The existence of a spin gap is studied in a generalization of the one-dimensional t-J model. A frustrated next-nearest- neighbor exchange interaction, J', gives rise to a spin gap at half-filling that survives for small doping and arbitrary values of J. Regions of phase separation and divergent superconducting fluctuations are distorted but still present in the extended model.
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Ogata et al. (1991) studied this question.
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