In RMF with NL3*, small components of Dirac spinors for neutrons near the Fermi level contribute to the proton potential and help form the kink in Sn charge radii at N=82, with j=l-1/2 states more effective than j=l+1/2, but the effect alone does not fully explain the observed magnitude.
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Charge radii of Sn isotopes in the relativistic mean field approximation
In RMF with NL3*, small components of Dirac spinors for neutrons near the Fermi level contribute to the proton potential and help form the kink in Sn charge radii at N=82, with j=l-1/2 states more effective than j=l+1/2, but the effect alone does not fully explain the observed magnitude.