Abstract
The hyperfine structure in the 3Π1 state of InH, which deviates strongly from the magnetic hyperfine interval rule, is explained by the electric quadrupole interaction of the In nucleus. The quadrupole coupling constant for the 3Π1 (v=0) state eQqπ is +0.1 cm−1±100%. The off‐diagonal quadrupolar interaction, namely the eQ sin2θ exp (±2iφ)/r3 part, gives an F‐dependent contribution to the Λ‐type doubling of the 3Π1 (v=0) state, eQq′ = +0.066 cm−1(2000 Mc/sec)±50%. An upper limit to the quadrupole coupling constant of the X 1Σ+ (v=0) state is ∼|eQqx|≳0.07 cm−1±100%. The theory of hyperfine structure in Hund's Case (c) is discussed, and the matrix elements of the hyperfine interactions are evaluated for two Case (c) coupling schemes for a diatomic molecule with two nuclear spins. The matrix elements are evaluated by the generalization of Van Vleck's method of reversed angular momenta to spherical tensor form.