2004
DOI: 10.1117/12.559859
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Simplified optimum phase-only configuration for a TNLCD

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Cited by 3 publications
(2 citation statements)
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“…We implemented experimentally CGHs that encode Bessel and Laguerre-Gauss beams. In this task we employed a twisted nematic liquid crystal device as a phasemostly SLM employing a linear polarizer followed by a quarter wave plate at the input, and a second linear polarizer at the output [9]. The phase modulation depth obtained when a He-Ne laser {/i=633 nm) is employed as illuminating source was =1.2?!.…”
Section: (18) the Fourier Spectrum Function Hi(u-uov-vq) Which Apmentioning
confidence: 99%
“…We implemented experimentally CGHs that encode Bessel and Laguerre-Gauss beams. In this task we employed a twisted nematic liquid crystal device as a phasemostly SLM employing a linear polarizer followed by a quarter wave plate at the input, and a second linear polarizer at the output [9]. The phase modulation depth obtained when a He-Ne laser {/i=633 nm) is employed as illuminating source was =1.2?!.…”
Section: (18) the Fourier Spectrum Function Hi(u-uov-vq) Which Apmentioning
confidence: 99%
“…The twisted angle and the birefringence of a TNLC are two main parameters that control the modulation. There are several proposed methods and configurations to find these parameters to introduce the Jones matrix of TNLC [22][23][24][25][26]. On the contrary, Martín-Badosa et al proposed a method to characterize liquid crystal displays (LCDs) based on the fringe analysis obtained by a Mach-Zehnder interferometer configuration, without the necessity of finding the physical properties of LCD [27].…”
Section: Introductionmentioning
confidence: 99%