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Related papers: Five-quark components in baryons

200 papers

The role of 5-quark components in the pion and electromagnetic decays and transition form factors of the N(1440) is explored. The $qqqq\bar q$ components, where the 4-quark subsystem has the flavor-spin symmetries $[4]_{FS}[22]_F[22]_S$ and…

Nuclear Theory · Physics 2008-11-26 Q. B. Li , D. O. Riska

A new analysis is performed in QCD sum rule for the lightest negative parity baryon Lambda (1405). Mixings of three-quark and five-quark Fock components are taken into account. Terms containing up to dimension 12 condensates are computed in…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Nakamura , J. Sugiyama , N. Ishii , T. Nishikawa , M. Oka

An admixture of 10-20 % of qqqq\bar q components in the Delta(1232) resonance is shown to reduce the well known underprediction for the decay width for Delta(1232)->N gamma decay by about half and that of the corresponding helicity…

Nuclear Theory · Physics 2009-11-11 Q. B. Li , D. O. Riska

We have investigated the axial charges of the ground octet baryons within the extended chiral constituent quark model, where all the possible compact five-quark Fock components $qqq(q\bar{q}) (q=u, d, s)$ in the baryons are considered. The…

High Energy Physics - Phenomenology · Physics 2022-06-29 Rui Qi , Jin-Bao Wang , Gang Li , Chun-Sheng An , Cheng-Rong Deng , Ju-Jun Xie

A whole class of non-perturbative QCD studies, e.g. the instanton models, chiral quark models, etc. indicates that the effective degrees of freedom for the physics in the low Q^(2) < 1 GeV^(2) region could be the constituent quarks (CQs)…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. P. Cheng , Ling-Fong Li

The electroweak properties of nucleons and hyperons are calculated in a relativistic constituent quark model. The baryons are treated as three quark bound states, and the diagrams of perturbation theory are considered on the light front.…

High Energy Physics - Phenomenology · Physics 2009-09-25 Felix Schlumpf

Magnetic moments of the low lying and charmed spin 1/2^+ and spin 3/2^+ baryons have been calculated in the SU(4) chiral constituent quark model (\chiCQM) by including the contribution from c \bar c fluctuations. Explicit calculations have…

High Energy Physics - Phenomenology · Physics 2010-08-19 Neetika Sharma , Harleen Dahiya , P. K. Chatley , Manmohan Gupta

Baryons of the type Qqqqq-bar (where Q = c,b and q = u,d,s quarks) forming anti-decapenta (15)-plets with spin-parity one half-plus are predicted on simple theoretical considerations. The lightest members of these multiplets are explicitly…

High Energy Physics - Phenomenology · Physics 2010-03-11 Dmitri Diakonov

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…

High Energy Physics - Phenomenology · Physics 2016-09-06 Fl. Stancu

We perform a preliminary study of the 1/2+ and 3/2+ ground-state baryons containing a heavy quark in the framework of the chiral SU(3) quark model. By using the calculus of variations, masses of Lambda_Q, Sigma_Q, Xi_Q, Omega_Q, Sigma_Q^*,…

Nuclear Theory · Physics 2011-06-27 Qiao-Yan Zhao , Dan Zhang , Qiu-Yang Zhang

We treat the baryon as a composite system made out of a \lq\lq core" of three quarks (as in the standard quark model) surrounded by a \lq\lq sea" (of gluons and $q\bar{q}$-pairs) which is specified by its total quantum numbers like flavor,…

High Energy Physics - Phenomenology · Physics 2014-11-17 V. Gupta , R. Huerta , G. Sanchez-Colon

The calculation of the meson masses based on the 5D homogeneous space-time quantum projection was shown explicitly. There are no adjustable parameters, except the rest quark mass. The discovered p-p 125 GeV resonance was proposed by us as a…

General Physics · Physics 2015-04-14 K. W. Wong , G. Dreschhoff , H. Jungner

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…

High Energy Physics - Phenomenology · Physics 2008-02-03 M. A. Moinester , D. Ashery , L. G. Landsberg , H. J. Lipkin

If quark matter is energetically favored over nuclear matter at zero temperature and pressure then it has long been expected to take the form of strange quark matter (SQM), with comparable amounts of $u$, $d$, $s$ quarks. The possibility of…

High Energy Physics - Phenomenology · Physics 2018-06-06 Bob Holdom , Jing Ren , Chen Zhang

Recently LHCb reported the discovery of five extremely narrow excited $\Omega_c$ baryons decaying into $\Xi_c^+ K^-$. We interpret these baryons as bound states of a $c$-quark and a $P$-wave $ss$-diquark. For such a system there are exactly…

High Energy Physics - Phenomenology · Physics 2017-06-21 Marek Karliner , Jonathan L. Rosner

The spectra of baryons containing two heavy quarks test the form of the $QQ$ potential through the spin-averaged masses and hyperfine splittings. The mass splittings in these spectra are calculated in a nonrelativistic potential model and…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. L. Stong

Baryons with three heavy quarks are the last missing pieces of the lowest-lying baryon multiplets in the quark model after the discovery of doubly heavy baryons. In this work, we study nonleptonic weak decays of triply heavy baryons…

High Energy Physics - Phenomenology · Physics 2021-11-24 Fei Huang , Ji Xu , Xi-Ruo Zhang

Several experimental groups have reported evidence for baryons with flavor exotic quantum numbers that cannot be explained as $qqq$ bound states but require a minimum of five quarks -- $qqqq \bar q$. These pentaquark states include the…

High Energy Physics - Experiment · Physics 2009-11-10 A. R. Dzierba , C. A. Meyer , A. P. Szczepaniak

The effects of "quark sea" in determining the flavor structure of the octet baryons have been investigated in the chiral constituent quark model (\chiCQM). The \chiCQM is able to qualitatively generate the requisite amount of quark sea and…

High Energy Physics - Phenomenology · Physics 2014-11-21 Neetika Sharma , Harleen Dahiya

According to general understanding, the proton as one of the main ingredients of the nucleus is composed of one down and two up quarks bound together by gluons, described by Quantum Chromodynamics (QCD). In this view, heavy quarks do not…

High Energy Physics - Phenomenology · Physics 2023-12-22 A. R. Olamaei , S. Rostami , K. Azizi