2002
DOI: 10.1364/jot.69.000441
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Four-ray splitting in optical crystals

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Cited by 5 publications
(5 citation statements)
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“…The second wedge has thickness d 2 (at x = 0) and its optic axis is in the xy plane and forms an angle of 45 • with respect to the first one. It is well known that, when an arbitrarily polarized beam impinges onto the separation surface of two uniaxial crystals with their optic axes arbitrarily oriented, up to four refracted (and four reflected) beams are produced [17][18][19]. Now we will derive the propagation directions and the corresponding amplitudes of the four plane waves that are produced when an arbitrary polarized monochromatic plane wave impinges orthogonally on a DWD.…”
Section: Preliminariesmentioning
confidence: 99%
“…The second wedge has thickness d 2 (at x = 0) and its optic axis is in the xy plane and forms an angle of 45 • with respect to the first one. It is well known that, when an arbitrarily polarized beam impinges onto the separation surface of two uniaxial crystals with their optic axes arbitrarily oriented, up to four refracted (and four reflected) beams are produced [17][18][19]. Now we will derive the propagation directions and the corresponding amplitudes of the four plane waves that are produced when an arbitrary polarized monochromatic plane wave impinges orthogonally on a DWD.…”
Section: Preliminariesmentioning
confidence: 99%
“…Since, within our approximations, both the phases δ 1 and δ 2 are linear functions of the x coordinate, this equation shows that the output field consists of four linearly polarized plane waves [29,30]. Two of these waves have polarizations parallel to that of the input field (first term of the right hand side of equation ( 41)) and propagate along different directions, so that they interfere to produce a fringe pattern in the irradiance profile, with period L x .…”
Section: Totally and Uniformly Polarized Input Beammentioning
confidence: 94%
“…The optic axis of the second wedge is parallel to the bisector of the x and y axes. When a plane wave impinges perpendicularly to the input face of a DWD, the ordinary and extraordinary components of the field propagate through the first wedge and both of them split into two new ordinary and extraordinary components in the second one [29,30]. Two of these components propagate, after the DWD, following the same direction as the incident plane wave but with different phases and orthogonal polarizations.…”
Section: Double-wedge Depolarizermentioning
confidence: 99%
“…If a plane wave impinges perpendicularly to the input face of the DW with arbitrary state of polarization, e.g., linearly polarized with π/4 azimuth, four field components can be identified at the output [80,[131][132][133][134]: two plane waves propagating along the same direction as the incident wave but with different phases and orthogonal polarization, and two plane waves, also having mutually orthogonal polarization, that propagate along slightly tilted directions. The effect of the superposition of such waves is a modulation of the state of polarization of the field across the exit plane of the device.…”
Section: Double Wedgementioning
confidence: 99%