Abstract

We present numerical MCSCF calculations of the electronic and nuclear components of the parallel molecular polarizabilities (α zz ) and the second hyperpolarizabilities (γ zzzz ) of H2, HD and D2. Contrary to the H+ 2 case, where the vibrational contribution to γ is fifty times larger than the pure electronic γ, the vibrational γ and the electronic γ for H2 have the same magnitude. The electronic correlation has a stronger effect on α and γ for vibrationally-excited states than for the ground state.

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