Exact sum rules are obtained for the nearest-neighbor Heisenberg antiferromagnet and $X Y$ ferromagnet in one dimension. In the Heisenberg case the sum rules may be used to show that most of the spectral weight of the spin correlation function at small k and $T=0$ is concentrated near the frequency of the "des Cloizeaux-Pearson" states. In the $X Y$ case, the corresponding "Schultz-Lieb-Mattis" states only carry a negligible portion of the weight at small k.
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Hohenberg et al. (1974) studied this question.
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