“…Spin-dependent effects on the propagation of wave packets and particles have been widely studied in general relativity using different methods, such as WKBtype approximations [25-28, 30, 32, 34, 35, 49-55], the Mathisson-Papapetrou equations for spinning objects [27,[56][57][58][59][60], approximation methods inspired from quantum mechanics [29,31,33] and others [61,62] (see also [63][64][65][66][67][68][69]). Furthermore, gravitational spin Hall effects are predicted for different fields propagating in curved spacetime, such as electromagnetic [26][27][28][29], linearized gravitational [30,31] and massive and massless Dirac fields [32,34,35] (spin Hall effects have also been predicted for more exotic particles such as massless particles with anyonic spin [70][71][72][73]).…”