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Related papers: Open charm-bottom scalar tetraquarks and their str…

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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

The spectroscopic parameters and decay channels of the doubly charged scalar, pseudoscalar and axial-vector charm-strange tetraquarks $Z_{ \overline{c}s}=[sd][\overline u \overline c]$ are explored within framework of the QCD sum rule. The…

High Energy Physics - Phenomenology · Physics 2018-04-04 S. S. Agaev , K. Azizi , 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

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

The strong decays of the pseudoscalar and scalar double-charmed tetraquarks $ T_{cc;\overline{u}\overline{d}}^{+}$ and $\widetilde{T}_{cc;\overline{u} \overline{d}}^{+}$ are investigated in the framework of the QCD sum rule method. The mass…

High Energy Physics - Phenomenology · Physics 2019-06-26 S. S. Agaev , K. Azizi , H. Sundu

The fully heavy scalar tetraquarks $T_{\mathrm{4Q}}=QQ\overline{Q}\overline{Q }$, ($Q=c, b$) are explored in the context of QCD sum rule method. We model $ T_{\mathrm{4Q}}$ as diquark-antidiquark systems composed of pseudoscalar…

High Energy Physics - Phenomenology · Physics 2023-10-12 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

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 mass and width of the tensor tetraquark $T=bb\overline{c}\overline{c}$ with spin-parity $J^{\mathrm{P}}=2^{+}$ are calculated in the context of the QCD sum rule method. The tetraquark $T$ is modeled as a diquark-antidiquark state built…

High Energy Physics - Phenomenology · Physics 2024-07-23 S. S. Agaev , K. Azizi , H. Sundu

Mass and width of a hidden charm-bottom axial-vector structure $T$ containing $bc \overline{b}\overline{c}$ quarks are calculated in QCD sum rule framework. It is treated as a diquark-antidiquark state built of scalar diquark and…

High Energy Physics - Phenomenology · Physics 2025-03-20 S. S. Agaev , K. Azizi , H. Sundu

In this work, we study the properties of the pseudoscalar hidden-charm tetraquark states by analyzing their two-body strong decays via the QCD sum rules based on rigorous quark-hadron duality. We take into account the vacuum condensates up…

High Energy Physics - Phenomenology · Physics 2026-05-05 Yu-Hang Xu , Zhi-Gang Wang

The mass and coupling of the doubly charmed $J^P=0^{-}$ diquark-antidiquark states $T_{cc;\bar{s} \bar{s}}^{++}$ and $T_{cc;\bar{d} \bar{s}}^{++}$ that bear two units of the electric charge are calculated by means of QCD two-point sum rule…

High Energy Physics - Phenomenology · Physics 2019-01-30 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

The weak decays of the axial-vector tetraquark $T_{bb;\bar{u} \bar{d}}^{-}$ to the scalar state $Z_{bc;\bar{u} \bar{d}}^{0}$ are investigated using the QCD three-point sum rule approach. In order to explore the process $T_{bb; \bar{u}…

High Energy Physics - Phenomenology · Physics 2019-02-13 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

Parameters of the heavy four-quark scalar meson $T_{\mathrm{bc\overline{b} \overline{c}}}$ with content $bc \overline{b}\overline{c}$ are calculated by means of the sum rule method. This structure is considered as a diquark-antidiquark…

High Energy Physics - Phenomenology · Physics 2024-09-27 S. S. Agaev , K. Azizi , H. Sundu

We apply the method of QCD sum rules to study the doubly heavy tetraquark states $QQ\bar{q}\bar{n}$ with spin-parity $J^{P}=1^{+}$ and strangeness $S=0, -1$ using careful estimates of the Borel and threshold parameters involved. Masses of…

High Energy Physics - Phenomenology · Physics 2023-08-15 Di Gao , Duojie Jia , Yan-Jun Sun

Temperature dependences of masses and current couplings of the ground state of the fully heavy tetraquarks $T_{4c}$ and $T_{4b}$, composed of charm $(c)$ and bottom $(b)$ quarks and antiquarks with spin-parities $J^{PC} = 0^{++}$ are…

High Energy Physics - Phenomenology · Physics 2025-01-20 A. Aydın , H. Sundu , J. Y. Süngü , E. Veli Veliev

Properties of doubly charged scalar tetraquarks $bb\overline{c}\overline{c}$ are investigated in the framework of the QCD sum rule method. We model them as diquark-antidiquark states $X_{\mathrm{1}}$ and $X_{\mathrm{2}}$ built of…

High Energy Physics - Phenomenology · Physics 2023-12-19 S. S. Agaev , K. Azizi , B. Barsbay , H. Sundu

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

Within the framework of QCD sum rules, we have investigated the tetraquark states with three heavy quarks. We systematically construct the interpolating currents for the possible $cc\bar{c}\bar{q}$, $cc\bar{b}\bar{q}$, $bc\bar{b}\bar{q}$,…

High Energy Physics - Phenomenology · Physics 2017-11-30 Jin-Feng Jiang , Wei Chen , Shi-Lin Zhu

Based on the diquark configuration, we construct the diquark-antidiquark interpolating tetraquark currents with $J^{PC}=1^{-\pm}$ and $1^{+\pm}$, which can couple to the scalar and pseudoscalar tetraquark states respectively, since they are…

High Energy Physics - Phenomenology · Physics 2018-06-25 Zun-Yan Di , Zhi-Gang Wang

Masses of tetraquarks with two heavy quarks and open charm and bottom are calculated in the framework of the diquark-antidiquark picture in the relativistic quark model. All model parameters were regarded as fixed by previous considerations…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Ebert , R. N. Faustov , V. O. Galkin , W. Lucha
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