2007
DOI: 10.1088/1464-4258/9/8/s22
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Design strategies for optimizing holographic optical tweezers set-ups

Abstract: Abstract. We provide a detailed account of the construction of a system of holographic optical tweezers. While a lot of information is available on the design, alignment and calibration of other optical trapping configurations, those based on holography are relatively poorly described. Inclusion of a spatial light modulator in the setup gives rise to particular design trade-offs and constraints, and the system benefits from specific optimization strategies, which we discuss.

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Cited by 64 publications
(48 citation statements)
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“…Multiple optical traps are created by using diffractive optical elements to split and steer the light from a single beam between multiple traps, which can easily become dynamic by using liquid crystal devices, such as SLMs, to display phase-only holograms (Curtis et al 2002). The working principles of HOTs generated from an SLM are illustrated in figure 1g (Martin-Badosa et al 2007). A continuous-wave TEM 00 laser beam is first expanded and then collimated by two lenses.…”
Section: Multiple Trapsmentioning
confidence: 99%
“…Multiple optical traps are created by using diffractive optical elements to split and steer the light from a single beam between multiple traps, which can easily become dynamic by using liquid crystal devices, such as SLMs, to display phase-only holograms (Curtis et al 2002). The working principles of HOTs generated from an SLM are illustrated in figure 1g (Martin-Badosa et al 2007). A continuous-wave TEM 00 laser beam is first expanded and then collimated by two lenses.…”
Section: Multiple Trapsmentioning
confidence: 99%
“…10 Traps were generated and controlled via a LabView programme which was based on the commonly used "superposition of gratings and lenses" (SGL) algorithm.…”
Section: All-optical Manipulation Of Photonic Membranesmentioning
confidence: 99%
“…5), which consists from a hand-made inverted light microscope with Zeiss 100× objective (1.32 NA, oil immersion, Plan-Apochromat), a reflective LCoS-SLM (Holoeye LCR-2500, twisted nematic, 8-bit grayscale signal, pixel size δ = 19 µm) operating in phase-only modulation, and Nd:YAG laser with wavelength λ = 532 nm and 400 mW. Theory and experimental implementation of such systems are studied in [19] and [20], to name a few. The CGH is addressed onto a phase-only SLM that modulates a collimated laser beam.…”
Section: Experimental Implementationmentioning
confidence: 99%
“…Because of such a filtering process the maximum beam output power is about one half of the one corresponding to the input collimated beam. Wavefront distortion φ ab arising from the SLM non-flatness, mainly astigmatism and spherical aberration, was calibrated following the suggestions reported in [20]. The SLM also allows compensating the wavefront aberrations corresponding to the optical setup, see Refs.…”
Section: Experimental Implementationmentioning
confidence: 99%