Two-proton emitters with diproton-correlated initial states can deliver spin-entangled proton pairs exceeding local-hidden-variable bounds in democratic three-body emission.
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A projector overlap matrix unifies contextuality indicators and yields S2 as a state-independent witness that remains positive for KCBS contextuality even when Maassen-Uffink bounds become trivial.
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Two-proton emission as source of spin-entangled proton pairs
Two-proton emitters with diproton-correlated initial states can deliver spin-entangled proton pairs exceeding local-hidden-variable bounds in democratic three-body emission.
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Contextuality from the Projector Overlap Matrix
A projector overlap matrix unifies contextuality indicators and yields S2 as a state-independent witness that remains positive for KCBS contextuality even when Maassen-Uffink bounds become trivial.