Abstract

AbstractIn a symmetrical hyperspherical framework, the internal coordinates for the treatment of N‐body systems are conveniently broken up into kinematic invariants and kinematic rotations. Kinematic rotations describe motions that leave unaltered the moments of the inertia of the N‐body system and perform the permutation of particles. This article considers the corresponding expansions of the wave function in terms of hyperspherical harmonics giving explicit examples for the four‐body case, for which the space of kinematic rotations (the “kinetic cube”) is the space SO(3)/V4 and then the related eigenfunctions will provide a basis on such manifold, as well as be symmetrical with respect to the exchange of identical particles (if any). V4 is also denoted as D2. The eigenfunctions are obtained studying the action of projection operators for V4 on Wigner D‐functions. When n of the particles are identical, the exchange symmetry can be obtained using the projection operators for the Sn group. This eigenfunction expansion basis set for kinematic rotations can be also of interest for the mapping of the potential energy surfaces. © 2002 Wiley Periodicals, Inc. Int J Quantum Chem, 2002

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