2017
DOI: 10.1016/j.optcom.2016.08.050
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Engineering an achromatic Bessel beam using a phase-only spatial light modulator and an iterative Fourier transformation algorithm

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Cited by 14 publications
(7 citation statements)
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“…In addition, the transverse intensity profile of the twisted beams exhibits a ringlike pattern with a dark spot (vortex) at the center [20]. In experiments, twisted (Bessel) beams can nowadays be readily produced by means of * anton.peshkov@uni-jena.de spatial light modulators [21] or axicons [22][23][24]. During recent years a number of studies have shown that the OAM and the intensity profile of these twisted beams may affect different fundamental light-matter interaction processes such as the Compton scattering [25][26][27], photoexcitation [28][29][30][31][32][33] and photoionization [34,35] of atoms, the generation of electric currents in quantum rings [36] and molecules [37], electromagnetically induced transparency [38], four-wave mixing in atomic vapors [39].…”
Section: Introductionmentioning
confidence: 99%
“…In addition, the transverse intensity profile of the twisted beams exhibits a ringlike pattern with a dark spot (vortex) at the center [20]. In experiments, twisted (Bessel) beams can nowadays be readily produced by means of * anton.peshkov@uni-jena.de spatial light modulators [21] or axicons [22][23][24]. During recent years a number of studies have shown that the OAM and the intensity profile of these twisted beams may affect different fundamental light-matter interaction processes such as the Compton scattering [25][26][27], photoexcitation [28][29][30][31][32][33] and photoionization [34,35] of atoms, the generation of electric currents in quantum rings [36] and molecules [37], electromagnetically induced transparency [38], four-wave mixing in atomic vapors [39].…”
Section: Introductionmentioning
confidence: 99%
“…The non-interferometric phase readout method based on iterative Fourier transform (IFT) algorithm is an iterative single operation method [38][39][40] , which is proposed by R. W. Gerchberg and W. O. Saxton in 1970s and modified by James R. Fienup in 1980s. Until now, the IFT algorithm and its derivative algorithms have large amount of applications such as digital encryption, image resolution enhancement, wavefront shaping and so on [41][42][43][44] . Generally, the reconstruction of relative faithful phase information require hundreds of iterations, which casting a heavy burden on computation time and reducing the data transfer rate eventually.…”
Section: Phase-modulated Chdssmentioning
confidence: 99%
“…This is of particular importance for applications requiring deep tissue imaging, since high laser powers are needed to reach deep into the samples. Future efforts could adopt a Fourier plane setup, in which iterative Fourier transform algorithms [25] can be implemented to generate the desired annuli. Still, the generated beams using the simple diverting setup were sufficient in investigating the hypothesis experimentally.…”
Section: Imaging Tissue Phantomsmentioning
confidence: 99%