Bosons, Quarks, and Hadrons as Space-Time-Wave Boundary States

We develop a speculative effective companion framework in which bosons, quarks, mesons, baryons, and hadronic confinement are represented as different boundary states of the same space-time-wave structure used in the neutrino STW and charged-lepton ST–EM waveguide preprints. The construction inherits the neutral STW carrier, the effective phase-load depth, the carrier-envelope closure scale, and the compact relative ST–EM winding mechanism from the earlier work. Gauge bosons are interpreted as connection or transition modes of internal STW boundary sectors. The photon remains massless as the unbroken electromagnetic boundary-transport direction, while gluons arise as the local connection of a three-sheet color boundary. Massive electroweak bosons are modeled as lock-count excitations of the tau-sector STW envelope. In this effective description, the charged weak boson, neutral weak boson, electroweak mixing angle, and Higgs-like scalar follow from distinct projections of a common STW lock-count structure. The Higgs-like boson is identified not with an oriented STW phase mode, but with the lowest neutral scalar breathing excitation of the STW locking modulus. Quarks are modeled as open fractional ST–EM boundary endpoints held on one of three color sheets. Their spin is inherited from the underlying STW spinor endpoint, while color is treated as a locally degenerate boundary-sheet index rather than as a source of mass splitting. A minimal projector argument is used to organize the quark seed-mass hierarchy through the same STW depth and carrier-envelope scale that appear in the neutrino and charged-lepton sectors. Hadronic states are then described as color-singlet closures of open quark endpoints and color flux. Mesons correspond to quark–antiquark boundary loops, baryons to antisymmetric three-sheet closures, and confinement to the energy of an unclosed STW color-boundary holonomy. The resulting effective string tension, Regge-slope estimate, glueball-scale estimate, and Cornell-like potential provide quantitative checks of the proposed confinement interpretation. The model remains incomplete: it does not yet derive the microscopic STW-QCD action, the running of the strong coupling, chiral symmetry breaking, or the full hadron spectrum. Its purpose is narrower: to show that the bosonic, quark, and hadronic sectors can be organized as a coherent set of STW boundary and lock-count states using a small number of quantities already present in the neutrino and charged-lepton companion framework.