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, it does not imply that the necessary conditions of relativistic locality, locality of all interactions, particle spin (Weyl) statistics, CPT invariance are satisfied. The states belonging to this category are unphysical. Moreover, such states violate causality and lead to negative probabilities. The second category corresponds to the states that are described by the Jost solutions. The dynamics of these states in the non-relativistic framework is local, so that the notion of non-locality arises only in the relativistic framework. Therefore, in the non-relativistic framework we can talk about the non-locality of the states belonging to this category. It is shown in [@BoPi:07] that the results of this paper are valid for any initial states in the second category. The first category is the extension of these results to the non-relativistic case. [10]{} J. Aharonov, D. Bohm, Phys. Rev. [**115**]{}, 485 (1959) D. Bohm, Phys. Rev. [**85**]{}, 166, 180 (1952) D. Bohm, B. J. Hiley, Phys. Rev. Lett. [**54**]{}, 1690 (1985) D. Bohm, B. J. Hiley, Phys. Lett. A [**160**]{}, 316 (1991) Y. Aharonov, D. Bohm, Phys. Rev. [**122**]{}, 1649 (1961) Y. Aharonov, S. Popescu, D. Rohrlich, Lett. Math. Phys. [**24**]{},299 (1992) Y. Aharonov, D. Rohrlich, [*Lectures on Quantum Theory*]{} (World Scientific Publishing Company, Singapore, 1993) J. M. Jauch, F. Rohrlich, [*The Theory of Photons and Electrons*]{} (Springer-Verlag, Berlin, 1976) S. Goldstein, [*The Equivalence Principle*]{}, (Springer-Verlag, Berlin, 2001) R. G
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