In the SQUS discussion model, one independent phase traces a circle S¹, while
two independent phases span a torus T² = S¹ × S¹. The torus is therefore a
picture of the fermion's two-phase state, not by itself a derivation of spin.
A bosonic channel keeps one phase combination φp,q = pθ₁ + qθ₂,
reducing the information to a single circle. Drag the scene or use the control
below to follow the 2:1 winding: the minor cycle closes twice while the major
cycle closes once, so the full configuration returns only after 4π.
The conceptual diagram compares a two-phase torus T² for a fermionic
spinor state with its one-phase bosonic projection S¹. The spinor changes
sign after 2π and returns after 4π; the projected channel returns after 2π.
FERMION · T²two phases · spinor orientation
BOSON · S¹ + S¹major and minor cycle projections
θ₁ · LARGE CYCLE
θ₂ · WHITE CROSS-SECTION BESIDE T² · 2:1
DRAG TO ROTATE
STATUS [A/C]
A two-component normalized spinor belongs to S³ ≃ SU(2); fixing component
amplitudes leaves a toroidal two-phase slice. Antiperiodicity
Ψ(θ + 2π) = −Ψ and Ψ(θ + 4π) = Ψ gives the fermionic 4π cycle, while a
bilinear BΓ = Ψ̄ΓΨ removes the sign and is 2π-periodic [A].
The two circles visualize separate projections of the torus's major phase θ₁
and minor cross-sectional phase θ₂, with θ₂ = 2θ₁. At Ω = 2π the small cycle
has closed but the large cycle is displaced by π; at Ω = 4π both return to
their starting configuration. A physical bosonic channel may instead retain
a combination φp,q = pθ₁ + qθ₂.
Interpreting this torus as SQUS fermion geometry and the circle as an emergent
bosonic correlation channel remains a hypothesis [C], pending a Dirac operator,
spin connection, holonomy, and gauge-field derivation.