The parity non-conservation (PNC) terms of the molecular Hamiltonian are presented, including the nuclear anapole term. The formulae giving the PNC contribution to the nuclear magnetic shielding tensor σ, to the indirect spin—spin coupling tensor J and to the spin—rotation tensor C are derived from a perturbation calculation. Some remarks concerning the tensor symmetry are given.
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A.-L. Barra (1996) studied this question.
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