Photonics 2015
DOI: 10.1002/9781119009719.ch3
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Light Beams with Spatially Variable Polarization

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Cited by 30 publications
(31 citation statements)
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“…Beyond that, spatial modulation of polarization states becomes more and more important (see sections 7 and8) [59]. While primarily interferometric methods and so-called q-plates allow thegeneration of radially and azimuthally polarized beams, liquid crystal SLMs havepioneered therealization of extended Poincaré beams.…”
Section: Statusmentioning
confidence: 99%
“…Beyond that, spatial modulation of polarization states becomes more and more important (see sections 7 and8) [59]. While primarily interferometric methods and so-called q-plates allow thegeneration of radially and azimuthally polarized beams, liquid crystal SLMs havepioneered therealization of extended Poincaré beams.…”
Section: Statusmentioning
confidence: 99%
“…Several methods have been proposed and carried out to experimentally synthesize different types of NUP beams. They use Mach-Zehnder interferometers (MZIs), fiber lasers running in either CW or pulsed mode, digital lasers, spatial light modulators (SLMs), metasurfaces, stressed optical windows, q-plates, spiral phase plates, photoaligned liquid crystals, digital micromirrors, and more (see, e.g., [6,23,25,28,33,46,52,57,61,66,69,[92][93][94][95]). In this tutorial, we will describe some techniques to generate NUTP beams that could be implemented with conventional optical systems and do not require sophisticated optical equipment, such as SLMs, or complex configurations, such as modifications of a laser cavity, and so on.…”
Section: Synthesizing Nutp Beamsmentioning
confidence: 99%
“…Polarization of light is an exciting subject, and numerous books and research articles have been devoted to understanding and modeling this characteristic of light, even in very recent times [1][2][3][4][5][6][7][8][9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…Spin-orbit beams are beams embedded with polarization singularities 3 6 and can be described as a superposition of orthogonal OAM states in orthogonal spin angular momentum (SAM) states. In recent years, beams with single polarization singularity at the center of the beam are called by special names such as Poincaré beams 7 , cylindrical vector beams 8 , vector vortex beams 9 , Majorana beams 10 . Here, we deal with higher order Poincaré sphere (HOPS) beams 11 13 and hybrid order Poincaré sphere beams (HyOPS) 14 17 that contain a polarization singularity at the center of the beam and only two dimensional field distributions are considered.…”
Section: Introductionmentioning
confidence: 99%