Abstract:By the reaction of kaon interacting with a proton, we investigate the production of the newly observed η 1 (1855) and its C-parity partner η ′ 1 (1855) predicted in the picture of the K K1 (1400) molecular state. The total and differential cross sections of the concrete K − p → η 1 (1855)Λ and η ′ 1 (1855)Λ reactions are obtained. At the center of mass energies about 3.4∼3.6 GeV, the minimum cross-section of η 1 (1855) and and η ′ 1 (1855) production via the K − p reaction are about 0.59 nb and 19.2 nb, respec… Show more
“…However, their nature is still elusive due to our poor understanding of the gluon degree of freedom [38][39][40][41][42][43][44][45][46][47][48][49]. Besides, these states can also be interpreted as the compact tetraquarks and hadronic molecules [50][51][52][53][54][55][56][57][58].…”
We apply the QCD sum rule method to study the double-gluon hybrid states with the quarkgluon contents qqgg (q = u/d) and ssgg. We construct twenty-eight double-gluon hybrid currents, eleven of which are found to be zero due to some internal symmetries between the two gluons fields. We concentrate on the non-vanishing currents with the exotic quantum numbers J P C = 1 −+ and 3 −+ . Their masses are calculated to be M |qqgg;1 −+ = 4.35 +0.26 −0.30 GeV, M |ssgg;1 −+ = 4.49 +0.25 −0.30 GeV, M |qqgg;3 −+ = 3.02 +0.24 −0.31 GeV, and M |ssgg;3 −+ = 3.16 +0.22 −0.28 GeV. The decay behaviors of the J P C = 3 −+ states are studied, and we propose to search for them in the πa1(1260)/ρω/φφ channels in future particle experiments.
“…However, their nature is still elusive due to our poor understanding of the gluon degree of freedom [38][39][40][41][42][43][44][45][46][47][48][49]. Besides, these states can also be interpreted as the compact tetraquarks and hadronic molecules [50][51][52][53][54][55][56][57][58].…”
We apply the QCD sum rule method to study the double-gluon hybrid states with the quarkgluon contents qqgg (q = u/d) and ssgg. We construct twenty-eight double-gluon hybrid currents, eleven of which are found to be zero due to some internal symmetries between the two gluons fields. We concentrate on the non-vanishing currents with the exotic quantum numbers J P C = 1 −+ and 3 −+ . Their masses are calculated to be M |qqgg;1 −+ = 4.35 +0.26 −0.30 GeV, M |ssgg;1 −+ = 4.49 +0.25 −0.30 GeV, M |qqgg;3 −+ = 3.02 +0.24 −0.31 GeV, and M |ssgg;3 −+ = 3.16 +0.22 −0.28 GeV. The decay behaviors of the J P C = 3 −+ states are studied, and we propose to search for them in the πa1(1260)/ρω/φφ channels in future particle experiments.
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