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Related papers: Vector hidden-bottom tetraquark candidate: $Y(1075…

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Experimentally several charged axial-vector hidden-charm states were reported. Within the framework of the color-magnetic interaction, we have systematically considered the mass spectrum of the hidden-charm and hidden-bottom tetraquark…

High Energy Physics - Phenomenology · Physics 2014-12-01 Lu Zhao , Wei-Zhen Deng , Shi-Lin Zhu

In this article, we study the mass spectrum of the scalar hidden charm and bottom tetraquark states with the QCD sum rules. The numerical results are compared with the corresponding ones from a relativistic quark model based on a…

High Energy Physics - Phenomenology · Physics 2010-04-23 Zhi-Gang Wang

We study the spectroscopy and dominant decays of the bottomonium-like tetraquarks (bound diquarks-antidiquarks), focusing on the lowest lying P-wave $[bq][\bar{b}\bar{q}]$ states $Y_{[bq]}$ (with $q=u,d$), having $J^{PC}=1^{--}$. To search…

High Energy Physics - Phenomenology · Physics 2010-05-28 Ahmed Ali , Christian Hambrock , Ishtiaq Ahmed , M. Jamil Aslam

In this article, we investigate the mass spectrum of the ground state hidden-charm tetraquark molecular states without strange, with strange and with hidden-strange via the QCD sum rules in a comprehensive way and revisit the assignments of…

High Energy Physics - Phenomenology · Physics 2021-10-13 Zhi-Gang Wang

Accessing a full picture of the internal structure of hadrons would be a key topic of hadron physics, with the main motivation to study the strong interaction binding the visible matter. Furthermore, the underlying structure of known exotic…

High Energy Physics - Phenomenology · Physics 2024-12-10 U. Özdem

We tentatively assign the $Y(4230)$ as the vector tetraquark state with a relative P-wave between the scalar diquark pair, and explore the three-body strong decays $Y(4230) \to \bar{D}^{*-}D^{*0}\pi^+$, $\bar{D}^{*-}D^0\pi^+$,…

High Energy Physics - Phenomenology · Physics 2024-02-13 Zhi-Gang Wang

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

In this article, we construct the axialvector-diquark-scalar-antidiquark type currents to interpolate the axialvector doubly heavy tetraquark states, and study them with the QCD sum rules in details by carrying out the operator product…

High Energy Physics - Phenomenology · Physics 2018-10-26 Zhi-Gang Wang

The masses, current couplings and widths of the fully heavy scalar tetraquarks $X_{\mathrm{4Q}}=QQ\overline{Q}\overline{Q}$, $Q=c, b$ are calculated by modeling them as four-quark systems composed of axial-vector diquark and antidiquark.…

High Energy Physics - Phenomenology · Physics 2023-11-01 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

We use the QCD sum rules to evaluate the mass of a possible scalar mesonic state that couples to a molecular $D_{s}^{*}\bar{D}_s^{*}$ current. We find a mass $m_{D_s^*D_s^*}=(4.14\pm 0.09)$ GeV, which is in a excellent agreement with the…

High Energy Physics - Phenomenology · Physics 2015-05-13 Raphael M. Albuquerque , Mirian E. Bracco , Marina Nielsen

We use QCD sum rules to test the nature of the recently observed mesons Y(4260), Y(4350) and Y(4660), assumed to be exotic four-quark $(c\bar{c}q\bar{q})$ or $(c\bar{c}s\bar{s})$ states with $J^{PC}=1^{--}$. We work at leading order in…

High Energy Physics - Phenomenology · Physics 2011-04-28 R. M. Albuquerque , M. Nielsen

Symmetries play important roles in the understanding of hadron structures and spectroscopy. Motivated by the discovery of the doubly charmed tetraquark $T_{cc}^+(3875)$, we study the ground states of the doubly heavy tetraquarks with the…

High Energy Physics - Phenomenology · Physics 2023-04-26 Tian-Wei Wu , Yong-Liang Ma

We investigate the newly observed $X(4500)$ and $X(4700)$ based on the diquark-antidiquark configuration within the framework of QCD sum rules. Both of them may be interpreted as the $D$-wave $cs\bar{c}\bar{s}$ tetraquark states of $J^P =…

High Energy Physics - Phenomenology · Physics 2017-03-17 Hua-Xing Chen , Er-Liang Cui , Wei Chen , Xiang Liu , Shi-Lin Zhu

In this article, we study the $C\gamma_5\otimes \gamma_5C$ type and $C\otimes C$ type scalar $cs\bar{c}\bar{s}$ tetraquark states with the QCD sum rules by calculating the contributions of the vacuum condensates up to dimension 10 in a…

High Energy Physics - Phenomenology · Physics 2017-02-03 Zhi-Gang Wang

We introduce a relative P-wave to construct the vector doubly-charm diquark $(\widetilde{V})$, therefore, the scalar and tensor four-quark currents to investigate the decay widths of the fully-charm tetraquark states with the…

High Energy Physics - Phenomenology · Physics 2025-04-30 Xiao-Song Yang , Zhi-Gang Wang

The mass and coupling of the scalar tetraquark $T_{bb;\overline{u}\overline{d }}^{-}$ (hereafter $T_{b:\overline{d}}^{-} $) are calculated in the context of the QCD two-point sum rule method. In computations we take into account effects of…

High Energy Physics - Phenomenology · Physics 2020-08-26 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

The scalar tetraquarks $T_{b}$ and $T_{c}$ with asymmetric contents $bb \overline{b}\overline{c}$ and $cc \overline{c}\overline{b}$ are explored using the QCD sum rule method. These states are modeled as the diquark-antidiquarks composed of…

High Energy Physics - Phenomenology · Physics 2025-05-26 S. S. Agaev , K. Azizi , H. Sundu

Inspired by the newly reported $Z_{cs}(3985)^{-}$ by the BESIII Collaboration, we systematically investigate the strange hidden-charm tetraquark systems $cs\bar{c}\bar{u}$ with two structures: meson-meson and diquark-antidiquark. Two quark…

High Energy Physics - Phenomenology · Physics 2022-01-05 Xin Jin , Xuejie Liu , Yaoyao Xue , Hongxia Huang , Jialun Ping

Using the QCD sum rule approach we study the Y(4260) state assuming that it can be described by a mixed charmonium-tetraquark current with $J^{PC}=1^{--}$ quantum numbers. For the mixing angle around $\theta \approx (53.0\pm 0.5)^{0}$, we…

High Energy Physics - Phenomenology · Physics 2013-06-19 J. M. Dias , R. M. Albuquerque , M. Nielsen , C. M. Zanetti

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