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Related papers: Axial Vector Tetraquark with Two s-quarks

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Possibility of an axial vector isoscalar tetraquark with $ud\bar{s}\bar{s}$ is discussed. If the pentaquark $\Theta^+(1540)$ has the $(qq)_{\bar{3}}(qq)_{\bar{3}}\bar{q}$ configuration, the isoscalar $ud\bar{s}\bar{s}$($\vartheta^+$-meson)…

High Energy Physics - Phenomenology · Physics 2008-11-26 Y. Kanada-En'yo , O. Morimatsu , T. Nishikawa

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

If a narrow Theta^+ pentaquark exists, it is likely that a ud\bar s-ud triquark-diquark configuration is a significant component of its wave function. If so, the mechanism responsible for the binding of a triquark and a diquark is also…

High Energy Physics - Phenomenology · Physics 2010-04-05 Marek Karliner , Harry J. Lipkin

The low-lying $S$-wave $QQ\bar{s}\bar{s}$ ($Q=c, b$) tetraquark states with $IJ^P=00^+$, $01^+$ and $02^+$ are systematically investigated in the framework of complex scaling range of chiral quark model. Every structure including…

High Energy Physics - Phenomenology · Physics 2020-09-30 Gang Yang , Jialun Ping , Jorge Segovia

The spectroscopic parameters and decay channels of the axial-vector tetraquark $T_{bb;\overline{u}\overline{s}}^{-}$ (in what follows, $T_{b: \overline{s}}^{\mathrm{AV}}$) are explored using the quantum chromodynamics (QCD) sum rule method.…

High Energy Physics - Phenomenology · Physics 2021-02-03 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

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

We discuss the likely tetraquark interpretation of the X(1576) K+ K- isovector resonance recently reported by BES with J^{PC}=1^{--}. We point out that if this interpretation as a four-quark state is correct, the (s u sbar dbar) tetraquark…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marek Karliner , Harry J. Lipkin

Recent data from Belle show unusually large partial widths Upsilon(5S) --> Upsilon(1S) pi^+pi^- and \Upsilon(5S) --> \Upsilon(2S) pi^+ pi^-. The Z(4430) narrow resonance also reported by Belle in psi' pi^+ spectrum has the properties…

High Energy Physics - Phenomenology · Physics 2008-03-04 Marek Karliner , Harry J. Lipkin

We look for the existence of stable (by strong interactions) tetraquarks, mesons containing two heavy antiquarks and two light quarks, specifically a $|{\bar b}{\bar b}qq\rangle$ state. This state is viewed as two $|{\bar b}q\rangle $…

High Energy Physics - Phenomenology · Physics 2016-09-01 Myron Bander , A. Subbaraman

If the exotic baryon $\Theta^+(1540)$ is a correlated $udud\bar{s}$ with $J^P = {1/2}^+$, then there should exist an exotic meson, $J^P = 1^-$ $\vartheta^+ (S=+2)$ $\to K^+K^0$ $\sim 1.6$GeV with width $O(10-100)$MeV. The $\pi_1(1400;1600)$…

High Energy Physics - Phenomenology · Physics 2014-11-18 T. Burns , F. E. Close , J. J. Dudek

We determine the mass of tetraquark bound states from a coupled system of covariant Bethe-Salpeter equations. Similar in spirit to the quark-diquark model of the nucleon, we approximate the full four-body equation for the tetraquark by a…

High Energy Physics - Phenomenology · Physics 2015-06-05 Walter Heupel , Gernot Eichmann , Christian S. Fischer

The charged axial-vector $J^{P}=1^{+}$ tetraquarks $Z_{q}=[cq][\bar {b} \bar q ]$ and $Z_{s}=[cs][\bar {b} \bar s]$ with the open charm-bottom contents are studied in the diquark-antidiquark model. The masses and meson-current couplings of…

High Energy Physics - Phenomenology · Physics 2017-06-28 S. S. Agaev , K. Azizi , H. Sundu

We study features of the resonances $X(2100)$ and $X(2239)$ by treating them as the axial-vector and vector tetraquarks with the quark content $ss \overline{s}\overline{s}$, respectively. The spectroscopic parameters of these exotic mesons…

High Energy Physics - Phenomenology · Physics 2020-01-08 K. Azizi , S. S. Agaev , H. Sundu

Spectroscopic parameters and widths of the fully open-flavor axial-vector and pseudoscalar tetraquarks $X_{\mathrm{AV}}$ and $X_{\mathrm{PS}}$ with content $[ud][\overline{c}\overline{s}]$ are calculated by means of the QCD sum rule…

High Energy Physics - Phenomenology · Physics 2023-03-22 H. Sundu , S. S. Agaev , K. Azizi

It is suggested that the narrow meson state seen in the the SELEX experiment is a $(c\bar{s} s\bar{s})$ tetraquark state. Characteristics of other possible tetraquarks formed out of $c$ and $s$ quarks and antiquarks are considered.

High Energy Physics - Phenomenology · Physics 2010-11-05 Virendra Gupta

The mass and coupling of the axial-vector tetraquark $T_{bc;\bar{u}\bar{d} }^{0}$ (in a short form $T_{bc}^{0}$) are calculated by means of the QCD two-point sum rule method. In computations we take into account contributions arising from…

High Energy Physics - Phenomenology · Physics 2020-01-29 S. S. Agaev , K. Azizi , H. Sundu

Using the color-magnetic interaction Hamiltonian with SU(3) flavor symmetry breaking, we perform a schematic study of the masses of the $J^P=1^+$ tetraquarks in the anti-decuplet representation. After diagonalizing the mass matrix, we find…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ying Cui , Xiao-Lin Chen , Wei-Zhen Deng , Shi-Lin Zhu

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

We study tetraquark resonances using lattice QCD potentials for a pair of static antiquarks $\bar{b}\bar{b}$ in the presence of two light quarks $ud$. The system is treated in the Born-Oppenheimer approximation and we use the emergent wave…

High Energy Physics - Lattice · Physics 2019-09-04 Martin Pflaumer , Pedro Bicudo , Marco Cardoso , Antje Peters , Marc Wagner

The BESIII Collaboration has observed a candidate for a $c \bar c s \bar u$ tetraquark $Z_{cs}$ at $(3982.5^{+1.8}_{-2.6} \pm 2.1)$ MeV and width $(12.8^{+5.3}_{-4.4} \pm 3.0)$ MeV, while the LHCb Collaboration has observed a $Z_{cs}$…

High Energy Physics - Phenomenology · Physics 2021-09-08 Marek Karliner , Jonathan L. Rosner
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