Two methodological troubles of the quantum theory of collisions are considered. The first is the undesirable interference of the incident and scattered waves in the stationary approach to scattering. The second concerns the nonstationary approach to the theory of collisions of the type a + b c + d. In order to calculate the cross section one uses the matrix element <cd|S|ab> of the S matrix. The element is proportional to d function expressing the energy conservation. The corresponding probability |<cd|S|ab>|² contains d² which is mathematically senseless. The known regular way to overcome the difficulty seems to be unsatisfactory. In this paper, both the troubles are resolved using wave packets of incident particles.

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