Abstract
We review higher-order spectral sum rules in scattering theory for d ≤ 3 dimensions. These rules generalize the well-known Levinson theorem [1] for partial-wave scattering, relating the number of bound states with the value of the scattering phase shift at the threshold energy zero, and they are valid for non-spherically symmetric short-range interactions. They involve the scattering matrix, the bound-state wave functions and some correction terms arising from the high-energy behavior of the scattering problem. These correction terms are shown to be d-dimensional generalizations of the polynomial conserved densities of the Korteweg-de Vries equation [2], [3]. The modifications of these rules necessary to allow Coulomb-type interactions are presented.
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Bollé, D. (1987). Higher-Order Levinson Theorems and the Planck-Larkin Partition Function for Reacting Plasmas. In: Rogers, F.J., Dewitt, H.E. (eds) Strongly Coupled Plasma Physics. NATO ASI Series, vol 154. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-1891-0_21
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DOI: https://doi.org/10.1007/978-1-4613-1891-0_21
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