Three fundamental properties (a=parity, b=conservation, c=dimensionality)^[2,7] are used as independent bases for an absolute phase space {a,b,c}^[6], in which a phase operator is the basis for all sub-physical interactions. Representative number types are determined by {a,c}, after Hestenes and Clifford, and the given phase algebra leads naturally to symmetric conservation (Noether) and applications of group theory (Lie, etc). All bosons are bound pairs of continuous modal waves, and a fermion event occurs where two bosons (four wavefunctions) locally have only two waves at conserved (-b) phase; the remaining nonconserved waves describe its vacuum field. To unambiguously resolve systems having more than two members, we deduce a 'general exclusion principle' that requires out-of-phase local states, and generates the (latent) nonconserved (not -b) bosonic domain with non-local solutions that form the macroscopic physical structure. Significantly, this identifies the sub-physical (point-local) phase space, the quantum phase interactions that provide the 'nonconservation bridge' to the macroscopic, and an integral basis for the Euclidian 3D space we readily understand, in parallel with action and gauge theory. From this, we propose a useful field unification, which naturally mixes parameters like gravity, space, proper local time, and charges (strong, weak, and electric), offering many perspectives for analysis. We use the model to examine qualitative structures in QCD, QED, and nuclear forces. Finally, some interpretations are offered in terms of this representation for the fundamental or derived nature of the energy states and processes known to physics, including correlations with - and additions to - the Standard Model.