2020
DOI: 10.1088/1361-6501/aba56b
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Comprehensive model and performance optimization of phase-only spatial light modulators

Abstract: Several spurious effects are known to degrade the performance of phase-only spatial light modulators. We introduce a comprehensive model that takes into account the major ones: curvature of the back panel, pixel crosstalk and the internal Fabry–Perot cavity. To estimate the model parameters with high accuracy, we generate blazed grating patterns and acquire the intensity response curves of the first and second diffraction orders. The quantitative model is used to generate compensating holograms, which can prod… Show more

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Cited by 18 publications
(10 citation statements)
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“…Nevertheless, most previous works mainly focused on the compensation of one factor. Recently, Pushkina [54] established a comprehensive model to compensate the effect of pixel cross talk, the back panel curvature (static aberration), and the internal Fabry-Perot cavity simultaneously. As a result, the performance of LC-SLM has been substantially improved.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…Nevertheless, most previous works mainly focused on the compensation of one factor. Recently, Pushkina [54] established a comprehensive model to compensate the effect of pixel cross talk, the back panel curvature (static aberration), and the internal Fabry-Perot cavity simultaneously. As a result, the performance of LC-SLM has been substantially improved.…”
Section: Conclusion and Discussionmentioning
confidence: 99%
“…When computing the hologram, we compensate for the incoming beam's non-uniform profile and the SLM backplane curvature using the procedure described in Ref. [22]. The holograms can be modified further to alter the waist, displacement and orientation of the generated modes.…”
Section: Spatial Light Modulatormentioning
confidence: 99%
“…The heterodyne detector is sensitive only to the component of the field that matches the LO mode, effectively selecting the necessary field projections. Since it is technically easier to prepare HG modes [22,23] than sort them [24][25][26], this approach significantly simplifies the experiment. We acquire heterodyne photocurrents for HG m,n with m and n ranging from 0 to 20.…”
mentioning
confidence: 99%
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“…The heterodyne detector is sensitive only to the component of the field that matches the LO mode, effectively selecting the necessary field projections. Since it is technically easier to prepare HG modes [27,28] than sort them [29][30][31], this approach significantly simplifies the experiment. We acquire heterodyne photocurrents for HG m;n with m and n ranging from 0 to 20.…”
mentioning
confidence: 99%