1998
DOI: 10.1080/095003498151357
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The production of multiringed Laguerre-Gaussian modes by computer-generated holograms

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Cited by 75 publications
(84 citation statements)
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“…This was soon followed by the demonstration of a spiral phase plate (SPP) operating at optical wavelength [12] and at milimeter range [13] for creating helical-wavefront to directly transform Gaussian beam to OAM beams. At the same time, computer-generated holograms with pitchfork structures were applied using a spatial light modulator (SLM) to convert Gaussian beams into LG beams [3,14]. Different from the astigmatic mode converter, both SPP and SLM are not pure mode converters.…”
Section: Introductionmentioning
confidence: 99%
“…This was soon followed by the demonstration of a spiral phase plate (SPP) operating at optical wavelength [12] and at milimeter range [13] for creating helical-wavefront to directly transform Gaussian beam to OAM beams. At the same time, computer-generated holograms with pitchfork structures were applied using a spatial light modulator (SLM) to convert Gaussian beams into LG beams [3,14]. Different from the astigmatic mode converter, both SPP and SLM are not pure mode converters.…”
Section: Introductionmentioning
confidence: 99%
“…Many techniques are presently available to generate a higher-order LG p mode from a laser emitting an LG 0 0 beam. Cylindrical mode converters [19] can transform higher-order Hermite-Gauss beams [9] into higher-order LG p beams, using astigmatic lenses; spiral phase plates [20] are optics whose varying thickness induce the typical LG p spiralling phase pattern into the input beam; diffractive optics, which include computer generated holograms [21], spatial light modulators [22] and etched-glass diffractive optics [23] can modulate the amplitude and the phase of the incoming beam to obtain a higher-order LG p mode.…”
mentioning
confidence: 99%
“…The simplest way to generate a Laguerre-Gaussian donut mode (i.e., LG l p=0 ) is to apply an additional phase wrap to the hologram Φ LG = mφ , where φ is the polar angle on the SLM and m = ±l is an integer denoting the azimuthal index 19,20 . This approach, however, does not produce a pure LG donut mode, rather it generates a superposition of higher-order radial p modes for a given azimuthal mode l. The result is a series of concentric, annular rings, albeit with the majority of the power in the p = 0 mode.…”
Section: Wavefront Engineeringmentioning
confidence: 99%