We establish a basis set of atomic orbitals suitable to describe molecular wave functions at arbitrary magnetic field strengths and for an arbitrary orientation of the molecule relative to the magnetic field. A simple calculation for the hydrogen atom demonstrates the superiority of such an orbital over common orbitals. All types of matrix elements of the Hamiltonian of a molecule in a strong magnetic field are evaluated within our basis set of atomic orbitals.
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Schmelcher et al. (1988) studied this question.
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