The ground-state energy and the singlet-triplet energy gap of the antiferromagnetic Heisenberg model on a ladder is investigated using a mean-field theory and the density-matrix renormalization group. Spin-wave theory shows that the corrections to the local magnetization are infinite. This indicates that no long-range order occurs in this system. A flux-phase state is used to calculate the energy gap as a function of the transverse coupling, J_⊥, in the ladder. It is found that the gap is linear in J_⊥ for J_⊥{}1 and goes to zero for J_⊥{→}0. The mean-field theory agrees well with the numerical results.
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Azzouz et al. (1994) studied this question.
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