The bending mode of vibration in ICN introduces an asymmetry in the electric field gradient at the iodine nucleus. From an observed variation in the l-type doublet splittings of various hyperfine components for the v₂=1 state, the asymmetry parameter is determined as η=0.0087. It is found that the measured splittings can be accounted for fully by including second-order perturbation terms arising from field asymmetry. The ratio (eqQ)ᵥ₌₀(eqQ)_v₂=1 is measured as 1.0039. This ratio and the observed value of η are discussed in terms of the molecular bending and I-C bonding electrons.
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A. Javan (1955) studied this question.
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