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The reader should be aware that the domain of applicability of this theorem might, in spite of its declared hypothesis, not cover the case of Hamiltonians including long-range interactions at collective states such as the so-called QSS (quasi-stationary state). The 20 March 2006, in a telephone conversation with Prof. Werner Braun (while he was in Texas, and myself at the Santa Fe Institute, New Mexico), he shared with me [nearly literal transcription]: "We were thinking of a potential that has no singularities at the origin and elsewhere, and that decays sufficiently quickly at infinity... In this case we are sure that we are allowed to do all the derivatives and integrals that we do in the paper... Although I cannot be sure after so many years, my guess would be that our arguments are NOT valid if (< d. In such a case, I would guess that strange structures could be present in phase space... I am not sure about all this, but this would be my guess. This conversation followed
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