Introduction to the Lie-admissible treatment of non-potential interactions in Newtonian, statistical, and particle mechanics

Views on the experimental origin, theoretical formulation, and mathematical structure of nonpotential interactions in Newtonian, statistical, and particle mechanics are presented. The simplest but most dominant consideration of this introduction is the expectation that the charge distribution of hadrons is not perfectly rigid, but admits deformations under suitable impacts with other hadrons. These rather natural deformations then imply: (1) the breaking of the SU(2)-spin symmetry for the interior strong problem, with the understanding that conventional, conserved, total spin quantities are recovered in the exterior treatment; (2) the consequential necessary breaking of the T- and P-symmetries, also for the interior strong problem, owing to the explicit dependence of the discrete operators on spin, with the understanding that the center-of-mass trajectories of closed strong systems recover the T- and P-symmetries; and (3) the origin of irreversibility at the most elemental level of nature, via the nonpotential interactions originating from mutual penetrations and overlappings of hadrons under strong interactions