2020
DOI: 10.1364/oe.387866
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Experimental observation of three-dimensional non-paraxial accelerating beams

Abstract: We experimentally realize three-dimensional non-paraxial accelerating beams associated with different coordinate systems. They are obtained by Fourier transforming a phase-modulated wave front in an aberration-compensated system. The phase pattern is encoded to include the phase and amplitude modulation for the accelerating beams with additional correction phase for the aberration compensation. These beams propagate along a circular trajectory, but they exhibit rather complex intensity patterns corresponding t… Show more

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Cited by 7 publications
(6 citation statements)
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“…Additionally, the self-bending feature would create an artifact near the edge of the scan region, and this issue could be solved using a more advanced azimuthally self-accelerating beam [110,111]. The non-paraxial self-accelerating beam with a larger bending angle would allow better axial resolution in the MPM [18]. The incoherent accelerating beams beyond the paraxial regime would improve the SNR [157].…”
Section: Axial Resolution In Two-photon Microscopy With Self-accelerating Beamsmentioning
confidence: 99%
See 1 more Smart Citation
“…Additionally, the self-bending feature would create an artifact near the edge of the scan region, and this issue could be solved using a more advanced azimuthally self-accelerating beam [110,111]. The non-paraxial self-accelerating beam with a larger bending angle would allow better axial resolution in the MPM [18]. The incoherent accelerating beams beyond the paraxial regime would improve the SNR [157].…”
Section: Axial Resolution In Two-photon Microscopy With Self-accelerating Beamsmentioning
confidence: 99%
“…The study on self-accelerating Airy beam has excited a series of researches on the non-diffracting accelerating wave packets predicted by the Maxwell equation [17,18]. Some examples include the linear and nonlinear generation of non-paraxial accelerating beams [19], non-paraxial Webber beams [20], and full vectorial accelerating diffraction-free Helmholtz beams [21,22].…”
Section: Introductionmentioning
confidence: 99%
“…j and, Σ is given by ϑ ä [0, π] and j ä [−π/2, π/2], where ( )  J is given in terms of spherical harmonic functions [33], parabolic, oblate, and prolate spheroidal functions [34,35], and the angular spectrum determined by the nondiffracting Mathieu and parabolic beams [36], respectively. It is important to comment that, in reference [33] the associated caustic of these three-dimensional accelerating beams was obtained, as the turning points of an effective potential, which appears when the separation of variables method is applied to the Helmholtz equation.…”
Section: Introductionmentioning
confidence: 99%
“…[ 13–15 ] In addition to Airy beams, other accelerating beams following any arbitrary trajectories have been demonstrated. [ 16–19 ] Furthermore, by means of the caustic approach, researchers have experimentally generated nonparaxial accelerating beams with arbitrary trajectories in a more effective and flexible strategy. [ 20–22 ]…”
Section: Introductionmentioning
confidence: 99%
“…[13][14][15] In addition to Airy beams, other accelerating beams following any arbitrary trajectories have been demonstrated. [16][17][18][19] Furthermore, by means of the caustic approach, researchers have experimentally generated nonparaxial accelerating beams with arbitrary trajectories in a more effective and flexible strategy. [20][21][22] In lots of research where paraxial accelerating beams were explored, one can find that the acceleration of such beams is always DOI: 10.1002/andp.202000438 limited to a small scope.…”
Section: Introductionmentioning
confidence: 99%