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Related papers: Negative parity tetraquarks with the open charm

200 papers

The masses of the excited heavy tetraquarks with hidden charm are calculated within the relativistic diquark-antidiquark picture. The dynamics of the light quark in a heavy-light diquark is treated completely relativistically. The diquark…

High Energy Physics - Phenomenology · Physics 2008-12-18 D. Ebert , R. N. Faustov , V. O. Galkin

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The solutions of these equations using the method based on the extraction of leading singularities of the amplitudes are obtained. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. M. Gerasyuta , V. I. Kochkin

We argue that the hypothesis that positive-parity charm meson resonances exhibit a compact tetraquark structure has some clear tension with recent lattice results for the $S$-wave $\pi D$ system for an SU(3) flavor symmetric setting. In…

High Energy Physics - Phenomenology · Physics 2025-08-08 Feng-Kun Guo , Christoph Hanhart

The relativistic six-quark equations are constructed in the framework of the dispersion relation technique. The relativistic six-quark amplitudes of dibaryons including the light $u$, $d$ and heavy $c$, $b$ quarks are calculated. The…

High Energy Physics - Phenomenology · Physics 2015-05-30 S. M. Gerasyuta , E. E. Matskevich

The masses of negative parity $(70,1^-)$ charmed nonstrange baryons are calculated in the relativistic quark model. The relativistic three-quark equations of the $(70,1^-)$ charmed baryon multiplet are found in the framework of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Gerasyuta , E. E. Matskevich

A number of new four-quark states containing from one to four charm or anti-charm quarks have been observed recently. Many of these new states have been discovered at the LHC. The production of these states via intrinsic charm in the proton…

High Energy Physics - Phenomenology · Physics 2025-01-03 R. Vogt

In this work, we estimate the masses of tetraquark states with four different flavors by virtue of QCD sum rules, in both $b$ and $c$ sectors. We construct four $[8_c]_{\bar{b} s} \otimes [8_c]_{\bar{d} u}$ tetraquark currents with $J^P =…

High Energy Physics - Phenomenology · Physics 2016-11-23 Liang Tang , Cong-Feng Qiao

We study the masses of open charm and bottom tetraquark states within the diquark-antidiquark scenario in the relativized quark model proposed by Godfrey and Isgur. The diquark and antidiquark masses are firstly solved by relativized quark…

High Energy Physics - Phenomenology · Physics 2016-12-07 Qi-Fang Lü , Yu-Bing Dong

Masses of the ground and excited (1P, 2S, 1D, 2P, 3S) states of the fully-heavy tetraquarks, composed of charm ($c$) and bottom ($b$) quarks and antiquarks, are calculated in the diquark-antidiquark picture within the relativistic quark…

High Energy Physics - Phenomenology · Physics 2022-12-14 R. N. Faustov , V. O. Galkin , E. M. Savchenko

Masses of the ground-state teraquarks composed from heavy $c$ and $b$ quarks and antiquarks are calculated in the diquark-antidiquark picture in the framework of the relativistic quark model based on the quasipotential approach. The…

High Energy Physics - Phenomenology · Physics 2021-01-12 R. N. Faustov , V. O. Galkin , E. M. Savchenko

The relativistic model of the ground state and excited heavy tetraquarks with hidden bottom is formulated within the diquark-antidiquark picture. The diquark structure is taken into account by calculating the diquark-gluon vertex in terms…

High Energy Physics - Phenomenology · Physics 2009-04-17 D. Ebert , R. N. Faustov , V. O. Galkin

Diquarks are found to have the right degrees of freedom to describe the tetraquark poles in hidden-charm to open-charm meson-meson amplitudes. Compact tetraquarks result as intermediate states in non-planar diagrams of the 1/N expansion and…

High Energy Physics - Phenomenology · Physics 2016-07-20 L. Maiani , A. D. Polosa , V. Riquer

We investigate the production mechanism for doubly charmed tetraquark mesons within a coupled-channel formalism. The two-body Feynman kernel amplitudes are constructed using effective Lagrangians that respect heavy quark symmetry, chiral…

High Energy Physics - Phenomenology · Physics 2025-07-16 Hee-Jin Kim , Hyun-Chul Kim

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

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The solutions of these equations using the method based on the extraction of the leading singularities of the amplitudes are obtained.…

High Energy Physics - Phenomenology · Physics 2017-01-24 S. M. Gerasyuta , V. I. Kochkin

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

We give a review of the calculations of the masses of tetraquarks with two and four heavy quarks in the framework of the relativistic quark model based on the quasipotential approach and QCD. The diquark-antidiquark picture of heavy…

High Energy Physics - Phenomenology · Physics 2021-04-21 R. N. Faustov , V. O. Galkin , E. M. Savchenko

Charmed tetraquarks $T_{cc}=(cc\bar{u}\bar{d})$ and $T_{cs}=(cs\bar{u}\bar{d})$ are studied through the S-wave meson-meson interactions, $D$-$D$, $\bar{K}$-$D$, $D$-$D^{*}$ and $\bar{K}$-$D^{*}$, on the basis of the (2+1)-flavor lattice QCD…

A general classification of tetraquark states in terms of the spin-flavour, colour and spatial degrees of freedom has been constructed. The permutational symmetry properties of both the spin-flavour and orbital parts of the quark-quark and…

High Energy Physics - Phenomenology · Physics 2017-08-23 Elena Santopinto , Giuseppe Galatà

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