arXiv2026
We construct an exact spin-$1$ parent Hamiltonian for constrained valence-bond loop manifolds on the checkerboard and pyrochlore lattices. The Hamiltonian is local, SU(2)- and time-reversal-invariant, and built from positive-semidefinite projectors acting on triangular faces. Each projector removes only the maximally polarized state of a triangle, so the model is frustration-free. Its zero-energy states are generated by an AKLT-like construction in which each spin-$1$ moment is resolved into two virtual spin-$\tfrac12$ degrees of freedom, singlets are formed inside every crossed plaquette or tetrahedron, and the physical spin-$1$ Hilbert space is recovered by projection. The resulting ground states are fully packed singlet-loop states on the corner-sharing lattice. Thus, a loop or dimer constraint, usually introduced as part of an effective Rokhsar--Kivelson description, appears here as the exact zero-energy manifold of a microscopic spin Hamiltonian. We analyze spin correlations within this manifold and show that, for a fixed loop covering, they are determined by loop connectivity. We also project symmetry-allowed perturbations into the ground-state manifold and derive the resulting low-energy pseudospin dynamics. The checkerboard and pyrochlore cases differ sharply. On the pyrochlore lattice, tetrahedral symmetry removes simple local bias terms, and the leading nontrivial next-nearest-neighbour Heisenberg perturbation gives an emergent spin-$\tfrac12$ XY model on the diamond lattice of tetrahedron centers. These results give an exact spin-$1$ microscopic starting point for constrained valence-bond physics in two and three dimensions, and show how loop, dimer, and gauge-theoretic descriptions can be approached from a small-spin, SU(2)-invariant frustrated magnet.