χ_c1(3872) is treated as a bound state in adjoint-meson Born-Oppenheimer potentials within a diabatic model, with calculated spin splittings and decay widths for its multiplet and bottom analogs after tuning to threshold.
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New orthogonal constructions of charged physical states in SU(2)×U(1) lattice gauge-Higgs theory with a static fermion reveal multiple masses in the charged spectrum.
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$\boldsymbol{\chi_{c1}}(3872)$ and its Partners in the Diabatic Born-Oppenheimer Approximation for QCD
χ_c1(3872) is treated as a bound state in adjoint-meson Born-Oppenheimer potentials within a diabatic model, with calculated spin splittings and decay widths for its multiplet and bottom analogs after tuning to threshold.
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Varieties of electrically charged physical states in SU(2)$\times$U(1) lattice gauge Higgs theory
New orthogonal constructions of charged physical states in SU(2)×U(1) lattice gauge-Higgs theory with a static fermion reveal multiple masses in the charged spectrum.