Chapter 03
The whole family.
Once you see the pattern, you see it everywhere. A "loop" in OPH is any cycle in a graph of overlapping descriptions. When the cycle fails to close, the residue is physical.
Aharonov–Bohm effect
- Local
- B = 0 along both electron paths.
- Loop
- Enclosed flux Φ_B shifts the interference.
- Holon
- exp(i q ∮A·dx / ℏ)
Berry / geometric phase
- Local
- Quantum state evolves adiabatically.
- Loop
- Slow loop in parameter space leaves a residual phase.
- Holon
- exp(i ∮ ⟨ψ|i∇|ψ⟩ · dR)
Foucault pendulum
- Local
- Plumb line obeys local gravity at every point.
- Loop
- Day-long latitude loop rotates the plane of swing.
- Holon
- Δθ = 2π (1 − sin λ)
Three-body problem
- Local
- Pairwise Newtonian forces are simple.
- Loop
- Triangle of pair-relations carries action holonomy.
- Holon
- exp(i ∮γ (p dq − H dt) / ℏ)
Yang–Mills / Wilson loops
- Local
- Field strength F_μν vanishes in vacuum patches.
- Loop
- Closed Wilson loop tr P exp(i ∮A) is observable.
- Holon
- tr P exp(i ∮γ A)
Parallel transport on a sphere
- Local
- Each step preserves the vector locally.
- Loop
- Trip around a triangle rotates the vector.
- Holon
- Δθ = (solid angle enclosed)
Consensus on graphs
- Local
- Each edge agrees on a shared variable.
- Loop
- Cycles can carry a constraint that no assignment satisfies.
- Holon
- cocycle obstruction in H¹
Distributed systems (CRDT merge)
- Local
- Each pairwise merge is well-defined.
- Loop
- Cycles of merges may diverge from the join.
- Holon
- non-commutative residual
The unification.
OPH says: there is no "gauge" trick, no "geometric phase" trick, no "chaos" trick. There is one move — repair the patch net to its quotient-normal form. Every item above is a special case.
Potentials, gauge phases, multi-body dynamics, distributed consensus — the same lesson told four ways.