2012
DOI: 10.1364/oe.20.026913
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Negative propagation effect in nonparaxial Airy beams

Abstract: Abstract:Negative propagation is an unusual effect concerning the local sign change in the Poynting vector components of an optical beam under free propagation. We report this effect for finite-energy Airy beams in a subwavelength nonparaxial regime. This effect is due to a coupling process between propagating and evanescent plane waves forming the beam in the spectral domain and it is demonstrated for a single TE or TM mode. This is contrary to what happens for vector Bessel beams and vector X-waves, for whic… Show more

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Cited by 51 publications
(24 citation statements)
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“…(c)). Analysis presented in Ref . concludes that the break up of the beam shape occurs exclusively due to the propagating component of the radiation while the interference of the propagating and evanescent waves can cause an inversion of energy flow (negative propagation) for some of the beam lobes.…”
Section: Non‐paraxial Casementioning
confidence: 99%
“…(c)). Analysis presented in Ref . concludes that the break up of the beam shape occurs exclusively due to the propagating component of the radiation while the interference of the propagating and evanescent waves can cause an inversion of energy flow (negative propagation) for some of the beam lobes.…”
Section: Non‐paraxial Casementioning
confidence: 99%
“…An analytic expression for an SAB was not found. However, its paraxial solution vx; z can easily be built by using the angular spectrum formalism [15] vx;z 1 (2) where VK;z ≡ F fvx;zg and the even cubic phase enters the argument of V 0 :…”
mentioning
confidence: 99%
“…Relying on the decomposition of the Poynting vector in two constituents corresponding to the orbital energy and spin flows, we offer an interpretation of the reverse energy flow, which has been known in optics for quite long (since 1919 [31,7]) but has so far failed to obtain the proper interpretation. Energy backflow is a rather universal optical phenomenon that occurs not only in sharp focus, but also in some laser beams like, e.g., vector X-waves [32], nonparaxial Airy beams [33] and fractional Bessel vortex beams [34]. Below, we prove that the reverse energy flow occurs in the optical field regions where the on-axis projection of the spin flow is negative and larger in magnitude than the always positive onaxis projection of the orbital energy flow.…”
Section: Introductionmentioning
confidence: 61%