Bifurcating trajectory of non-diffractive electromagnetic airy pulse

Alexander G. Nerukh, Denis A. Zolotariov, Dmitry Nerukh

Research output: Other contribution

Abstract

The explicit expression for spatial-temporal Airy pulse is derived from the Maxwell's equations in paraxial approximation. The trajectory of the pulse in the time-space coordinates is analysed. The existence of a bifurcation point that separates regions with qualitatively different features of the pulse propagation is demonstrated. At this point the velocity of the pulse becomes infinite and the orientation of it changes to the opposite.
Original languageEnglish
TypePublication on ArXiv
Media of outputOnline
Publication statusUnpublished - 15 Aug 2011

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trajectories
electromagnetism
pulses
Maxwell equation
propagation
approximation

Bibliographical note

Creative Commons

Keywords

  • physics
  • optics

Cite this

Nerukh, A. G., Zolotariov, D. A., & Nerukh, D. (2011, Aug 15). Bifurcating trajectory of non-diffractive electromagnetic airy pulse. Unpublished.
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Bifurcating trajectory of non-diffractive electromagnetic airy pulse. / Nerukh, Alexander G.; Zolotariov, Denis A.; Nerukh, Dmitry.

2011, Publication on ArXiv.

Research output: Other contribution

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AU - Zolotariov, Denis A.

AU - Nerukh, Dmitry

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N2 - The explicit expression for spatial-temporal Airy pulse is derived from the Maxwell's equations in paraxial approximation. The trajectory of the pulse in the time-space coordinates is analysed. The existence of a bifurcation point that separates regions with qualitatively different features of the pulse propagation is demonstrated. At this point the velocity of the pulse becomes infinite and the orientation of it changes to the opposite.

AB - The explicit expression for spatial-temporal Airy pulse is derived from the Maxwell's equations in paraxial approximation. The trajectory of the pulse in the time-space coordinates is analysed. The existence of a bifurcation point that separates regions with qualitatively different features of the pulse propagation is demonstrated. At this point the velocity of the pulse becomes infinite and the orientation of it changes to the opposite.

KW - physics

KW - optics

M3 - Other contribution

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