Theoretical analysis demonstrates topological derivation of antimatter conjugation via an orientation parameter, indicating identical gravitational attraction and exact charge inversion.
In this work, the topological foundations of CPT antimatter conjugation and baryon number conservation are formally derived through the Global Orientation Parameter Ω ∈ {+1, -1}, anchored to the tri-coordinated Y-gate in the bilateral braneworld (FCD-RBv6). Naive models of antimatter—based on continuous mass swaps across the 5D inter-brane substrate—suffer from three catastrophic failures: (1) charge degeneracy that conflates weak flavor changes with antiparticles; (2) unconstrained baryon number, permitting unphysical states (e.g., Q = -1e with B = +1); and (3) confusion between the non-collisional mirror dark sector and local, annihilating CPT antimatter. We uncouple antimatter conjugation from inter-brane mass transport by proving that Ω operates as a discrete global sign parity across the three Einstein-Rosen (ER) dipoles of the nucleon: Q_visible = Ω · Q_TBMAR = -Ω [(m_mirror - m_visible)/M] e, and B = Ω · |B_0| = Ω · (+1). Under Ω = +1, standard matter is recovered: Proton (Q = +1e, B = +1) and Neutron (Q = 0, B = +1). Under Ω = -1, exact CPT antimatter emerges without transferring mass: Antiproton (Q = -1e, B = -1) and Antineutron (Q = 0, B = -1, with magnetic moment μ_n̄ = +1.913 μ_N). We establish that the electronic Rayleigh surface mode (-0.511 MeV) at the minority-mass endpoint responds with charge q_lepton = -Ω · e, projecting two orbital positrons at the boundary of the antiproton and directly deriving the 1.022 MeV pair annihilation threshold. Topological discreteness is strictly enforced by the tri-coordinated closure singularity of the Y-gate (Φ_A = Φ_B = Φ_C = 0), dynamically triggered by the sign of the pressure gradient ∇P_bulk in the 5D matrix. Finally, because the rest masses anchored at the Compton centrifugal floor (R_0 ≈ 0.6308 fm) remain unaltered, antimatter gravitates with identical positive attraction (g_antimatter = g_matter) via phase-space mode depletion (S = 0, dS = 0).
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Ricardo J Miralles (2026) studied this question.
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