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Table 1

Overview of the properties of the four beam shifts discussed in this paper.

Property Spatial Goos-Hänchen Angular Goos-Hänchen Spatial Imbert-Federov Angular Imbert-Federov
Type of shift Shift of beam of light Angular deviation of beam of light Shift of beam of light Angular deviation of beam of light
Nature of effect Separate shifts for light polarized parallel and perpendicular to plane of incidence Separate shifts for light polarized parallel and perpendicular to plane of incidence Separate shifts for diagonally and antidiagonally polarized light as well as for right-handed and left-handed circularly polarized light Separate shifts for diagonally and antidiagonally polarized light
Plane/direction of occurrence In plane of incidence In plane of incidence Perpendicular to plane of incidence Away from plane of incidence
Origin of shift Variation of Fresnel phases over range of angles of incidence Variation of Fresnel amplitudes over range of angles of incidence Conservation of total angular momentum in direction normal to surface of mirror Conservation of linear momentum in direction perpendicular to plane of incidence
Main dependence on Fresnel equations Phase gradient Amplitude gradient Retardance Diattenuation
Dependence on incident Stokes parameters Q Q Primarily U and V, weakly Q Primarily U, weakly Q
Dependence on f-number of incident beam No Yes No Yes
Typical size A tenth of a wavelength 1–100 μrad, strongly dependent on f-number of incident beam of light Less than a tenth of a wavelength 0.1-10 μrad, strongly dependent on f-number of incident beam of light
Effect in focal plane for incident unpolarized light PSF shifted and broadened with underlying polarization structure, in particular splitting of opposite polarizations (ghost PSF) Basically none PSF broadened (but not shifted) with underlying polarization structure, in particular splitting of opposite polarizations (ghost PSF) Basically none
Important for high-contrast imaging Yes No Yes No

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