Abstract
When we study complicated quantum physical systems, we divide them into their parts and study these parts separately. The parts can be constituents, but the parts can also be other subsystems, like certain collective motions (e.g. rotations about the center of mass). In either case the space of physical states of the subsystem is a factor space of the tensor product space for the whole system. One can then study the structure of the subsystem for each definite state of the remainder of the whole system.
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© 1989 Plenum Press, New York
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Bohm, A. (1989). Berry’s Connection, the Charge-Monopole System and the Group Theory of the Diatomic Molecule. In: Gruber, B., Iachello, F. (eds) Symmetries in Science III. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0787-7_4
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DOI: https://doi.org/10.1007/978-1-4613-0787-7_4
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