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Related papers: An open charm tetraquark candidate: note on $X_{0}…

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Prompted by a recent lattice QCD calculation, we review the SU(3) light quark flavor structure of charmed tetraquarks with spin-0 diquarks. Fermi statistics forces the three light quarks to be in the representation 3*x3*= 3+6*. This agrees…

High Energy Physics - Phenomenology · Physics 2024-07-15 L. Maiani , A. D. Polosa , V. Riquer

In this article, we assume that there exists a scalar hidden charm tetraquark state in the $\pi^+ \chi_{c1}$ invariant mass distribution, and study its mass using the QCD sum rules. The numerical result $M_{Z}=(4.36\pm0.18) \rm{GeV}$ is…

High Energy Physics - Phenomenology · Physics 2009-07-07 Zhi-Gang Wang

Stimulated by the recent experimental results on the fully-charm tetraquark states, we systematically calculate the mass spectra of the fully-charm tetraquark states in $8_{[c\bar{c}]}\otimes8_{[c\bar{c}]}$ color configuration via QCD sum…

High Energy Physics - Phenomenology · Physics 2024-08-06 Chun-Meng Tang , Chun-Gui Duan , Liang Tang

In a constituent quark model, a hidden charmed tetraquark is assumed consisting of a $cq$ diquark and an $\bar c\bar q$ antidiquark or vice versa. The Semay-Silvestre-Brac potentials are employed to calculate the masses of $cq$ (q=u, d)…

High Energy Physics - Phenomenology · Physics 2025-09-05 You-You Lin , Ji-Ying Wang , Ailin Zhang

We evaluate the masses and decay constants of the $0^+$ and $1^-$ open-charm $(\bar{c}\bar{d})(us)$ tetraquarks and molecular states from QCD spectral sum rules (QSSR) by using QCD Laplace sum rule (LSR). This method takes into account the…

High Energy Physics - Phenomenology · Physics 2021-02-22 R. M. Albuquerque , S. Narison , D. Rabetiarivony , G. Randriamanatrika

Four exotic charmonium-like states, i.e. $X(4140)$, $X(4274)$, $X(4500)$, and $X(4700)$, have been observed very recently by LHCb Collaboration in the decay process $B^+\to J/\psi \phi K^+$ using the 3${\rm fb}^{-1}$ data of $p\bar p$…

High Energy Physics - Phenomenology · Physics 2016-09-21 Ruilin Zhu

We study the exotic $bc\bar{q}\bar{q}$, $bc\bar{s}\bar{s}$ and $qc\bar{q}\bar{b}$, $sc\bar{s}\bar{b}$ systems by constructing the corresponding tetraquark currents with $J^P=0^+$ and $1^+$. After investigating the two-point correlation…

High Energy Physics - Phenomenology · Physics 2014-04-10 Wei Chen , T. G. Steele , Shi-Lin Zhu

Diquarks with $J^{P}=0^{\pm}$, $1^{\pm}$ containing a heavy (charm or bottom) quark and a light quark are investigated using QCD Laplace sum rules. Masses are determined using appropriately constructed gauge invariant correlation functions,…

High Energy Physics - Phenomenology · Physics 2013-06-17 R. T. Kleiv , T. G. Steele , Ailin Zhang , Ian Blokland

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

High Energy Physics - Phenomenology · Physics 2008-12-18 D. Ebert , R. N. Faustov , V. O. Galkin

Recently, the LHCb Collaboration reported their observation of the first two fully open-flavor tetraquark states named $X_0(2900)$ and $X_1(2900)$ with unknown parity. Inspired by the report, we consider all of possible four-quark…

High Energy Physics - Phenomenology · Physics 2021-09-22 Yue Tan , Jialun Ping

In this article, we take the point of view that the $D_s(2700)$ be a tetraquark state, which consists of a scalar diquark and a vector antidiquark, and calculate its mass with the QCD sum rules. The numerical result indicates that the mass…

High Energy Physics - Phenomenology · Physics 2015-05-13 Zhi-Gang Wang

We investigate features of the hidden charm-strange scalar tetraquark $c \overline{c}s\overline{s}$ by calculating its spectral parameters and width, and we compare the obtained results with the mass and width of the resonance $ X(3960)$…

High Energy Physics - Phenomenology · Physics 2023-03-29 S. S. Agaev , K. Azizi , H. Sundu

The LHCb Collaboration has reported resonant activity in the channel $D^+ K^-$, identifying two components: $X_0(2900)$ with $J^P = 0^+$ at $2866 {\pm} 7$ MeV, $\Gamma_0=57{\pm} 13$ MeV and $X_1(2900)$ with $J^P = 1^-$ at $2904 {\pm} 7$…

High Energy Physics - Phenomenology · Physics 2020-11-25 Marek Karliner , Jonathan L. Rosner

We have studied the mass spectra of the hidden-charm/bottom $qc\bar q\bar c$, $sc\bar s\bar c$ and $qb\bar q\bar b$, $sb\bar s\bar b$ tetraquark states with $J^{PC}=0^{++}$ and $2^{++}$ in the framework of QCD sum rules. We construct ten…

High Energy Physics - Phenomenology · Physics 2017-12-20 Wei Chen , Hua-Xing Chen , Xiang Liu , T. G. Steele , Shi-Lin Zhu

Recently, a new hadronic structure at around $6.9$ GeV was observed in an LHCb experiment. From its limited yet known decay mode, one could still determine that it contains at least four charm quarks and hence belongs to the category of…

High Energy Physics - Phenomenology · Physics 2021-05-13 Bing-Dong Wan , Cong-Feng Qiao

Very recently the LHCb Collaboration reported their observation of the first two fully open-flavor tetraquark states, the $X_0(2900)$ of $J^P = 0^+$ and the $X_1(2900)$ of $J^P = 1^-$. We study their possible interpretations using the…

High Energy Physics - Phenomenology · Physics 2022-04-08 Hua-Xing Chen , Wei Chen , Rui-Rui Dong , Niu Su

The masses of heavy tetraquarks with hidden charm and bottom are calculated in the framework of the relativistic quark model. The tetraquark is considered as the bound state of a heavy-light diquark and antidiquark. The light quark in a…

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

The observation of $X_0(2900)$ in $B^+\rightarrow D^+D^-K^+$ decay process indicates the existence of open flavor tetraquark states. We study the production and decay of $X_0(2900)$ state with final state interaction mechanism, where we…

High Energy Physics - Phenomenology · Physics 2024-12-17 Zi-Yan Yang , Qian Wang , Wei Chen

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

In this work, $T_{cc}$ double charm tetraquark and $1^{+}$ and $0^{+}$ hidden charm tetraquarks are studied within the QCD sum rules framework. In the heavy-quark limit, the $1^+$ and $0^+$ tetraquarks are degenerate and the difference in…

High Energy Physics - Phenomenology · Physics 2025-02-11 Semra Sari Ferah , Altug Ozpineci