A recent paper established technical conditions for the construction of a class of induced representations of the nonrelativistic current group SΛK, where S is Schwartz’s space of rapidly decreasing C∞ functions, and K is a group of C∞ diffeomorphisms of Rs. Bose and Fermi N‐particle systems were recovered as unitarily inequivalent induced representations of the group by lifting the action of K on an orbit Δ⊆S′ to its universal covering space δ. For s⩾3, δ is the coordinate space for N particles, which is simply connected. In two‐dimensional space, however, the coordinate space is multiply connected, implying induced representations other than those describing the usual Bose or Fermi statistics; these are explored in the present paper. Likewise the Aharonov–Bohm effect is described by means of induced representations of the local observables, defined in a nonsimply connected region of Rs. The vector potential plays no role in this description of the Aharonov–Bohm effect.
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