2016
DOI: 10.1515/aot-2016-0030
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Exploring the unlimited possibilities of modular aspheric Gauss to top-hat beam shaping

Abstract: Beam shaping is a field of research with growing importance. Therefore, a new refractive beam shaping system is presented. The knowledge gained from analyzing patent systems was used to derive our own improved design. It is compared to a patent system, and some selected results are presented in this work. Furthermore, possibilities to scale the entrance and exit beam diameters with the help of SPA™ Beam Expander Kit and SPA™ AspheriColl (both from asphericon GmbH, Jena, Germany) are shown, so that a modular to… Show more

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Cited by 15 publications
(7 citation statements)
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“…There are three main strategies to achieve uniform illumination. One is based on a beamshaper. However, this device is expensive, and its wavelength dependence makes the method unsuitable for multicolor imaging. The second strategy is based on the method of Kohler illumination, using a diffuser and a pair of microlens arrays to achieve a uniform distribution of light in the focal plane of the objective. , This method requires a complex optical design and is thus difficult to adopt in common laboratories.…”
Section: Resultsmentioning
confidence: 99%
“…There are three main strategies to achieve uniform illumination. One is based on a beamshaper. However, this device is expensive, and its wavelength dependence makes the method unsuitable for multicolor imaging. The second strategy is based on the method of Kohler illumination, using a diffuser and a pair of microlens arrays to achieve a uniform distribution of light in the focal plane of the objective. , This method requires a complex optical design and is thus difficult to adopt in common laboratories.…”
Section: Resultsmentioning
confidence: 99%
“…Two laser sources (06-MLD 638 nm and 06-DPL 561 nm, Cobolt) were combined, split into two fiber couplers and delivered to the microscope. One output beam from a single-mode fiber (P5-630PM-FC-2, Thorlabs) was collimated with an achromatic lens (L1, f = 63.5 mm, #49-780, Edmund Optics) and sent to the beam shaper (TopShape, asphericon GmbH) where the input size was ~10 mm (1/e 2 ), but it is generally acceptable in a range between 9.2 mm and 10.8 mm 26 . Two mirrors (M1 and M2) served as four extra degrees of freedom to guide the beam into the TopShape.…”
Section: Methodsmentioning
confidence: 99%
“…Since the beam-shaping element (TopShape) is based on refraction, which causes a smooth redistribution of the beam intensity, the flat-top beam profile simulations can be performed using methods based on geometrical optics 26 . Here, the beam profile was calculated at a certain distance behind the beam shaping system before entering the microscope.…”
Section: Simulated Beam Intensity Distributionmentioning
confidence: 99%
“…The zoomed-in top view clearly shows the precision of the pulse selection as well as the high signal-to-noise ratio (SNR) of this demonstration in the central part of the pulse train. Indeed, the peripheral positions of the pulse train have a lower SNR than its central part, but this problem could be circumvented by using an appropriate shaping of the pump beam in square shape and top hat intensity [44].…”
Section: Parallel Modulation and Codingmentioning
confidence: 99%