Abstract
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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