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相关论文: Pentaquark in a supersmmetric quark-diquark model

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Recent experimental evidence for the Theta^+(1540) has given rise to much theoretical interest in exotic baryons. The Theta^+ is a baryon that has strangeness S=+1, meaning that it contains an anti-strange quark. Thus it cannot be…

高能物理 - 唯象学 · 物理学 2007-05-23 Margaret E Wessling

In some models, exotic baryons with strangeness and anticharm or antibeauty should exist and even be stable against strong decay. We consider the stability of such possible exotic baryons, which in the constituent quark picture are called…

高能物理 - 唯象学 · 物理学 2008-11-26 D. B. Lichtenberg

We propose a collective stringlike model of pentaquarks with the geometry of an equilateral tetrahedron in which the four quarks are located at the four corners and the antiquark in its center. The nonplanar equilibrium configuration is a…

高能物理 - 唯象学 · 物理学 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

The pentaquarks are exotic baryons formed of four quarks and an antiquarks. Their existence has been discussed in the literature over the last 30 years or more, first in connection with kaon nucleon scattering data. The subject has been…

高能物理 - 唯象学 · 物理学 2016-09-06 Fl. Stancu

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…

高能物理 - 唯象学 · 物理学 2007-05-23 Markus Eidemuller

We discuss the properties of the pentaquark in a collective stringlike model with a nonplanar configuration of the four quarks and the antiquark. In an application to the mass spectrum of exotic Theta baryons, we find that the ground state…

高能物理 - 唯象学 · 物理学 2017-11-02 R. Bijker , M. M. Giannini , E. Santopinto

Masses of heavy mesons, tetraquarks and pentaquarks computed in a potential model are shown. Tetraquarks are studied as bound states of a diquark and an antidiquark. Pentaquarks are constructed from a series of two-body interactions between…

高能物理 - 唯象学 · 物理学 2024-05-31 Floriana Giannuzzi

The strange pentaquarks with hidden heavy quark pair ($q^3c\bar c$ and $q^3b \bar b$) are investigated by the coupled-channel quark cluster model. Two types of the $q^3$ color-octet configurations are found to provide the attraction, which…

高能物理 - 唯象学 · 物理学 2025-07-29 Sachiko Takeuchi , Alessandro Giachino , Makoto Takizawa , Elena Santopinto , Makoto Oka

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 $\pi_1(1400;1600)$…

高能物理 - 唯象学 · 物理学 2014-11-18 T. Burns , F. E. Close , J. J. Dudek

Heavy baryon chiral perturbation theory for pentaquarks is applied beyond leading order. The mass splitting in the pentaquark anti-decuplet is calculated up to NNLO. An expansion in the coupling of pentaquarks to non-exotic baryons…

高能物理 - 唯象学 · 物理学 2009-11-10 Vivek Mohta

Spontaneous chiral symmetry breaking, mesons and baryons are illustrated in the language of the Dirac theory. Various forces acting between quarks inside baryons are discussed. I explain why the naive quark models typically overestimate…

高能物理 - 唯象学 · 物理学 2017-08-23 Dmitri Diakonov

The observation of the $T_{c\bar{s}}(2900)$ indicates the potential existence of strange double charm pentaquarks based on the heavy antidiquark symmetry. We systematically study the mass spectra of strange double charm pentaquarks with…

高能物理 - 唯象学 · 物理学 2024-05-21 Zi-Yan Yang , Qian Wang , Wei Chen

The strange-anticharmed Pentaquark is a uud(cbar)s or udd(cbar)s five-quark baryon that is expected to be either a narrow resonance, or possibly even stable against strong decay. We describe this hyperon here; its structure, binding energy…

高能物理 - 唯象学 · 物理学 2008-02-03 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

A dynamically broken hadron supersymmetry appears to exist as a consequence of QCD. The reasons for the supersymmetry appear most transparently in the framework of the constituent quark model with a diquark approximation to two quarks.…

高能物理 - 唯象学 · 物理学 2007-05-23 D. B. Lichtenberg

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…

高能物理 - 唯象学 · 物理学 2016-07-19 Majid Monemzadeh , Narges Tazimi , Shahnaz Babaghodrat

We consider exotic baryons with hidden charm as antiquark-diquark-diquark composite systems. Spin and isospin structure of such exotic states is given and masses are estimated. The data for production of pentaquarks in the reaction…

高能物理 - 唯象学 · 物理学 2015-07-29 V. V. Anisovich , M. A. Matveev , J. Nyiri , A. V. Sarantsev , A. N. Semenova

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…

高能物理 - 唯象学 · 物理学 2009-11-10 C. Semay , F. Brau , B. Silvestre-Brac

Pentaquark baryons are a natural expectation of an extended picture of hadrons where quarks and diquarks are the fundamental units. The parity/mass pattern observed, when compared to that of exotic mesons, appears as the footprint of a…

高能物理 - 唯象学 · 物理学 2015-09-30 L. Maiani , A. D. Polosa , V. Riquer

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…

高能物理 - 唯象学 · 物理学 2021-01-12 R. N. Faustov , V. O. Galkin , E. M. Savchenko

We analyse the width of the $\theta(\frac12^+)$ pentaquark assuming that it is a bound state of two extended spin-zero $ud$-diquarks and the $\bar s$ antiquark (the Jaffe-Wilczek scenario). The width obtained when the size parameters of the…

高能物理 - 唯象学 · 物理学 2009-11-10 D. Melikhov , S. Simula , B. Stech
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