Abstract
The shielding correction Δ defined by Q=(1+Δ)Q′ (Q=true quadrupole moment; Q′=apparent quadrupole moment obtained by spectroscopic means neglecting the shielding effect) was investigated in the cases of the state 5d46s of Ta I and 5d66s6p of Os189 I. In these cases the correction Δ for the group 5d46s or 5d66s was found to be of the order of 9±5; namely the shielding effect predominates over the antishielding effect. It is highly probable that Δ is around zero in the state 5d6 of Os I. The quadrupole moment of Os189 is 0.8±0.2 barn. The hyperfine structure due to Os187 was also studied, and μ(187)=+0.0656±0.0006 nm, was obtained.