“…In the first case, polarization transformations in the system [7][8][9][10][11][12] are represented as points on the Poincaré sphere, forming a contour of polarization changes (opened or closed), and the geometric phase is determined by the relative position of these points, in particular, by the surface area bounded by the contour 2,5 . In another group of methods, the geometric (as well as the dynamic) phase leads to a shift of interference peaks, and numerically can be obtained by the magnitude of this shift 4-6. The dynamic and geometric phase constitute the total phase of the beam, which manifests itself in interference [7][8][9]12 . In some interference methods, two orthogonal states of linear input polarization are used to determine the geometric phase 4 .…”