2010
DOI: 10.1364/josaa.27.000327
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Normalization of optical Weber waves and Weber-Gauss beams

Abstract: The normalization of energy divergent Weber waves and finite energy Weber-Gauss beams is reported. The well-known Bessel and Mathieu waves are used to derive the integral relations between circular, elliptic, and parabolic waves and to present the Bessel and Mathieu wave decomposition of the Weber waves. The efficiency to approximate a Weber-Gauss beam as a finite superposition of Bessel-Gauss beams is also given.

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Cited by 25 publications
(7 citation statements)
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“…Optical diffraction sets universal performance limits on microscopy, lithography, and imaging, among myriad other areas. This fundamental limitation has motivated a long-standing effort for developing strategies to combat diffractive spreading [1][2][3][4][5][6][7], culminating in so-called 'diffraction-free' beams [8][9][10][11][12], of which Airy beams are the only scalar 1D diffraction-free optical sheet [13,14]. In considering pulsed beams (or wave packets), propagation invariance in free space has been predicted for specific wave packets, including Brittingham's focus-wave mode (FWM) [15], Mackinnon's wave packet [16], Xwaves [17][18][19], among many others [20][21][22][23][24][25] (see [26,27] for reviews).…”
Section: Introductionmentioning
confidence: 99%
“…Optical diffraction sets universal performance limits on microscopy, lithography, and imaging, among myriad other areas. This fundamental limitation has motivated a long-standing effort for developing strategies to combat diffractive spreading [1][2][3][4][5][6][7], culminating in so-called 'diffraction-free' beams [8][9][10][11][12], of which Airy beams are the only scalar 1D diffraction-free optical sheet [13,14]. In considering pulsed beams (or wave packets), propagation invariance in free space has been predicted for specific wave packets, including Brittingham's focus-wave mode (FWM) [15], Mackinnon's wave packet [16], Xwaves [17][18][19], among many others [20][21][22][23][24][25] (see [26,27] for reviews).…”
Section: Introductionmentioning
confidence: 99%
“…The demonstration of monochromatic quasi-diffraction-free Bessel beams by Durnin et al [1] fueled tremendous interest in devising optical fields that are propagation invariant [2,3]. The transverse spatial profile of such beams are eigenfunctions of the Helmholtz equation in various coordinate systems [4][5][6]; see [7] for a classification of all such solutions. There has been similar interest in synthesizing propagation-invariant pulsed beams (or wave packets) that are diffractionfree and dispersion-free in free space [8,9].…”
Section: Introductionmentioning
confidence: 99%
“…Starting in the year 1987 with the prediction and experimental implementation of the Bessel beam [11][12][13], in the following years the focus was put on the examination of nondiffracting beams characterized by a field distribution in curvilinear symmetries. It was already known that there are four different families of nondiffracting beams, and an extensive investigation was carried out for Bessel beams [14] and Mathieu beams [15,16], as well as Weber beams [17,18]. However, only small efforts were put into characterizing the beam family that is described in Cartesian coordinates, namely discrete nondiffracting beams (DNBs).…”
Section: Introductionmentioning
confidence: 99%