2004
DOI: 10.1117/12.567390
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Truncated ultrashort-pulse small-angle Bessel beams

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Cited by 7 publications
(5 citation statements)
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“…The positions of minima remain constant for symmetric spectra, whereas the contrast significantly depends on the bandwidth and, for pulses with space-time coupling effects by travel time differences, on the pulse duration. This is further confirmed by the experimentally detected spatio-spectral map in the center of the Bessel zone (Figure 5), where most of the spectral content is localized within the central lobe and the spectrally resolved Bessel fringes diverge with increasing wavelength [2,80,118]. Therefore, a nondiffractive selection of the central lobe enables to minimize the spatial chirp and to optimize free-space pulse transfer.…”
Section: Ultrashort Pulsed Needle Beams and Linear Rogue Wavessupporting
confidence: 55%
See 1 more Smart Citation
“…The positions of minima remain constant for symmetric spectra, whereas the contrast significantly depends on the bandwidth and, for pulses with space-time coupling effects by travel time differences, on the pulse duration. This is further confirmed by the experimentally detected spatio-spectral map in the center of the Bessel zone (Figure 5), where most of the spectral content is localized within the central lobe and the spectrally resolved Bessel fringes diverge with increasing wavelength [2,80,118]. Therefore, a nondiffractive selection of the central lobe enables to minimize the spatial chirp and to optimize free-space pulse transfer.…”
Section: Ultrashort Pulsed Needle Beams and Linear Rogue Wavessupporting
confidence: 55%
“…If the central lobe is selected by a well-adapted diaphragm which matches the first minimum of the intensity distribution, i.e. the dark zone with the smallest intensity gradient, diffraction at the edge is minimized [2,118]. The configuration is based on a field apodization and was referred to as 'selfapodizing truncation' [2].…”
Section: Self-apodizing Truncation Of Bessel Beamsmentioning
confidence: 99%
“…A timeline of significant events in the development of propagation-invariant wave packets. In chronological order: Brittingham's FWM (1983) [25]; finite-energy FWM (1985) [156]; synthesis of acoustic FWMs (1990) [85] and ultrasonic X-waves (1992) [33]; producing incoherent optical X-waves (1997) [34] and incoherent optical FWMs (2002) [96]; nonlinear X-waves (2003) [158] and coherent optical X-waves (2003) [159]; observing X-wave self-healing (2004) [160]; producing a needle beam (2004) [161]; observing a nonlinear transition from X-to O-shaped spectra in water (2005) [141]; measuring the group velocity of X-waves [162]; and accelerating X-waves (2009) [163]. Baseband ST wave packets have been pursued since 2016 [97].…”
Section: First Period: 1983-1996mentioning
confidence: 99%
“…In both cases, only a bright central peak is obtained. Measurements reveal that this truncation produces a stable 'needle beam' for an extended propagation distance with no side 'fringes' [161,188,189]. This unique feature allows for images to be transmitted with no diffraction by pixellating the transverse profile and utilizing an array of needle beams, one at each pixel [190][191][192].…”
Section: Second Period: 1996-2003mentioning
confidence: 99%
“…aperture diameter matching the first dark fringe of a Bessel intensity pattern) maintain ultra-broad spectral bandwidth as well as their pulse duration [3]. Compared to focused Gaussian beams, such needle-shaped TBB ("needle beams"; see ref.…”
Section: Introductionmentioning
confidence: 99%