2013
DOI: 10.1364/oe.21.024837
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Precise shaping of laser light by an acousto-optic deflector

Abstract: We present a laser beam shaping method using acousto-optic deflection of light and discuss its application to dipole trapping of ultracold atoms. By driving the acousto-optic deflector with multiple frequencies, we generate an array of overlapping diffraction-limited beams that combine to form an arbitrary-shaped smooth and continuous trapping potential. Confinement of atoms in a flat-bottomed potential formed by a laser beam with uniform intensity over its central region confers numerous advantages over the h… Show more

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Cited by 52 publications
(38 citation statements)
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“…Experiments have been performed with discrete arrays of optical dipole traps, loaded with either thermal atoms [4,5] or quantum degenerate atomic gases [3,6,7], in which individual trapping sites can be moved, addressed and manipulated. Important too are continuous trapping geometries: the primary subject of the present work are extended (as opposed to diffractionlimited) power-law potentials, proposed both as a static supplement to a trapping potential to cancel unwanted external potentials [8], and in a dynamic sequence as a tool for the efficient production of Bose-Einstein condensates [9]. Other interesting continuous potentials include engineered waveguides with dynamic bright regions, shown to be suitable for studies of BEC superfluidity [10].…”
Section: Introductionmentioning
confidence: 99%
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“…Experiments have been performed with discrete arrays of optical dipole traps, loaded with either thermal atoms [4,5] or quantum degenerate atomic gases [3,6,7], in which individual trapping sites can be moved, addressed and manipulated. Important too are continuous trapping geometries: the primary subject of the present work are extended (as opposed to diffractionlimited) power-law potentials, proposed both as a static supplement to a trapping potential to cancel unwanted external potentials [8], and in a dynamic sequence as a tool for the efficient production of Bose-Einstein condensates [9]. Other interesting continuous potentials include engineered waveguides with dynamic bright regions, shown to be suitable for studies of BEC superfluidity [10].…”
Section: Introductionmentioning
confidence: 99%
“…Technologies employed so far in the realisation of these arbitrary optical trapping patterns include acousto-optic deflection of a laser beam to produce either a composite static intensity distribution [8] or a rapidly-scanned profile [3,7,11], digital micro-mirror devices (DMDs) [4], and computer-generated holograms implemented with phase-only spatial light modulators (SLMs) [5,6,9,10,[12][13][14][15]. The high phase-resolution available in phase-only SLMs offers significant advantages for versatility of the accessible trapping patterns, though at the cost of lower switching speed between frames if compared to acousto-optic modulators and digital mirror devices.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the mass range for LA-MS is limited between masses similar to the coolant ion-as low as 2 Da for LA-MS[Be + ] [41]-up to ∼ 10 3 Da. This includes volatile organic compounds, the amino acids, explosive agents, and some peptides; modifications may extend the mass range to include heavier biomolecules such as nucleic acids [38,42].…”
Section: Discussionmentioning
confidence: 99%
“…LCoS-SLM is based on the individual manipulation of the refractive index of pixels of a liquid crystal display, while acousto-optic beam shaping (AOS) is based on a fast variation of an acoustic wave enabling a spatially dependent phase variation of laser beams. The AOS technology enables wavefront shaping [11] particularly for 3D nonlinear microscopy [12] and intensity profile shaping [13].…”
Section: Introductionmentioning
confidence: 99%