SearcharxivSearch

arXiv subjects

Kento Kumakawa

Publications and source records attributed to Kento Kumakawa.

2 recordsLinked to original sources

Excitation spectra of heavy baryons in diquark models

The excitation energy spectra of heavy baryons consisting of a heavy quark and two light quarks are investigated by using diquark models in order to examine the nature of the diquark as a constituent of single heavy baryons. We consider two diquark models; in model A the diquark is treated as a point-like particle, while it has a spatial size in model B. We determine the masses of scalar and axial vector diquarks by the mass difference of the ground state charmed baryons to the $Λ_{c}$ baryon, while the mass of the $ud$ scalar diquark in the $Λ_{c}$ baryon is assumed to be 500 MeV as a reference. The parameters of these models are fixed by the $1p$ excitation energy of $Λ_{c}$. We find that model A reproduces well the excitation energy spectra of the charmed and bottomed baryons, although the string tension of the confinement potential in model A should be a half of that of the charmonium, while Model B suggests degeneracy of the $2s$ and $1d$ states, which is not seen in the $Λ_{c}$ spectrum.

hep-ph

Excitation energy spectra of the Lambda_c and Lambda_b baryons in a finite-size diquark model

The excitation energies of the $Λ_{c}$ and $Λ_{b}$ baryons are investigated in a finite-size diquark potential model, in which the heavy baryons are treated as bound states of a charm quark and a scalar-isoscalar diquark. The diquark is considered as a sizable object. The quark-diquark interaction is calculated as a sum of the quark-quark interaction which is assumed to be half of the quark-antiquark interaction for the color singlet. The potential parameters in the quark-antiquark interaction are fixed so as to reproduce the charmonium spectrum. We find the diquark size to be 1.1 fm for the diquark mass 0.5 GeV/c$^{2}$ to reproduce the $1p$ excitation energy of $Λ_{c}$. In this model, the $Λ_{c}$ and $Λ_{b}$ excitation spectra are reproduced well, while this model does not explain $Λ_{c}(2765)$, whose isospin nor spin-parity are unknown yet. Thus, the detailed properties of $Λ_{c}(2765)$ is very important to the presence of the diquark in heavy baryons as a effective constituent. We also discuss the $Ξ_{c}$ spectrum with the scalar strange diquark.

nucl-th