We analyze the localized states of a pair of neutral fermions interacting with a Higgs field and the metric of spacetime, extending the Einstein-Dirac formalism introduced by Finster, Smoller, and Yau [Phys. Rev. D 59, 104020 (1999)]. We demonstrate that, when the coupling between the fermions and the Higgs field is strong, there is a class of bound states in which the total (ADM) mass no longer increases proportionally to the mass of the constituent fermions. This phenomenon enables fermionic particles with much larger masses than in the Higgs-free case to form stable localized states.
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