{'fraction_non_alphanumeric': 0.05345501955671447, 'fraction_numerical': 0.00651890482398957, 'mean_word_length': 4.774436090225564, 'pattern_counts': {'":': 0, '<': 0, '<?xml version=': 0, '>': 0, 'https://': 0, 'lorem ipsum': 0, 'www.': 0, 'xml': 0}, 'pii_count': 0, 'substrings_counts': 0, 'word_list_counts': {'cursed_substrings.json': 0, 'profanity_word_list.json': 0, 'sexual_word_list.json': 0, 'zh_pornsignals.json': 0}}
Bound States of (Anti-)Scalar-Quarks in SU(3) c Lattice QCD

Light scalar‐quarks φ (colored scalar particles or idealized diquarks) and their color‐singlet hadronic states are studied with quenched SU(3)c lattice QCD in terms of mass generation. We investigate “scalar‐quark mesons” φ†φ and “scalar‐quark baryons” φφφ as the bound states of scalar‐quarks φ. We also investigate the bound states of scalar‐quarks φ and quarks ψ, i.e., φ†ψ, ψψφ and φφψ, which we name “chimera hadrons”. All the new‐type hadrons including φ are found to have a large mass due to large quantum corrections by gluons, even for zero bare scalar‐quark mass mφ = 0 at a−1 ∼ 1GeV. We conjecture that all colored particles generally acquire a large effective mass due to dressed gluon effects.