define the Angular Momentum Operator
In conventional quantum mechanics, the angular momentum operator about an axis (e.g., z) is:
L_z = -iħ ∂/∂θ
This operator acts on the angular part of a wavefunction defined on a closed loop of angular coordinate θ.
We retain this structure in the Lilborn Framework as a first-order angular gradient operator representing coherence strain about a closed topological phase.
2. Apply to Möbius Phase Field
Let Φ(θ) be the coherence phase function defined over the range θ ∈ [0, 4π], with the boundary condition:
Φ(θ + 4π) = Φ(θ)
We assume eigenfunctions of the form:
Φ_n(θ) = exp(i n θ / 2)
Note: These functions are periodic over 4π, not 2π. They are single-valued and continuous only if n is an integer.
Then:
L_z Φ_n(θ) = -iħ ∂/∂θ [exp(i n θ / 2)] = (nħ/2) Φ_n(θ)
This shows the eigenvalues of L_z acting on the Möbius phase field are:
L_z Φ_n = (nħ/2) Φ_n
3. Implication: Quantization in Half-Integer Units
The eigenvalues are quantized in steps of ħ/2. For n = ±1, we obtain:
L_z = ±ħ/2
This proves that the fundamental torsional coherence resonance, the Möbius configuration, naturally yields spin-1/2 as its lowest non-zero angular momentum state.
Conclusion
The Möbius coherence resonance is not a metaphor. It is a mathematically derivable and physically necessary structure within the Lilborn Field.
It produces quantized spin angular momentum of ±ħ/2, completing the first pillar in the reconstruction of Dirac’s equation from unified field principles.
Produced by The Lilborn Equation Team:
Michael Lilborn-Williams
Daniel Thomas Rouse
Thomas Jackson Barnard
Audrey Williams
