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Many newly discovered mesons behave like $\ccbar$ charmonium states in that they preferentially decay into final states that contain a $c$- and a $\bar{c}$-quark, but do not fit expectations for any of the unfilled levels of the…

High Energy Physics - Experiment · Physics 2010-02-25 Stephen L. Olsen

In this work, we carry out the study of hidden-charm hexaquark states with the typical configurations $qqc\bar{q}\bar{q}\bar{c}$ ($q=u, d, s$). The mass spectra of hidden-charm hexaquark states are obtained within the chromo-magnetic…

High Energy Physics - Phenomenology · Physics 2022-02-08 Zhe Liu , Hong-Tao An , Zhan-Wei Liu , Xiang Liu

We study hadronic molecular states in a coupled system of $J/\psi N - \Lambda_c\bar{D}^{(*)} - \Sigma_c^{(*)}\bar{D}^{(*)}$ in $I(J^P) = \frac{1}{2}(\frac{3}{2}^-)$ channel, using the complex scaling method combined with the Gaussian…

High Energy Physics - Phenomenology · Physics 2017-11-22 Yuki Shimizu , Masayasu Harada

After Y(4630) is discovered, theorists have given various explanations. We find that if Y(4630) is interpreted as the D-wave resonant state of $\Lambda_c \bar {\Lambda}_c$ system, the particle mass, decay width and all quantum numbers are…

High Energy Physics - Phenomenology · Physics 2023-02-22 Xiao-Hui Mei , Zhuo Yu , Mao Song , Jian-You Guo , Gang Li , Xuan Luo

In this work, we introduce an explicit P-wave to construct the diquarks $[qc]_{\widehat{V}}$, then construct the local four-quark currents to explore the hidden-charm tetraquark states with the $J^{PC}=0^{++}$, $1^{+-}$ and $2^{++}$ in the…

High Energy Physics - Phenomenology · Physics 2025-09-10 Zhi-Gang Wang

Recently the observation of a new pentaquark state, the hidden-charmed strange $P_{cs}(4459)^0$, was reported by the LHCb Collaboration. The spin-parity quantum numbers of this state were not determined as a result of insufficient…

High Energy Physics - Phenomenology · Physics 2021-06-02 K. Azizi , Y. Sarac , H. Sundu

We study the $Z^\pm(4430)$ meson within a heavy hadron molecule interpretation where the $Z$ is considered as a bound state of a vector $D^\ast(2010)$ and an axial-vector $D_1(2420)$. We give predictions for the strong hidden-charm…

High Energy Physics - Phenomenology · Physics 2010-10-20 Tanja Branz , Thomas Gutsche , Valery E. Lyubovitskij

The $D_s(2320)$ state recently observed by BaBar in the $D_s^+\pi^0$ channel may be the first of a host of $cq\bar q\bar q$ four-quark states. We give a phenomenological account of the masses and decay modes. The isosinglet $D_s(2320)$…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Wei-Shu Hou

We determine the radiative decay amplitudes for decay into $D^*$ and $\bar{D} \gamma$, or $D^*_s$ and $\bar{D}_s \gamma$ of some of the charmonium like states classified as X,Y,Z resonances, plus some other hidden charm states which are…

High Energy Physics - Phenomenology · Physics 2014-11-20 Wei Hong Liang , R. Molina , E. Oset

Inspired by the newly observed $X$(4160) and $X$(3915) states, we analyze the mass spectrum of these states in different quark models and calculate their strong decay widths by the $^3P_0$ model. According to the mass spectrum of charmonium…

High Energy Physics - Phenomenology · Physics 2010-05-25 You-chang Yang , Zurong Xia , Jialun Ping

We present evidence for the exotic charged charmonium-like state $Z_c^{\pm}(3900)$ in semi-inclusive weak decays of $b$-flavored hadrons. The signal is correlated with a $J/\psi \pi^+ \pi^-$ system in the invariant mass range 4.2$-$4.7~GeV…

High Energy Physics - Experiment · Physics 2018-10-09 D0 Collaboration

We study the three-body $\Lambda_b$ decays of $\Lambda_b\to J/\psi pM$ with $M=K^-$ and $\pi^-$. The two new states ${\cal P}_{c1}\equiv {\cal P}_c(4380)^+$ and ${\cal P}_{c2}\equiv {\cal P}_c(4450)^+$ observed recently as the resonances in…

High Energy Physics - Phenomenology · Physics 2016-08-17 Y. K. Hsiao , C. Q. Geng

In this thesis, the QCD sum rules approach has been used to study the nature of the following charmonium resonances: Y(3930), Y(4140), X(4350), Y(4260), Y(4360) and Y(4660). There is a strong evidence that these states have non-conventional…

High Energy Physics - Phenomenology · Physics 2013-06-21 Raphael M. Albuquerque

We carry out a systematic study of the $1S$-wave hidden and double charm-strange tetraquarks $cs\bar{c}\bar{s}$ and $cc\bar{s}\bar{s}$ in a nonrelativistic potential quark model framework with the explicitly correlated Gaussian method, and…

High Energy Physics - Phenomenology · Physics 2024-07-30 Feng-Xiao Liu , Ru-Hui Ni , Xian-Hui Zhong , Qiang Zhao

The LHCb has discovered two new states with preferred $J^P$ quantum numbers $3/2^-$ and $5/2^+$ from $\Lambda_b$ decays. These new states can be interpreted as hidden charm pentaquarks. It has been argued that the main features of these…

High Energy Physics - Phenomenology · Physics 2016-01-27 Guan-Nan Li , Min He , Xiao-Gang He

The masses of the ground state and excited heavy tetraquarks with hidden charm and bottom are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely…

High Energy Physics - Phenomenology · Physics 2009-11-13 D. Ebert , R. N. Faustov , V. O. Galkin

In this article, we distinguish the charge conjugations of the interpolating currents, calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the masses and pole residues of the…

High Energy Physics - Phenomenology · Physics 2014-05-13 Zhi-Gang Wang

We calculate the mass spectrum of the S-wave fully heavy tetraquark systems $ QQ\bar Q\bar Q~(Q=c,b) $ with both normal $ (J^{PC}=0^{++},1^{+-},2^{++}) $ and exotic $ (J^{PC}=0^{+-},1^{++},2^{+-}) $ C-parities using three different quark…

High Energy Physics - Phenomenology · Physics 2024-03-27 Wei-Lin Wu , Yan-Ke Chen , Lu Meng , Shi-Lin Zhu

The purpose of the present study is to explore the mass spectrum of the hidden charm tetraquark states within a diquark model. Proposing that a tetraquark state is composed of a diquark and an antidiquark, the masses of all possible…

High Energy Physics - Phenomenology · Physics 2021-05-31 Pan-Pan Shi , Fei Huang , Wen-Ling Wang

The partial decay widths and production mechanism of the three pentaquark states, $P_{\psi}^{N}(4312)$, $P_{\psi}^{N}(4440)$, and $P_{\psi}^{N}(4457)$, discovered by the LHCb Collaboration in 2019, are still under debate. In this work, we…

High Energy Physics - Phenomenology · Physics 2023-11-16 Ya-Wen Pan , Ming-Zhu Liu , Li-Sheng Geng