Abstract
We study lattice hamiltonians with continuous local SU(2) gauge invariance, for which the Hilbert space on each link is finite dimensional. As these are gauge-invariant generalizations of quantum magnets, we call them lattice gauge magnets. The generators of gauge transformations are built out of local spin operators. In the simplest version of such a theory, the gauge field components belong to a representation of the algebra SO(5). Long-wavelength excitations of this model are gapless and nonrelativistic at the tree level. In 2 + 1 dimensions, we study a parity violating model, which we argue is equivalent to the topologically massive Yang-Mills theory.
Original language | English |
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Pages (from-to) | 647-672 |
Number of pages | 26 |
Journal | Nuclear Physics B |
Volume | 338 |
Issue number | 3 |
DOIs | |
State | Published - 16 Jul 1990 |
Externally published | Yes |
ASJC Scopus subject areas
- Nuclear and High Energy Physics