Abstract:Recently, a hadronic state, named η 1 (1855), about 1.86 GeV was observed in BESIII experiment. This finding has a peculiar interest due to its exotic quantum number J P C = 1 −+ . In this paper, we examine the tetraquark interpretation for the structure of η 1 (1855) in the configurations of [1 c ] ss ⊗[1 c ] qq and [1 c ] sq ⊗ [1 c ] sq , and perform a mass spectrum calculation in the framework of QCD sum rules. The results show that the observed η 1 (1855) could be embedded into the [1 c ] ss ⊗ [1 c ] qq co… Show more
“…See Ref. [1065] for more QCD sum rule analyses. of a C-odd three-gluon glueball [934], given that two-gluon glueballs have been studied intensively but still difficult to be identified in experiments unambiguously.…”
The past decades witnessed the golden era of hadron physics. Many excited open heavy flavor mesons and baryons have been observed since 2017. We shall provide an updated review of the recent experimental and theoretical progresses in this active field. Besides the conventional heavy hadrons, we shall also review the recently observed open heavy flavor tetraquark states X(2900) and T + cc (3875) as well as the hidden heavy flavor multiquark states X(6900), P cs (4459) 0 , Z cs (3985) − , Z cs (4000) + , and Z cs (4220) + . We will also cover the recent progresses on the glueballs and light hybrid mesons, which are the direct manifestations of the non-Abelian SU (3) gauge interaction of the Quantum Chromodynamics in the low-energy region.
“…See Ref. [1065] for more QCD sum rule analyses. of a C-odd three-gluon glueball [934], given that two-gluon glueballs have been studied intensively but still difficult to be identified in experiments unambiguously.…”
The past decades witnessed the golden era of hadron physics. Many excited open heavy flavor mesons and baryons have been observed since 2017. We shall provide an updated review of the recent experimental and theoretical progresses in this active field. Besides the conventional heavy hadrons, we shall also review the recently observed open heavy flavor tetraquark states X(2900) and T + cc (3875) as well as the hidden heavy flavor multiquark states X(6900), P cs (4459) 0 , Z cs (3985) − , Z cs (4000) + , and Z cs (4220) + . We will also cover the recent progresses on the glueballs and light hybrid mesons, which are the direct manifestations of the non-Abelian SU (3) gauge interaction of the Quantum Chromodynamics in the low-energy region.
“…In our numerical calculations, related parameters of baryon octet are shown in table 2 and other inputs are adopted as follows [4,42,[50][51][52][53][54][55][56][57][58][59][60][61]: ⟨qq⟩ = −(0.24 ± 0.01) 3 GeV 3 , ⟨ss⟩ = (0.8 ± 0.1)⟨qq⟩,…”
Section: Numerical Results and Discussionmentioning
We investigate the hyperon semileptonic decays within the framework of QCD sum rules. The flavor SU(3) symmetry breaking effects are analyzed via the relevant form factors and corresponding branching fractions. Employing the z-series parameterization to capture the q2 dependence of form factors, we calculate the hyperon semileptonic decay rates and confront them with the recent experimental measurements. Moreover, we calculate as well the non-standard tensor form factors, which involve certain new physics beyond the standard model.
“…Recently, the BESIII Collaboration observed η 1 (1855) in the J/ψ → γηη ′ decay [2]. Since the η 1 (1855) is an isoscalar resonance with exotic J PC = 1 −+ quantum numbers, different explanations of exotic states like hybrid [4][5][6], the K K1 (1400) molecular state [7,8], and tetraquark state [9] were proposed, which shows that this observation attracted theorist's attention in the past months. Besides decoding the nature of the observed η 1 (1855), establishing the η 1 (1855) in experiment is also crucial.…”
Section: Discussionmentioning
confidence: 99%
“…respectively. Obviously, the observed η 1 (1855) cannot be grouped into the conventional hadron, which is a good candidate of exotic states as indicated by some theoretical groups, where the η 1 (1855) was interpreted as a hybrid state [4][5][6], a molecular state [7,8], and a tetraquark state [9]. At present, the η 1 (1855) was only observed in the radiative decay J/ψ → γηη ′ , confirming this observation by others processes is an interesting experimental topic, which will be helpful to establish this exotic state in experiment and may provide some valuable information to reflect its inner structure.…”
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, respectively. The differential cross sections for both reactions at the different center of mass energies are also available. Furthermore, we present the Dalitz processes of 2 → 3 and 2 → 4, and initially discuss the feasibility of finding out the η 1 (1855) and η ′ 1 (1855) in experiments like J-PARC.
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