Abstract

We derive a continuum field theory for the Majumdar-Ghosh model in the large-SS limit, where the field takes values in the manifold of the SO(3)SO(3) group. No topological term is induced in the action and the cases for integer spin and half-integer spin appear to be indistinguishable. A one-loop β\beta -function calculation indicates that the theory flows towards a strong coupling (disordered) phase at long distances. This is verified in the large-NN limit, where all excitations are shown to be massive. (Three figures not included)Comment: 27 pages, plain.tex, TIFR-TH-92-5

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