A homonuclear diatomic molecule is built from two identical nuclei

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Atomic, Molecular & Optical Physics · Symmetry, angular momentum and spin

Deriving the Spectrum, Ch Electronic spectra of diatomic molecules

Problem

A homonuclear diatomic molecule is built from two identical nuclei, each a boson with nuclear spin I=1I=1. Its ground electronic state is X 1Σg+X\,{}^1\Sigma_g^+, and a candidate excited state is A 1Σu−A\,{}^1\Sigma_u^-. ((a)) Using the electric-dipole selection rules for a diatomic electronic transition, together with the fact that the electric dipole operator is odd under spatial inversion, decide whether the transition A 1Σu−→X 1Σg+A\,{}^1\Sigma_u^- \to X\,{}^1\Sigma_g^+ is electric-dipole allowed. Justify each rule you apply. ((b)) For the ground state X 1Σg+X\,{}^1\Sigma_g^+, the pure rotational Raman spectrum shows an intensity alternation between even and odd initial rotational quantum number J′′J''. Using the requirement that the total wavefunction (electronic times vibrational times rotational times nuclear spin) be symmetric under exchange of the two identical bosonic nuclei, find the ratio of the statistical weight of an even-J′′J'' rotational level to that of an odd-J′′J'' level, and state which set of Raman lines (those starting from even J′′J'' or from odd J′′J'') is the stronger.

Related theory

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