We study the weakly frustrated two-dimensional antiferromagnetic Heisenberg model with first- (J₁), second- (J₂), and third-neighbor (J₃) exchanges. In the limit of low frequencies and long wavelengths the effective action is identified as the O(3) nonlinear {σ} model with an additional Berry phase. Use of renormalization-group methods allows us to estimate the stability of the N\'eel phase for the square and honeycomb lattices. For the spin-1/2 square lattice an analysis at the one-loop level suggests an upper bound for the disordering transition at (J₂+2J₃)/J₁=0.22±{}0.04, substantially below the estimate from O(1/S) spin-wave theory. Our analysis further indicates that the spin-1/2 disordered ground state is degenerate at weak frustration, with a fourfold degeneracy for the square lattice and a threefold degeneracy for the honeycomb lattice.
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Einarsson et al. (1991) studied this question.
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