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Related papers: Towards the assignment for the $4 ^1S_0$ meson non…

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Recently, the BESIII Collaboration reported three resonances: $X(2232)$ with $M = 2232 \pm 19 \pm 27$ MeV and $\Gamma = 93 \pm 53 \pm 20$ MeV, $X(2200)$ whose mass $M = 2200 \pm 11 \pm 17$ MeV and width $\Gamma = 74 \pm 20 \pm 24$ MeV as…

High Energy Physics - Phenomenology · Physics 2022-11-17 Ya-rong Wang , Yang Ma , Cheng-qun Pang

The structure, spectroscopic parameters and width of the resonance with quantum numbers $J^{PC}=1^{++}$ discovered by the COMPASS Collaboration and classified as the $a_1(1420)$ meson are examined in the context of QCD sum rule method. In…

High Energy Physics - Phenomenology · Physics 2018-03-14 H. Sundu , S. S. Agaev , K. Azizi

We investigate the mass and strong decay properties of the $\Omega(2012)$ resonance using QCD sum rules, assuming it to be an S-wave $\Xi(1530)\bar{K}$ molecular pentaquark state with $I(J^{P})= 0(\frac{3}{2}^{-})$. A unified interpolating…

High Energy Physics - Phenomenology · Physics 2026-05-14 Xiang Yu , Jin-Peng Zhang , Xu-Liang Chen , Ding-Kun Lian , Qi-Nan Wang , Wei Chen

Non-leptonic D meson decays may provide a reliable testbed for the multiquark interpretation of light scalar mesons. In this letter we consider D_s decay and show that a 4-quark f_0(980) meson could induce a decay pattern, which is…

High Energy Physics - Phenomenology · Physics 2008-11-26 L. Maiani , A. D. Polosa , V. Riquer

The full-heavy tetraquarks $cc\bar{c}\bar{b}$ and $bb\bar{b}\bar{c}$ are systematically investigated within the chiral quark model. The meson-meson structure, diquark-antidiquark structure and K-structure are considered in this work. There…

High Energy Physics - Phenomenology · Physics 2023-07-26 Jing Hu , Bing-Ran He , Jia-Lun Ping

We report a study of the B meson decays, B+ -> J/psi phi K+, B0 -> J/psi phi K0S, B0 -> J/psi phi, B0 -> J/psi eta and B0 -> J/psi eta' using 56 million BBbar events collected at the Y(4S) resonance with the BABAR detector at the PEP-II e+…

High Energy Physics - Experiment · Physics 2012-08-03 BABAR Collaboration , B. Aubert

The assignments of the isoscalar scalar mesons f0(980), f0(1370), and f0(1500) in terms of their qqbar substructure is still a matter of heated dispute. Here we employ the weak and electromagnetic decays D(s)(+) to f0+pi(+) and f0…

High Energy Physics - Phenomenology · Physics 2008-11-26 Frieder Kleefeld , Eef van Beveren , George Rupp , Michael D. Scadron

Light mesons have always been an important part of the whole hadron family, once inspiring the SU(3) classification of hadrons as a typical example~\cite{Gell-Mann:1964ewy}. Until now, the search for light mesons has been an ongoing task in…

High Energy Physics - Phenomenology · Physics 2024-10-17 Cheng-Xi Liu , Li-Ming Wang , Ting-Yan Li , Xiang Liu

Motivated by the recently observed $D_{s0}(2590)$ state by LHCb, we investigate the mass spectrum and the strong decay properties of the charmed-strange mesons within Godfrey-Isgur model considering the coupled-channel effects. Our results…

High Energy Physics - Phenomenology · Physics 2023-12-06 Jing-Jing Yang , Wei Hao , Xiaoyu Wang , De-Min Li , Yu-Xiao Li , En Wang

The coupling constants of the order $p^2$ low-energy weak effective lagrangian can be determined from the $K\to\pi$ and $K\to 0$ weak matrix elements, choosing degenerate quark masses for the first of these. However, for typical values of…

High Energy Physics - Lattice · Physics 2009-10-31 Maarten Golterman , Elisabetta Pallante

This letter reports results from the partial wave analysis of the $\pi^{-}\pi^{-}\pi^{+}\eta$ final state in $\pi^{-}p$ collisions at 18GeV/c. Strong evidence is observed for production of two mesons with exotic quantum numbers of spin,…

High Energy Physics - Experiment · Physics 2008-11-26 J. Kuhn

In the reactions $p\bar p\to\pi^0\pi^0,\eta\eta,\eta\eta'$ there are four relatively narrow resonances $f_2(1920)$, $f_2(2020)$, $f_2(2240)$, $f_2(2300)$, and a broad one $f_2(2000)$ in the mass region 1990--2400 MeV. In the framework of…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. V. Anisovich , M. A. Matveev , J. Nyiri , A. V. Sarantsev

We calculate the masses of the resonances D_{s0}^*(2317) and D_{s1}(2460) as well as their bottom partners as bound states of a kaon and a D^*- and B^*-meson, respectively, in unitarized chiral perturbation theory at next-to-leading order.…

High Energy Physics - Phenomenology · Physics 2011-03-02 Martin Cleven , Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

Inspired by the newly observed $\Omega_c^0$ states at LHCb, we decode their properties by performing an analysis of mass spectrum and decay behavior. Our studies show that the five narrow states, i.e., $\Omega_c(3000)^0$,…

High Energy Physics - Phenomenology · Physics 2017-12-06 Bing Chen , Xiang Liu

In the standard model the rate of the $\pi^0, \eta, \eta', K_S, K_L\to \nu \overline{\nu}$ decays is predicted to be extremely small. Therefore, observation of any of these mesons ($M^0$) decaying into an invisible final state would signal…

High Energy Physics - Phenomenology · Physics 2015-01-12 S. N. Gninenko

This talk reviews the last applications of the covariant quark model for studying the properties of the multiquark states: B_s-meson (quark-antiquark state), light baryons (three-quark states) and tetraquark (four-quark state). The form…

High Energy Physics - Phenomenology · Physics 2013-01-22 Mikhail A. Ivanov

The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the first time into Lambda(1405) K, Lambda(1520) K, Sigma(1385) K, Lambda K*, and Sigma K*, are examined in a relativized quark pair creation…

Nuclear Theory · Physics 2014-11-18 Simon Capstick , W. Roberts

We describe searches for $B^0$ meson decays to the charmless final states $\pi^0 K^0_SK^0_S$, $\eta K^0_S K^0_S$, and $\eta^{\prime}K^0_SK^0_S$. The data sample corresponds to $467 \times 10^{6}$ $B\bar{B}$ pairs produced in $e^+e^-$…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

In this work we calculate the mass spectrum of strangeonium up to the $3D$ multiplet within a nonrelativistic linear potential quark model. Furthermore, using the obtained wave functions, we also evaluate the strong decays of the…

High Energy Physics - Phenomenology · Physics 2021-05-13 Qi Li , Long-Cheng Gui , Ming-Sheng Liu , Qi-Fang Lü , Xian-Hui Zhong

Using 4.7 fb^-1 of data taken at CESR at energies at and near the Upsilon(4S) we have studied the decay B- -> D{*+}pi-pi- (and its conjugate). We observe a new, broad charmed meson state, which we interpret as D_J(j=1/2), in its decay to…

High Energy Physics - Experiment · Physics 2010-04-08 S. Anderson , CLEO Collaboration