2013
DOI: 10.1364/ol.38.004354
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Pulse compression to subcycle field waveforms with split-dispersion cascaded hollow fibers

Abstract: Carefully dispersion- and nonlinearity-managed cascades of gas-filled hollow-core fibers enable, as our theoretical analysis shows, efficient pulse compression with ultrahigh compression ratios. With dispersion and nonlinearity of individual fibers in such cascades optimized toward distinctly different goal functions, millijoule picosecond laser pulses can be compressed to sub-100-GW subcycle field waveforms.

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Cited by 15 publications
(8 citation statements)
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“…This approach would eliminate the need for the active pump-seed synchronization system for the OPCPA, because both the pump and the seed would travel comparable optical paths. In a cascaded gas-filled-HCF, the 1 ps input pulses centered at 1030 nm could be broadened to 700 − 1500 nm (Voronin et al, 2013). Although in this scheme the spectral phase in the vicinity of 1030 nm is not well-behaved and could cause a long pedestal in the time domain, the spectral phase in the blue and red wings of the spectrum are well-behaved and suitable for a type II DFG process.…”
Section: -Ps-pumped Multi-octave Seed Generationmentioning
confidence: 99%
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“…This approach would eliminate the need for the active pump-seed synchronization system for the OPCPA, because both the pump and the seed would travel comparable optical paths. In a cascaded gas-filled-HCF, the 1 ps input pulses centered at 1030 nm could be broadened to 700 − 1500 nm (Voronin et al, 2013). Although in this scheme the spectral phase in the vicinity of 1030 nm is not well-behaved and could cause a long pedestal in the time domain, the spectral phase in the blue and red wings of the spectrum are well-behaved and suitable for a type II DFG process.…”
Section: -Ps-pumped Multi-octave Seed Generationmentioning
confidence: 99%
“…9(a). The 10-fs-scale seed pulses may possibly also be derived directly from the output of the near-1-ps Yb:YAG pump source by cascaded temporal compression [182], as indicated by a dashed line in Fig. 9(a).…”
Section: B Generation Of Waveform-controlled Continua For Opa Seedingmentioning
confidence: 99%
“…Therefore, the requirement for the control of these recurrent dynamics can be easily satisfied via the longitudinal adjustment of waveguide structures [22]. This can be done by either tapering the optical fiber along the propagation axis [23,24] or concatenating fibers with longitudinal tailoring properties [25,26]. In such a configuration, the quasi-stabilization evolution of breather waves can be realized using the technique based on the similarity between compressed breathers and fundamental solitons [27].…”
Section: Introductionmentioning
confidence: 99%
“…Extremely short pulses were obtained in nonlinear optical fibers, both in the region of normal dispersion with the subsequent use of dispersion compressors [2][3][4], and in the region of anomalous dispersion due to multisoliton compression [5][6][7][8]. At a millijoule energy level, they were produced in gas-filled capillaries and photon-crystalline fibers due to the combined effect of ionization nonlinearity and plasma dispersion of group velocities [9][10][11][12]. A similar mechanism is realized by using filaments [13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%