Abstract

We study chiral partner structure of four light nucleons, $N(939)$, $N(1440)$, $N(1535)$ and $N(1650)$ using an effective chiral model based on the parity doublet structure. In our model we introduce four chiral representations, $({\bf 1},{\bf 2})$, $({\bf 2},{\bf 1})$, $({\bf 2},{\bf 3})$ and $({\bf 3},{\bf 2})$ under ${\rm SU}(2)_{\rm L} \otimes {\rm SU}(2)_{\rm R}$ symmetry. We determine the model parameters by fitting them to available experimental values of masses, widths and the axial charge of $N(939)$ together with the axial charges of $N(1535)$ and $N(1650)$ by lattice analyses. We find five groups of solutions: In a group the chiral partner to $N(939)$ is $N(1440)$ having small chiral invariant mass. In another group, the chiral partner is a mixture of $N(1535)$ and $N(1650)$ having a large chiral invariant mass. We claim that off-diagonal elements of axial-charge matrix can be used for distinguishing these groups. We also discuss changes of masses associated with chiral symmetry restoration, which could emerge in high density matter.

Highlights

  • One of the most important features of QCD relevant to the low-energy hadron physics is the chiral symmetry and its spontaneous breaking

  • It is interesting to study the role of the chiral symmetry breaking to determine the properties and structures of baryons such as amount of the masses of baryons generated by the chiral symmetry breaking and the chiral partner of ground state nucleon

  • One of the important features of the model is the existence of the chiral invariant mass denoted by m0 which is not originated from the spontaneous chiral symmetry breaking

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Summary

INTRODUCTION

One of the most important features of QCD relevant to the low-energy hadron physics is the chiral symmetry and its spontaneous breaking. The mass splitting between Nð939Þ and its chiral partner Nð1535Þ is given by the spontaneous chiral symmetry breaking, which implies that the masses of Nð939Þ and Nð1535Þ approach m0 when the chiral symmetry is restored This parity doublet structure is extended to include hyperons and/or excited nucleons such as Nð1440Þ and Nð1650Þ In a group of solutions, the chiral partner of Nð939Þ is Nð1440Þ having small chiral invariant mass of about 100 MeV and Nð939Þ is dominated by the 1⁄2ð2; 3Þ ⊕ ð3; 2ފ representation. In another group, on the other hand, Nð939Þ belongs dominantly to the 1⁄2ð1; 2Þ ⊕ ð2; 1ފ representation having a large.

AN EXTENDED PARITY DOUBLET MODEL
Mass matrix
CHIRAL INVARIANT MASSES AND PARTNER STRUCTURE
The relation values of gAðN2Þ is determined by
Change of nucleon masses
SUMMARY AND DISCUSSIONS
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