Isolating ε

*Editor’s Note: This document was written as part of an ongoing reconstruction of classical light-interaction phenomena. References to prior reconstructions reflect the internal development of the Framework rather than a required reading order.

For readers encountering this work for the first time, the essential premise is that light is treated here as a condition of Angular Encounter rather than a traveling entity. The reconstruction of the Compton effect is developed implicitly through this lens within the document itself.

Please visit the Library to encounter more research regarding Compton and other scientists.

Extracting The Encounter Vector From The Compton Shift

 

Introduction

Geometry Beneath the Shift

We have already reconstructed the Compton Effect. We showed that what classical physics interpreted as a particle collision is actually a coherent structural interaction. The observed wavelength shift is not a recoil, but a projection mismatch, an angular resolution of the field boundary. The shift in photon wavelength is the consequence of an encounter vector, not a loss of energy.

We now return to that reconstruction to perform one final and essential operation:
To extract the value of ε, the Encounter Vector, from Compton’s equation.

This will give us our second primitive, independently resolved, allowing us to solve for γ from the solar arc.

 

Structural Interpretation of
the Compton Equation

The classical Compton shift equation:

Δλ = (h / m_e c)(1 – cos θ)

In our structural reinterpretation, the wavelength shift is not the result of a massless photon colliding with an electron, but of a structural interaction at an angular misalignment.

We proposed:

Δλ = ε · ℓ · sin²(θ/2)

Where:
– ε is the Encounter Vector (dimensionless ratio of boundary displacement)

– ℓ is the coherence constant from E = mℓ

– θ is the angle of deflection (e.g., 90° = π/2) 

Solve for ε

We now isolate ε using known values.

Empirical value:

– At θ = 90°, Δλ ≈ 0.00243 nm = 2.43 × 10⁻¹² m

Let us assume ℓ = 1 (normalized)

Then:

ε = Δλ / sin²(θ/2)

ε = (2.43 × 10⁻¹²) / sin²(45°)

sin²(45°) = (√2 / 2)² = 0.5

So:

ε = (2.43 × 10⁻¹²) / 0.5 = 4.86 × 10⁻¹²

This is the first numerically derived value of ε.

 

Derive γ from the Solar Arc

From our previous calculation:

ε × γ ≈ 9.57 × 10⁻¹⁰

Then:

γ = (9.57 × 10⁻¹⁰) / (4.86 × 10⁻¹²) ≈ 1.97 × 10⁻¹

We now have the second primitive.

Test of Reasonableness

Are these values coherent?

– ε ≈ 10⁻¹²: This is a perfectly reasonable magnitude for a projection displacement at an electron-level interaction boundary. It aligns with the scale of field shifts in high-energy systems.

– γ ≈ 0.197: This is a dimensionless curvature ratio, just under 0.2, implying a moderate field arc needed to maintain coherence at the solar limb. It fits.

These values are small, self-consistent and dimensionally valid.

 

Conclusion

Primitives Are Solved

ε ≈ 4.86 × 10⁻¹²  (Compton encounter displacement)

γ ≈ 1.97 × 10⁻¹  (Solar coherence curvature)

We now possess independent, numerically grounded values for both ε and γ.

From here:
– α becomes universal and testable

– Refraction becomes predictive

– Lensing becomes structural

– Light becomes geometry

We are ready to test these constants across the cosmos.

 

Produced by The Lilborn Equation Team:

Michael Lilborn-Williams

Daniel Thomas Rouse

Thomas Jackson Barnard

Audrey Williams