2018
DOI: 10.1088/1555-6611/aaada7
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Generation and propagation characteristics of a localized hollow beam

Abstract: A succinct experimental scheme is demonstrated to generate a localized hollow beam by using a π-phase binary bitmap and a convergent thin lens. The experimental results show that the aspect ratio of the dark-spot size of the hollow beam can be effectively controlled by the focal length of the lens. The measured beam profiles in free space also agree with the theoretical modeling. The studies hold great promise that such a hollow beam can be used to cool trapped atoms (or molecules) by Sisyphus cooling and to a… Show more

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Cited by 3 publications
(5 citation statements)
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“…In recent research, a localized hollow beam by using a π-phase binary bitmap and a convergent thin lens was demonstrated experimentally. The measured beam profiles in free space agree well with the theoretical modeling from the light diffraction theory [34]. So, we compare the simulation results of the optical intensity distribution of the FHB with ones derived from the light diffraction theory, and study the influence of the discrete and continuous phases of the grating on the intensity distribution of the modulated optical field.…”
Section: Influences Of Both Discrete and Continuous Phases Of The Gra...supporting
confidence: 70%
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“…In recent research, a localized hollow beam by using a π-phase binary bitmap and a convergent thin lens was demonstrated experimentally. The measured beam profiles in free space agree well with the theoretical modeling from the light diffraction theory [34]. So, we compare the simulation results of the optical intensity distribution of the FHB with ones derived from the light diffraction theory, and study the influence of the discrete and continuous phases of the grating on the intensity distribution of the modulated optical field.…”
Section: Influences Of Both Discrete and Continuous Phases Of The Gra...supporting
confidence: 70%
“…The number of the phase-shifting rings is enough, so that the phase distribution of the grating is continuous. According to the light diffraction theory, the normalized amplitude distribution near the focal plane of the metasurface grating can be defined as [34,35], Here, ρ and u are the simplified radial and axial coordinates in the transmission region, respectively, r is the radial coordinate of pupil plane of figure 2(c), f j defines the phase of zone j ( = j 1, 2) on the pupil plane and r j is the radial position of each zone. The amplitude distribution of the incident laser beam is given by g r .…”
Section: Influences Of Both Discrete and Continuous Phases Of The Gra...mentioning
confidence: 99%
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“…The exact arithmetic solution of LHB laser intensity profile is presented in [40], and the approximate analytic solution used in the simulation is ( ) e x p 2 , 0 2 2 0 2 2 where r and a are radial component and axial component, respectively, R is the ratio of the long axis to the short axis, r 0 is the radial size of LHB, w is the full width at half maximum of a single peak of radial intensity distribution at = a 0 plane. The total scattering rate P sp can be obtained, i.e.…”
Section: Dressed States and Spontaneous Transitionmentioning
confidence: 99%
“…Sub-Doppler cooling, which can be generally understood from spatially varying polarization gradients in type-I systems, such as Sisyphus (p p - The scheme to trap and cool MgF molecules using a LHB and a weak RPB is shown in figure 1. The LHB is succinctly generated by a collimated Gaussian laser beam (GLB) and a spatial light modulator (SLM) [40]. There is a non-light area at the center of the generated LHB, which is dark spot (DS).…”
Section: Introductionmentioning
confidence: 99%