Mixing of the low-lying three- and five-quark ΩΩ states with negative parity

preprint2013arXivOpen access

Abstract

Mixing of the low-1/2^{-}and and 3/2^{-}isinvestigated,employinganinstanton−inducedquark−antiquarkpaircreationmodel,whichprecludestransitionsbetween is investigated, employing an instanton-induced quark-antiquark pair creation model, which precludes transitions between s^{3}and and s^{4}\bar{s}configurations.Modelswithhyperfineinteractionsbetweenquarksofthreedifferentkinds,namely,one−gluon−exchange,Goldstone−boson−exchange(GBE)andaninstanton−inducedinteraction(INS)arecalledOGE,GBEandINSmodels,respectively.Numericalresultsshowthattheinstanton−inducedpaircreationcausesstrongmixingbetweenthethree−andfive−quarkconfigurationswithspin3/2,andthatthismixingdecreasestheenergyofthelowestspin3/2statesinallthreedifferenthyperfineinteractionmodelsto configurations. Models with hyperfine interactions between quarks of three different kinds, namely, one-gluon-exchange, Goldstone-boson-exchange (GBE) and an instanton-induced interaction (INS) are called OGE, GBE and INS models, respectively. Numerical results show that the instanton-induced pair creation causes strong mixing between the three- and five-quark configurations with spin 3/2, and that this mixing decreases the energy of the lowest spin 3/2 states in all three different hyperfine interaction models to \sim 1750\pm50MeV.Ontheotherhand,transitioncouplingsbetween MeV. On the other hand, transition couplings between s^3and and s^{3}q\bar{q}stateswithspin1/2causedbyinstanton−induced states with spin 1/2 caused by instanton-induced q\bar{q}creationisverysmallandtheresultingmixingofthree−andfive−quarkconfigurationsintheOGEandINSmodelsisnegligible,whilethemixingofthespin1/2statesinGBEmodelisnot,buteffectsofthismixingonenergiesofmixedstatesarealsoverysmall.Accordingly,thelowest creation is very small and the resulting mixing of three- and five-quark configurations in the OGE and INS models is negligible, while the mixing of the spin 1/2 states in GBE model is not, but effects of this mixing on energies of mixed states are also very small. Accordingly, the lowest Ω$ states with negative parity in all three hyperfine interactions models have spin 3/2.

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