“…The equations of motion for spinning pole-dipole particles were first derived by Mathisson [1] in the context of general relativity, though similar equations, for the case of flat spacetime, had been derived earlier by Frenkel [2] (see also [3]) in a special relativistic treatment applying to a classical model of an electron. These equations have then been further worked out and rederived most notably by Weyssenhoff-Raabe [4,5], Möller [6], Bhabha-Corben [7][8][9], Dixon [10] and Gralla et al [11], in the framework of special relativity; and in general relativity by Papapetrou [12], who carried out an exact derivation for pole-dipole particles, Tulczyjew [13], Taub [14], Dixon [15,16] and Souriau [17,18], who made derivations covariant at each step, and more recently Natário [19] and Gralla et al [20].…”