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We compute the Gaussian-fluctuation corrections to the saddle-point Schwinger-boson results using collective coordinate methods. Concrete application to investigate the frustrated J₁-J₂ antiferromagnet on the square lattice shows that, unlike the saddle-point predictions, there is a quantum nonmagnetic phase for 0.53J₂/J₁0.64. This result is obtained by considering the corrections to the spin stiffness on large lattices and extrapolating to the thermodynamic limit, which avoids the infinite-lattice infrared divergencies associated with Bose condensation. The very good agreement of our results with exact numerical values on finite clusters lends support to the calculational scheme employed.
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Trumper et al. (1997) studied this question.
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