Lamb Shift

Lamb Shift

In quantum electrodynamics, the Lamb shift refers to a small difference in energy between the 2S1/2 and 2P1/2 states of hydrogen—levels that are degenerate in the Dirac equation.

The standard explanation invokes virtual photon exchange, vacuum polarisation, and loop corrections.

In modal dynamics, the Lamb shift arises from a distortion in modal anchoring structure near a dense coherence source—namely, the atomic nucleus.

No virtual particles are involved.
The effect is real, structural, and deterministic.


Anchored Electrons in a Coherence Field

In the modal picture:

Different electronic modes (e.g. s vs. p orbitals) experience different anchoring geometries:

This leads to non-identical anchoring cost landscapes even if the quantum numbers would suggest degeneracy.


The key insight is that the anchoring cost is not symmetric for all coherent configurations:

This small difference in anchoring cost creates a measurable energy shift:

ΔE=δCanchor

This is the Lamb shift—not a radiative correction, but a structural asymmetry in phase accommodation within a gradient field.


No Loops, No Renormalisation

In modal dynamics:

Every mode obeys the same cost functional. The differences arise not from quantum randomness, but from coherence geometry under boundary distortion.


Why It's a Signature

The Lamb shift confirms that:

This is a strong test of modal mechanics. The shift is small—but entirely predictable from the anchoring rules and phase profiles involved.

(See Appendices/Appendix AJ — Lamb Shift from Coherence Overlap.)


The Lamb shift is not a quantum correction.
It is a modal footprint left by anchoring near coherence saturation.