“…That is, the resulting Hamiltonian is very compact with a partitioned structure, and has a common formulation except for the mass-dependent prefactors regardless of types of orthogonal vectors [11,13,25,34,36,49,[66][67][68]. Otherwise, if non-orthogonal coordinates [25, [69][70][71][72][73][74][75][76] are used, the kinetic energy operators obtained are rather complicated. The complicated Hamiltonian will make calculations difficult, especially for polyatomic molecules, although the basis size can be somewhat reduced for rigid or semi-rigid molecules.…”