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In this article, we assume that there exist hidden charmed tetraquark states with the spin-parity $J^P=1^-$, and calculate their masses with the QCD sum rules. The numerical result indicates that the masses of the vector hidden charmed…

High Energy Physics - Phenomenology · Physics 2009-02-19 Zhi-Gang Wang

Treating the $X(4140)$ as a compact $J^{PC}=1^{++}$ $cs\bar{c}\bar{s}$ state and using its mass as a reference scale, we systematically estimate the masses of doubly heavy tetraquark states $QQ\bar{q}\bar{q}$ where $Q=c,b$ and $q=u,d,s$.…

High Energy Physics - Phenomenology · Physics 2024-11-26 Shi-Yuan Li , Yan-Rui Liu , Zi-Long Man , Zong-Guo Si , Jing Wu

We study the possible exotic states with $J^{PC} = 0^{+-}$ using the tetraquark interpolating currents with the QCD sum rule approach. The extracted masses are around 4.85 GeV for the charmonium-like states and 11.25 GeV for the…

High Energy Physics - Phenomenology · Physics 2013-09-17 Meng-Lin Du , Wei Chen , Xiao-Lin Chen , Shi-Lin Zhu

We study the masses of light tetraquark states $ud\bar{u}\bar{d}$ , $us\bar{u}\bar{s}$ and $ss\bar{s}\bar{s}$ with exotic quantum numbers $J^{PC}=2^{+-}$ using the method of QCD sum rules. It is found that there is no tetraquark operator…

High Energy Physics - Phenomenology · Physics 2024-08-16 Qi-Nan Wang , Ding-Kun Lian , Wei Chen

In the present work, the mass spectra of doubly heavy tetraquarks $T_{QQ^\prime}$ are systematically investigated in a relativized quark model. The four-body systems including the Coulomb potential, confining potential, spin-spin…

High Energy Physics - Phenomenology · Physics 2020-08-19 Qi-Fang Lü , Dian-Yong Chen , Yu-Bing Dong

We investigate gluonic hidden-charm tetraquark states composed of two valence quarks, two valence antiquarks and an explicit valence gluon. In the color configuration $[\bar{3}_c]_{c q}\otimes[8_c]_{G}\otimes[3_c]_{\bar{c}\bar{q}}$, a…

High Energy Physics - Phenomenology · Physics 2026-05-05 Bing-Dong Wan , Ming-Yang Yuan , Jun-Hao Zhang , Yan Zhang

In this article, we study the ground states and the first radial excited states of the tensor-tensor type scalar hidden-charm tetraquark states with the QCD sum rules. We separate the ground state contributions from the first radial excited…

High Energy Physics - Phenomenology · Physics 2016-11-29 Zhi-Gang Wang , Jun-Xia Zhang

In this work, we tentatively assign the $Y(4500)$ as the $[uc]_{\tilde{A}}[\overline{uc}]_{V}+[uc]_{V}[\overline{uc}]_{\tilde{A}}+[dc]_{\tilde{A}}[\overline{dc}]_{V} +[dc]_{V}[\overline{dc}]_{\tilde{A}}$ tetraquark state with the quantum…

High Energy Physics - Phenomenology · Physics 2023-06-23 Zhi-Gang Wang

We estimate the mass of the pentaquark state with QCD sum rules and find that pentaquark states with isospin $I=0, 1, 2$ lie close to each other around $(1.55\pm 0.15)$ GeV. The experimentally observed baryon resonance $\Theta^+ (1540)$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Shi-Lin Zhu

If the Theta^+(1540) is interpreted as a bound state of a $\bar s$ quark and two (ud) diquarks in a relative P-wave, then it is very likely that there exist pentaquark states with a heavy antiquark, $\bar b$ or $\bar c$, and two ``light''…

High Energy Physics - Phenomenology · Physics 2010-04-05 Iain W. Stewart , Margaret E. Wessling , Mark B. Wise

Using the method of QCD Sum Rules, we derive the correlator $\Pi^Z$ for a state consisting of two charm quarks and two light quarks, $c\bar{c}u\bar{d}$, and carry out a Borel transform to find $\Pi^Z(M_B)$. From this we find the solution…

High Energy Physics - Phenomenology · Physics 2015-09-16 Leonard S. Kisslinger , Steven Casper

In this article, we present the scalar-diquark-scalar-diquark-antiquark type and scalar-diquark-axialvector-diquark-antiquark type pentaquark configurations in the diquark model, and study the masses and pole residues of the…

High Energy Physics - Phenomenology · Physics 2016-01-28 Zhi-Gang Wang , Tao Huang

Doubly heavy tetraquark states are the prime candidates for tightly bound exotic states. We present a systematic study of the mass spectra of the $S$-wave doubly heavy tetraquark states $QQ\bar{q}\bar{q}$ ($q=u, d, s$ and $Q=c, b$) with…

High Energy Physics - Phenomenology · Physics 2022-02-09 Tao Guo , Jianing Li , Jiaxing Zhao , Lianyi He

In this work, we adopt the diquark model, construct the diquark-diquark-antiquark type currents with the light quarks $uus$ in two octets, and study the $uusc\bar{c}$ pentaquark states in the framework of the QCD sum rules systematically.…

High Energy Physics - Phenomenology · Physics 2026-03-12 Zhi-Gang Wang , Yang Liu

In the present work, the triply heavy tetraquarks states $QQ\bar{Q}\bar{q}$ with $Q=(c, b)$ and $q=(u, d, s)$ with all possible quantum numbers are systematically investigated in the framework of the chiral quark model with the resonance…

High Energy Physics - Phenomenology · Physics 2023-03-15 Xuejie Liu , Yue Tan , Dianyong Chen , Hongxia Huang , Jialun Ping

We derive covariant equations describing the tetraquark in terms of an admixture of two-body states $D\bar D$ (diquark-antidiquark), $MM$ (meson-meson), and three-body-like states $q\bar q (T_{q\bar q})$, $q q (T_{\bar q\bar q})$, and $\bar…

High Energy Physics - Phenomenology · Physics 2023-05-24 A. N. Kvinikhidze , B. Blankleider

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

States beyond those expected in the simple constituent quark model are now emerging. I focus on the scalar glueball and its mixing with states in the $q\bar{q}$ nonet, and also on correlations in Strong QCD that may form diquarks and seed…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. E. Close

For very heavy quarks $Q$, relations derived from heavy-quark symmetry predict the existence of novel narrow doubly heavy tetraquark states of the form $Q_iQ_j \bar q_k \bar q_l$ (subscripts label flavors), where $q$ designates a light…

High Energy Physics - Phenomenology · Physics 2017-11-29 Estia J. Eichten , Chris Quigg

In this article, we assign the $Y(4390)$ and $Y(4220)$ to be the vector molecular states $D\bar{D}_1(2420)$ and $D^*\bar{D}_0^*(2400)$, respectively, and study their masses and pole residues with the QCD sum rules in details. The present…

High Energy Physics - Phenomenology · Physics 2017-06-30 Zhi-Gang Wang