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Wigner picture of partially coherent accelerating beams

Sergey A. Ponomarenko, Morteza Hajati

Abstract

We advance a phase-space theory of partially coherent accelerating, non-diffracting beams employing the Wigner distribution function (WDF). We derive a general expression for the WDF of any accelerating, diffraction-free beam of arbitrary degree of spatial coherence and find an elegant closed-form expression for the WDF of such beam with a Gaussian energy spectrum of noise. We also show how partially coherent accelerating beams of finite power can be constructed within the Wigner picture.

Wigner picture of partially coherent accelerating beams

Abstract

We advance a phase-space theory of partially coherent accelerating, non-diffracting beams employing the Wigner distribution function (WDF). We derive a general expression for the WDF of any accelerating, diffraction-free beam of arbitrary degree of spatial coherence and find an elegant closed-form expression for the WDF of such beam with a Gaussian energy spectrum of noise. We also show how partially coherent accelerating beams of finite power can be constructed within the Wigner picture.
Paper Structure (21 equations, 3 figures)

This paper contains 21 equations, 3 figures.

Figures (3)

  • Figure 1: Evolution of the WDF of an accelerating wave packet with propagation distance $z$ produced by a fairly coherent source with $\xi_c = 4$. The cut-off parameter of a Gaussian cut-off is $a = 0.1$.
  • Figure 2: Evolution of the WDF of an accelerating wave packet with propagation distance $z$ engendered by a relatively incoherent source with $\xi_c = 1$. We employ a Gaussian cut-off with the cut-off parameter $a = 0.1$.
  • Figure 3: Intensity profiles of accelerating wave packets generated by highly coherent $\xi_c = 10$ (left) and moderately incoherent $\xi_c = 2$ (right) sources as functions of X for three propagation distances: $z = 0$ (solid curve), $z = 2$ (dashed curve), and $z = 4$ (dotted curve). The cut-off parameter of a Gaussian cut-off is $a = 0.1$.