Editing Openai/6897769e-4ee4-800f-aba5-69cca34f701c (section)

=== 1. QAT treats atoms / light exchanges as localized spherical boundary processes (4πr² surfaces) where EM interactions happen and where the moment of now emerges. ===
# Weak decays are transition events: an initial boundary state (particle / nucleus) transitions to final states. Transition amplitudes depend on overlap integrals of the boundary wavefunctions and on the interaction Hamiltonian. Geometry therefore enters the matrix element itself.
# Parity (P) and time (T) symmetry violations — the real properties of weak interactions — can be introduced in the boundary action in two ways: - explicitly, via chiral couplings (the weak force couples to left-handed currents), and - via complex geometric phases (Wilson loops, holonomies, Berry/Bohm phases picked up by boundary modes moving in curved / charged geometries). Those complex phases can play the role of the CP-violating phase.
# So: build an explicit boundary Lagrangian on the 2-D sphere, couple chiral fermions to gauge fields (SU(2)×U(1)), allow geometric (topological) terms that generate phases — then compute decay amplitude and CP asymmetry. That gives a direct, testable map between geometry and decay/CP observables.