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Related papers: Pentaquarks in the Jaffe-Wilczek approximation

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The masses of $uudd\bar s $, $uudd\bar d$, and $uuss\bar d$ pentaquarks are evaluated in a framework of both the Effective Hamiltonian approach to QCD and spinless Salpeter using the Jaffe-Wilczek diquark approximation and the string…

High Energy Physics - Phenomenology · Physics 2009-11-10 I. M. Narodetskii , C. Semay , B. Silvestre-Brac , Yu. A. Simonov

The masses of $uudd\bar s $ and $uudd\bar d$ pentaquarks are evaluated in a framework of the Effective Hamiltonian approach to QCD using the Jaffe-Wilczek $[ud]^2\bar q$ approximation. The mass of the $[ud]^2\bar s$ state is found to be…

High Energy Physics - Phenomenology · Physics 2015-06-25 I. M. Narodetskii , Yu. A. Simonov , M. A. Trusov , A. I. Veselov

The masses of pentaquarks $uudd\bar s$ are calculated within the framework of a semirelativistic effective QCD Hamiltonian, using a diquark picture. This approximation allows a correct treatment of the confinement, assumed here to be…

High Energy Physics - Phenomenology · Physics 2009-11-10 C. Semay , F. Brau , B. Silvestre-Brac

We have investigated uudd\sbar pentaquarks by employing quark models with the meson exchange and the effective gluon exchange as qq and q\qbar interactions. The system for five quarks is dynamically solved; two quarks are allowed to have a…

High Energy Physics - Phenomenology · Physics 2017-08-23 Sachiko Takeuchi , Kiyotaka Shimizu

In the article, we investigate the diquark-diquark-antiquark type fully-heavy pentaquark states with the spin-parity $J^P={\frac{1}{2}}^-$ via the QCD sum rules, and obtain the masses $M_{cccc\bar{c}}=7.93\pm 0.15\,\rm{GeV}$ and…

High Energy Physics - Phenomenology · Physics 2021-10-26 Zhi-Gang Wang

In this work we investigate the consequences of the Jaffe and Wilczek diquark model in the framework of QCD sum rules. An analysis of the Theta^+(1540) as (ud)^2\bar{s} state shows that the mass of the pentaquark is compatible with the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Markus Eidemuller

The mass spectra of light-heavy tetraquarks $cq\bar{c}\bar{q}$ (q= u, d) are computed in a non-relativistic diquark model with one-gluon exchange plus confining potential. In the diquark model, a $cq\bar{c}\bar{q}$ state is regarded to be…

High Energy Physics - Phenomenology · Physics 2022-05-03 Rohit Tiwari , Juhi Oudichhya , Ajay Kumar Rai

We have investigated negative-parity uudd\bar{s} pentaquarks by employing a quark model with the meson exchange and the effective gluon exchange as qq and q\bar{q} interactions. The system for the five quarks is dynamically solved; the…

High Energy Physics - Phenomenology · Physics 2009-11-10 Sachiko Takeuchi , Kiyotaka Shimizu

According to QCD, there exists a broken dynamical supersymmetry between an antiquark and a diquark. This supersymmetry can be used to relate the mass of a pentaquark to the mass of an antibaryon by replacing two antiquarks in an antibaryon…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg

In this article, we study the scalar-diquark-scalar-diquark-antiquark type $udsc\bar{c}$ pentaquark state with the QCD sum rules, the predicted mass $M_P=4.47\pm0.11\,\rm{GeV}$ is in excellent agreement with the experimental data $ 4458.8…

High Energy Physics - Phenomenology · Physics 2021-04-05 Zhi-Gang Wang

Masses of the ground state light tetraquarks are dynamically calculated in the framework of the relativistic diquark-antidiquark picture. The internal structure of the diquark is taken into account by calculating the form factor of the…

High Energy Physics - Phenomenology · Physics 2010-04-15 D. Ebert , R. N. Faustov , V. O. Galkin

In this paper, we consider an exotic baryon (pentaquark) as a bound state of two-particle systems composed of a baryon (nucleon) and a meson.We used a baryon - meson picture to reduce a complicated five-body problem to a simple two-body…

High Energy Physics - Phenomenology · Physics 2016-07-19 Majid Monemzadeh , Narges Tazimi , Shahnaz Babaghodrat

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 splittings between positive parity pentaquarks containing a single heavy (c,b) antiquark and four light (u,d) quarks are investigated in models having spin-dependent interactions generated by either effective Goldstone boson exchange or…

High Energy Physics - Phenomenology · Physics 2009-11-10 K. Maltman

Light and heavy pentaquarks are described within a constituent quark model based on a spin-flavor hyperfine interaction. In this model the lowest state acquires positive parity. The masses of the light antidecuplet members are calculated…

High Energy Physics - Phenomenology · Physics 2009-11-11 Fl. Stancu

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 stability of strange pentaquarks $uudd\bar s$ is studied in a constituent quark model based on a flavor-spin hyperfine interaction between quarks. With this interaction model, which schematically represents the Goldstone boson exchange…

High Energy Physics - Phenomenology · Physics 2015-06-25 Fl. Stancu , D. O. Riska

We present a numerical solution of the four-quark Bethe-Salpeter equation for ground-state scalar tetraquarks with J^PC = 0^++. We find that the four-body equation dynamically generates pseudoscalar-meson poles in the Bethe-Salpeter…

High Energy Physics - Phenomenology · Physics 2015-12-21 Gernot Eichmann , Christian S. Fischer , Walter Heupel

We study the stability of the pentaquarks uuddQbar, uudsQbar and udssQbar (Q = c, b, or t) of positive parity in a constituent quark model based on Goldstone boson exchange interaction between quarks. The pentaquark parity is the antiquark…

High Energy Physics - Phenomenology · Physics 2009-12-30 Fl. Stancu

Inspired by the observation of a resonant state $X(6600)$ of fully charm tetraquark by the CMS experiment of LHCb Collaboration in double $J/\psi $ decay channel, we perform a systematical study of all configurations of fully heavy…

High Energy Physics - Phenomenology · Physics 2023-09-14 WenXuan Zhang , HongTao An , Duojie Jia
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