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Related papers: S-wave bottom tetraquarks

200 papers

In this work, we calculate the higher mass spectra for the $2S$- and $1D$-wave fully-charmed and fully-bottom tetraquark states in a nonrelativistic potential quark model. The $2S$-wave fully-charmed/bottom tetraquark states lie in the mass…

High Energy Physics - Phenomenology · Physics 2022-01-12 Feng-Xiao Liu , Ming-Sheng Liu , Xian-Hui Zhong , Qiang Zhao

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

Tetraquark states are classified using the $SU(6)_{sf}$ spin-flavor symmetry and Young tableau technique. Further, by using the extension of Gursey-Radicati mass formula, masses of tetraquark states are predicted upto good level of…

High Energy Physics - Phenomenology · Physics 2023-09-04 Ankush Sharma , Alka Upadhyay

We investigate the $S$-wave triply heavy tetraquark systems, including the $QQ^{(\prime)}\bar Q^{(\prime)}\bar q$ and $QQ^{(\prime)}\bar Q^{(\prime)}\bar s$ configurations ($Q^{(\prime)} = c, b$, $q = u, d$) with spin-parity $J^P = 0^+$,…

High Energy Physics - Phenomenology · Physics 2025-02-18 Hui-Min Yang , Yao Ma , Wei-Lin Wu , Shi-Lin Zhu

We investigate the spectrum of $T_{\Upsilon\Upsilon}$ tetraquark candidates within a coupled-channels framework. The analysis includes all $L\leq2$ combinations of $\Upsilon(1S)$, $\Upsilon(2S)$, $\eta_b(1S)$, and $\eta_b(2S)$ in the $J^P =…

High Energy Physics - Phenomenology · Physics 2026-03-06 P. G. Ortega , D. R. Entem , F. Fernandez , J. Segovia

The chromomagnetic interaction, with full account for flavour-symmetry breaking, is applied to S-wave configurations containing two quarks and two antiquarks. Phenomenological implications are discussed for light, charmed, charmed and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Franco Buccella , Hallstein Hogaasen , Jean-Marc Richard , Paul Sorba

In the framework of an extended chromomagnetic model, we systematically study the mass spectrum of the $S$-wave $qQ\bar{Q}\bar{Q}$ tetraquarks. Their mass spectra are mainly determined by the color interaction. For the $qc\bar{c}\bar{c}$,…

High Energy Physics - Phenomenology · Physics 2022-02-25 Xin-Zhen Weng , Wei-Zhen Deng , Shi-Lin Zhu

Considering four-point correlation functions of color-singlet quark bilinears, we investigate, in the large-$N_{\mathrm{c}}$ limit of QCD, the subleading diagrams that involve, in the $s$-channel of meson-meson scattering amplitudes,…

High Energy Physics - Phenomenology · Physics 2017-12-20 Wolfgang Lucha , Dmitri Melikhov , Hagop Sazdjian

The $s-$wave meson-baryon scattering amplitude is analyzed for the strangeness $S=-1$ and isospin I=0 sector in a Bethe-Salpeter coupled channel formalism incorporating Chiral Symmetry. Four two-body channels have been considered: $\bar K…

Nuclear Theory · Physics 2016-08-16 C. Garcia-Recio , J. Nieves , E. Ruiz Arriola , M. Vicente Vacas

The relativistic five-quark equations are found in the framework of the dispersion relation technique. The five-quark amplitude for the N(1688) resonance including u-, d- quarks is calculated. The pole of this amplitude determines the mass…

High Energy Physics - Phenomenology · Physics 2007-07-05 S. M. Gerasyuta , V. I. Kochkin

The relativistic four-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 2009-10-31 S. M. Gerasyuta , V. I. Kochkin

Recent calculations are presented of top quark polarization in $t\bar t$ pair production close to threshold. S-P-wave interference gives contributions to all components of the top quark polarization vector. Rescattering of the decay…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Jezabek , R. Harlander , J. H. Kuehn , M. Peter

The lowest-lying charmonium-like tetraquarks $c\bar{c}q\bar{q}$ $(q=u,\,d)$ and $c\bar{c}s\bar{s}$, with spin-parity $J^P=0^+$, $1^+$ and $2^+$, and isospin $I=0$ and $1$, are systematically investigated within the theoretical framework of…

High Energy Physics - Phenomenology · Physics 2023-03-28 Gang Yang , Jialun Ping , Jorge Segovia

In the framework of the chiral quark model along with complex scaling range, we perform a dynamical study on the low-lying $S$-wave doubly-heavy tetraquark states ($QQ\bar{q}\bar{q}$, $Q=c, b$ and $q=u, d$) with an accurate computing…

High Energy Physics - Phenomenology · Physics 2020-01-08 Gang Yang , Jialun Ping , Jorge Segovia

We present our recent investigation on doubly bottom and bottom-strange tetraquarks in the isoscalar channel in search of a possible tetraquark bound state. The calculations are performed on four ensembles with dynamical quark fields up to…

High Energy Physics - Lattice · Physics 2026-03-20 Bhabani Sankar Tripathy , Nilmani Mathur , M. Padmanath

Stimulated by the observation of the $X(6900)$ from LHCb in 2020 and the recent results from CMS and ATLAS in the di-$J/\psi$ invariant mass spectrum, in this work we systemically study all possible configurations for the ground fully heavy…

High Energy Physics - Phenomenology · Physics 2023-08-28 Hong-Tao An , Si-Qiang Luo , Zhan-Wei Liu , Xiang Liu

The relativistic six-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the heavy hexaquark…

High Energy Physics - Phenomenology · Physics 2015-05-28 S. M. Gerasyuta , E. E. Matskevich

Four-quark states may exist as colorless meson-meson molecules or compact systems with two-body colored components. We derive an analytical procedure to expand an arbitrary four--quark wave function in terms of nonorthogonal color…

High Energy Physics - Phenomenology · Physics 2014-11-20 J. Vijande , A. Valcarce

The energies of the low-lying isoscalar and isovector ud anti-s anti-s configurations with spin-parity J^P=0^+, 1^+, and 2^+ are calculated in a non-relativistic constituent quark model by use of the variational method. The contributions of…

Nuclear Theory · Physics 2007-07-16 W. L. Wang , F. Huang , Z. Y. Zhang , Y. W. Yu , F. Liu

This paper focuses on tetraquarks containing one heavy quark and one heavy antiquark in the formal limit where the heavy quark masses go to infinity. It extends the theoretical framework developed for tetraquark containing two heavy quarks…

High Energy Physics - Phenomenology · Physics 2020-09-02 Yiming Cai , Thomas Cohen