2008
DOI: 10.1364/oe.16.019807
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Finite-energy, accelerating Bessel pulses

Abstract: Abstract:We numerically investigate the possibility to generate freely accelerating or decelerating pulses. In particular it is shown that acceleration along the propagation direction z may be obtained by a purely spatial modulation of an input Gaussian pulse in the form of finite-energy Bessel pulses with a cone angle that varies along the radial coordinate. We discuss simple practical implementations of such accelerating Bessel beams.

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Cited by 40 publications
(24 citation statements)
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“…More recently, a type of laterally accelerating localized wave called an Airy beam (or pulse, if generated using ultrashort pulses), has attracted attention [9][10][11]. Pulses can also accelerate due to diffraction, spherical aberration in lenses, and appropriately shaped nonlinear profiles of axicons [12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…More recently, a type of laterally accelerating localized wave called an Airy beam (or pulse, if generated using ultrashort pulses), has attracted attention [9][10][11]. Pulses can also accelerate due to diffraction, spherical aberration in lenses, and appropriately shaped nonlinear profiles of axicons [12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we report spatiotemporal measurements of accelerating and decelerating Bessel pulses. The term was proposed in [15] where generation and properties of such pulses have been theoretically investigated. These pulses are similar to the localized waves known as Bessel-X pulses [2,3,[6][7][8], with the main difference being that they are generated by crossing and interfering focusing pulses that have curved pulse fronts and form part of a spindle torus surface, rather than the double conical surface that is present in Bessel-X pulses.…”
Section: Introductionmentioning
confidence: 99%
“…Also similar to the Bessel-X pulse the boundary wave pulse has a letter X-like axial cross-section and propagates on the optical axis superluminally. But while the group velocity of the former has a constant value exceeding c, the central spot of the boundary wave pulse is decelerating (see also [1,[9][10][11]). The elementary boundary diffraction waves emanating from the edges of the aperture must travel a longer distance to reach the optical axis compared to the centre of the direct pulse and thus lag behind.…”
Section: Discussionmentioning
confidence: 99%
“…The Airy beam solution has been the most extensively studied to date (see [1] for a review), while accelerating parabolic beams [2], Bessel pulses [3], and Airy-Bessel pulses [4] have also attracted recent interest. In addition, by interfering two light fields of different frequencies, a traveling intensity modulation component can be created [5].…”
Section: Introductionmentioning
confidence: 99%