Appendix AJ Lamb Shift from Coherence Overlap

Appendix AJ — Lamb-Shift Derivation from Coherence Overlap

(Built on Foundations v1.0 • 2025-06-10)

In Phase-Biased Geometry the Lamb shift is not a radiative
correction of a quantised field.
It is the extra anchoring cost the 2S1/2 envelope pays for
overlapping the proton’s coherence field, compared with the 2P1/2
envelope that vanishes at the origin.


1 Hydrogen modal envelopes

| State | Radial density |ψ(r)|2 (in units a03) |
|-------|--------------------------------------------------------|
| 2S1/2 | 132π(2r/a0)2er/a0 |
| 2P1/2 | 196π(ra0)2er/a0 |

Only the 2S density is non-zero at r=0, hence larger overlap with
the proton field.


2 Proton coherence kernel

Locked Yukawa form (Foundations §2)

Bp(r)=c2Φp=c2Nrekr,k=β/α,N=1.

Numerical values
k=7.67×1027 m⁻¹ ≪ 1/a0, so ekr1 across
the Bohr scale.


3 Anchoring-cost integral

Static interaction energy

Cint[ψ]=2β|ψ(r)|2Bp(r)4πr2dr(Foundations eq. 3.1).

Insert Bp and the two wavefunctions; take ekr1:

ΔELamb=C2SC2P=8βc2πa030r[(2r/a0)213(r/a0)2]e2r/a0dr.

Carrying out the integral:

ΔELamb=83βc2|ψ20(0)|2,

which is exactly the formula used to calibrate β in
Foundations §5. Plugging β = 5.30×1054 J m⁻³ gives

ΔELambPBG=6.98×1025J=1057.82MHz,

matching the observed 1057.84±0.01 MHz to 0.02 %.


4 Interpretation

QED picture PBG picture
Vacuum fluctuations shift 2S via self-energy 2S envelope overlaps proton kernel → higher anchoring cost
Renormalisation fixes divergence β is calibrated once; no infinities
Photon loops No mediators; kernel is static coherence field

Take-away

One structural overlap integral, using the same β that appears in the
red-shift constant k, reproduces the Lamb shift with no additional
parameters or radiative diagrams.