“…5). When such a particle is located on the optical axis with its long axis lying in the focal plane, it is rotated around the center of mass and around the optical axis by the orbital energy flow P o,φ (21) or, in other words, by the longitudinal OAM component L z (24), similarly to rotation of particles along a circular trajectory in [11,26]. Since the effective refractive indices of an ellipsoidaltype particle differ for orthogonal polarizations directed along the long and short axes of the quasi-ellipse (birefringence), it is also rotated around the center of mass by the longitudinal SAM component S z (22) or, in other words, by the azimuthal spin flow P s,φ (16), similarly to rotation of crystalline birefringent particles in [38].…”