Abstract
The Galilei group is combined with two one-dimensional groups, to form a twelve-dimensional extended Galilei group. Irreducible representations of this group depend upon two indicesm, s that can, respectively, be interpreted as the mass and spin of a non-relativistic particle. It turns out that the true irreducible representations of the ordinary Galilei group correspond tom=0, and this explains why these representations have no physical interpretation.
Similar content being viewed by others
References
Bargmann, V. (1954).Annals of Mathematics,59, 1.
Inönü, E. and Wigner, E. P. (1952).Nuovo Cimento,IX, 705.
von Neumann, J. (1931).Mathematische Annalen,104, 570.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Holmaas, O. An extended Galilei group and its application. Int J Theor Phys 4, 223–227 (1971). https://doi.org/10.1007/BF00673800
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF00673800