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Related papers: Lowest vector tetraquark states: $Y(4260/4220)$ or…

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In this article, we construct the $C \otimes \gamma_\mu C$ and $C\gamma_5 \otimes \gamma_5\gamma_\mu C$ type currents to interpolate the vector tetraquark states, then carry out the operator product expansion up to the vacuum condensates of…

High Energy Physics - Phenomenology · Physics 2018-06-26 Zhi-Gang Wang

In this article, we introduce a P-wave between the diquark and antidiquark explicitly to construct the vector tetraquark currents, and study the vector tetraquark states with the QCD sum rules systematically, and obtain the lowest vector…

High Energy Physics - Phenomenology · Physics 2019-01-21 Zhi-Gang Wang

In this article, we construct the axialvector-diquark-axialvector-antidiquark type tensor current to interpolate both the vector and axialvector tetraquark states, then calculate the contributions of the vacuum condensates up to…

High Energy Physics - Phenomenology · Physics 2016-07-12 Zhi-Gang Wang

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 article, we tentatively assign the $Y(4140)$, $Y(4274)$ and $X(4350)$ to be the scalar and tensor $cs\bar{c}\bar{s}$ tetraquark states, respectively, and study them with the QCD sum rules. In the operator product expansion, we take…

High Energy Physics - Phenomenology · Physics 2015-02-17 Zhi-Gang Wang , Ye-Fan Tian

In this article, we take the $X(4140)$ as the diquark-antidiquark type $cs\bar{c}\bar{s}$ tetraquark state with $J^{PC}=1^{++}$, and study the mass and pole residue with the QCD sum rules in details by constructing two types interpolating…

High Energy Physics - Phenomenology · Physics 2016-11-30 Zhi-Gang Wang

In this article, we take the scalar diquark and antidiquark operators as the basic constituents, construct the $C\gamma_5\otimes\stackrel{\leftrightarrow}{\partial}_\mu\otimes \gamma_5C$ type tetraquark current to study the $Y(10750)$ with…

High Energy Physics - Phenomenology · Physics 2019-11-19 Zhi-Gang Wang

In this article, we separate the vector and axialvector components of the tensor diquark operators explicitly, construct the axialvector-axialvector type and vector-vector type scalar tetraquark currents and scalar-tensor type tensor…

High Energy Physics - Phenomenology · Physics 2019-10-28 Zhi-Gang Wang

In this paper, we apply the QCD sum rules to study the vector fully-light tetraquark states with an explicit P-wave between the diquark and antidiquark pair. We observed that the…

High Energy Physics - Phenomenology · Physics 2024-01-31 Qi Xin , Zhi-Gang Wang

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

In this article, we construct the axialvector-diquark-axialvector-antidiquark type currents to study both the vector and axialvector $QQ\bar{Q}\bar{Q}$ tetraquark states with the QCD sum rules, and obtain the masses…

High Energy Physics - Phenomenology · Physics 2019-07-16 Zhi-Gang Wang , Zun-Yan Di

Motivated by the enigmatic vector charmonium-like states, we investigate the strong decay behaviors of four kinds of vector tetraquark states, which are possible candidates for the $Y(4660)$, within the framework of three-point QCD sum…

High Energy Physics - Phenomenology · Physics 2026-05-18 Xiao-Song Yang , Zhi-Gang Wang

In this article, we calculate the contributions of the vacuum condensates up to dimension-10 in the operator product expansion, and study the $C\gamma_\mu-C\gamma_\nu$ type scalar, axial-vector and tensor tetraquark states in details with…

High Energy Physics - Phenomenology · Physics 2015-03-27 Zhi-Gang Wang

We suppose that there exist three vector hidden-charm tetraquark states with the $J^{PC}=1^{--}$ at the energy about $4.5\,\rm{GeV}$, and investigate the two-body strong decays systematically. We obtain thirty QCD sum rules for the hadronic…

High Energy Physics - Phenomenology · Physics 2024-06-13 Zhi-Gang Wang

In this article, we study the axial-vector mesons $Z_b(10610)$ and $Z_b(10650)$ with the $C\gamma_\mu-C\gamma_5$ type and $C\gamma_\mu-C\gamma_\nu$ type interpolating currents respectively by carrying out the operator product expansion to…

High Energy Physics - Phenomenology · Physics 2014-09-22 Zhi-Gang Wang , Tao Huang

In this article, we study the axialvector-diquark-axialvector-antidiquark type scalar, axialvector, tensor and vector $ss\bar{s}\bar{s}$ tetraquark states with the QCD sum rules. The predicted mass $m_{X}=2.08\pm0.12\,\rm{GeV}$ for the…

High Energy Physics - Phenomenology · Physics 2020-05-12 Zhi-Gang Wang

In this article, we assume the $Z_c(4200)$ as the color octet-octet type axial-vector molecule-like state, and construct the color octet-octet type axial-vector current to study its mass and width with the QCD sum rules. The numerical…

High Energy Physics - Phenomenology · Physics 2015-10-16 Zhi-Gang Wang

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

High Energy Physics - Phenomenology · Physics 2014-03-19 Zhi-Gang Wang , Tao Huang

In this article, we construct both the $[sc]_T[\bar{s}\bar{c}]_A+[sc]_A[\bar{s}\bar{c}]_T$ type and $[sc]_T[\bar{s}\bar{c}]_V-[sc]_V[\bar{s}\bar{c}]_T$ type axialvector currents with $J^{PC}=1^{++}$ to study the mass of the $X(4140)$ with…

High Energy Physics - Phenomenology · Physics 2019-01-30 Zhi-Gang Wang , Zun-Yan Di

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
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