Elementary particle models with internal degrees of freedom have been investigated within the framework of special relativity and orthodox quantum mechanics. Classical arguments indicate that systems whose extensions are {} their Compton wavelength have spin excitation energies {} their rest mass. The principal aim of this paper is enumeration and classification of particles with rigid internal structure and a useful classification of particle models is by their symmetry groups. In nonrelativistic mechanics this classification shows that there are only the three well-known types of rigid systems that might be labeled by number of degrees of freedom as [0], [2], and [3] and are exemplified by an ideal point, diatomic molecule and rotator, respectively; while of the three types, but one, [3], possesses a spin-{} state of the Pauli-electron type. The corresponding analysis for relativistic mechanics shows there are nine types labeled here [0], [2], [3], [3{'}], [4], [4{'}], [4{''}], [5], and [6], and in addition two one-parameter infinities of types [3f] and [5f] (0≤f≤π). An algorithm exists for obtaining the spin-spectra of rigid structures from their symmetry groups. Of the 9+2∞ types, just three ([4], [5], and [6]) possess spin-{} states of the Dirac-electron type. The apparent rest mass depends upon the internal rotational state of the particle, as is shown by an unrealistic example of a Lagrangian which is an extension of that of the Klein-Gordon particle.
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David Finkelstein (1955) studied this question.