Hyperfine splitting of quarkonium

Abstract
Using a QCD-motivated model we show that [M(3 S1 )]2-[M(1 S0 )]2 is nearly constant for all quarkonium states. We find that the acceptable range of the QCD scale parameter to explain the weak quark-mass dependence of [M(3 S1 )]2-[M(1 S0 )]2 is Λ=140±60 MeV.