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201
Pseudo Nambu–Goldstone modes in neutron stars
Published 2017-06-01“…We study NG modes within a schematic quark model whose parameters at high density are constrained by the two-solar mass constraint. …”
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202
Instanton effects in twist-3 generalized parton distributions
Published 2024-01-01“…The spin-orbit correlations are qualitatively different from naive quark model expectations.…”
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203
Weak decays of triply heavy baryons
Published 2025-01-01“…We first obtain the form factors using the light-front quark model in the three-quark picture, and then apply them to arrive at some phenomenological predictions, including the decay widths of semileptonic decays and nonleptonic decays. …”
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204
Leading neutron production at HERA in the color dipole approach
Published 2016-01-01“…We describe this process using the color dipole formalism and, assuming the validity of the additive quark model, we relate the dipole-pion with the well determined dipoleproton cross section. …”
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205
Semileptonic transition of $$\varLambda _{b}$$ Λ b baryon
Published 2020-10-01“…Abstract The semileptonic transition of $$\varLambda _b$$ Λ b baryon is studied using the Hypercentral constituent quark model. The six-dimensional hyperradial $$Schr\ddot{o}dinger$$ S c h r o ¨ d i n g e r equation is solved in the variational approach to get masses and wavefunctions of heavy baryons. …”
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206
Universal behavior of mass gaps existing in the single heavy baryon family
Published 2021-05-01“…Under the framework of a constituent quark model, we quantitatively explain why such interesting phenomenon happens, when these established excited heavy baryons are regarded as the $$\lambda $$ λ -mode excitations. …”
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207
Spectrum of the $$uudc \bar{c}$$ uudcc¯ hidden charm pentaquark with an SU(4) flavor-spin hyperfine interaction
Published 2019-11-01“…Abstract We study a few of the lowest states of the pentaquark $$uudc\overline{c}$$ uudcc¯ , of positive and negative parity, in a constituent quark model with an SU(4) flavor-spin hyperfine interaction. …”
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208
Investigation of multi-quark systems
Published 2021-02-01“…These calculations are calculated using the approach of diquark - antidiquark within the framework of the non-relativistic quark model. In the following, we calculate the mass of Pentaquark systems in the same way.…”
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209
Bridging the two order parameters for the QCD deconfiment phase transition
Published 2018-01-01“…We study the relation between two order parameters for deconfinement, normally employed in the literature: the continuum threshold s0, in the context of QCD Sum Rules, and the trace of the Polyakov loop ϕ in the framework of a nonlocal SU(2) chiral quark model. We establish a bridge between both order parameters at finite temperature T and baryonic chemical potential μ. …”
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210
Dynamically generated magnetic moment in the Wigner-function formalism
Published 2019-05-01“…We derive the equal-time transport and constraint equations for the quark Wigner function in a magnetized quark model and solve them in the semi-classical expansion. …”
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211
Linking infrared and ultraviolet parameters of pion-like states in strongly coupled gauge theories
Published 2018-11-01“…Abstract It has been shown previously that in a relativistic constituent-quark model, predictions for the electromagnetic form factor of the $$\pi $$ π meson match not only experimental data but also, in the limit of large momentum transfers, the asymptotics derived from Quantum Chromodynamics (QCD). …”
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212
Mass and decay properties of double heavy baryons with a phenomenological potential model
Published 2020-04-01“…Abstract We consider baryons in a nonrelativistic quark model, find the wave function and masses of the baryons with two heavy quarks including $$\Xi _{bc}(bcu)$$ Ξbc(bcu) , $$\Xi _{cc}(ccu)$$ Ξcc(ccu) , $$\Xi _{bb}(bbu)$$ Ξbb(bbu) , $$\Omega _{bb}(bbs)$$ Ωbb(bbs) , $$\Omega _{bc}(bcs)$$ Ωbc(bcs) and $${\Omega _{cc}}(ccs)$$ Ωcc(ccs) . …”
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213
πe3 Form Factor f- Near the Mass Shell
Published 2015-01-01“…A numerical estimate of the form factor yields a value two times higher than the previous estimate from the quark model. Off-shell form factors are known to be ambiguous because of the gauge dependence and the freedom in the parameterization of the fields. …”
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214
Double parton scattering and the proton transverse structure at the LHC
Published 2019-09-01“…We develop the formalism to extract this information from dPDFs and present results by using constituent quark model calculations within the Light-Front approach, focusing on radiatively generated gluon dPDFs. …”
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215
In-medium pion valence distributions in a light-front model
Published 2017-03-01“…Pion valence distributions in nuclear medium and vacuum are studied in a light-front constituent quark model. The in-medium input for studying the pion properties is calculated by the quark-meson coupling model. …”
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216
NON-STRANGE VECTOR-MESON PRODUCTION IN K-P INTERACTIONS AT 4.2 GEV-C
Published 1978“…The results are compared with duality and quark model predictions, as well as used to test current ideas in two-body phenomenology. © 1978.…”
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217
Baryon magnetic moments in a simultaneous expansion in 1/N and ms.
Published 1995“…At leading order in this expansion, the magnetic moments obey the non-relativistic quark-model relations. We compute corrections to these relations using an effective lagrangian formalism which respects chiral symmetry to all orders in the $1/N$ expansion. …”
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218
Exploring the internal structure of exotic resonances with ALICE
Published 2024-01-01“…In the last decade, several resonances in the mass range 1000-2000 MeV/c2 have emerged that cannot be explained by the quark model. The internal structure of exotic resonances such as f0, f1, and f2 is currently unknown. …”
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219
Comparisons of magnetic charge and axial charge meson cloud distributions in the PCQM
Published 2017-08-01“…Abstract The meson cloud distributions in r-space are extracted from the nucleon electromagnetic and axial form factors which are derived in the perturbative chiral quark model. The theoretical results indicate that the magnetic charge and axial charge distributions of the three-quark core have the similar distributions in r-space, the magnetic charge distributions of the meson cloud and three-quark core are more or less in the same region and peak at distances of around 0.4 fm, which is in good agreement with the finding of works in the framework of chiral perturbation theory, but the axial charge meson cloud distributes mainly inside the three-quark core.…”
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220
Ωcγ→Ωc⁎ transition in lattice QCD
Published 2015-07-01“…The magnetic dipole form factor is found to be mainly determined by the strange quark and the electric quadrupole form factor to be negligibly small, in consistency with the quark model. We also evaluate the helicity amplitudes and the decay rate.…”
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