2018
DOI: 10.1007/978-3-319-92843-2
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Generation and Parametric Amplification of Few‐Cycle Light Pulses at Relativistic Intensities

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“…Fortunately, defocused chirped lasers provide different wavefronts for each cycle due to the variational wavelength, i.e., variational Rayleigh length. To the best of our knowledge, chirped lasers, which are becoming accessible with relative bandwidth as high as 60% [37] and power approaching 100 TW [38] and even PW [39] in the future, are never used to generate IAPs based on RHHG although they have been investigated widely in particle acceleration [40,41], pair production [42], and even gaseous high-order harmonic generation [43,44].…”
Section: Introductionmentioning
confidence: 99%
“…Fortunately, defocused chirped lasers provide different wavefronts for each cycle due to the variational wavelength, i.e., variational Rayleigh length. To the best of our knowledge, chirped lasers, which are becoming accessible with relative bandwidth as high as 60% [37] and power approaching 100 TW [38] and even PW [39] in the future, are never used to generate IAPs based on RHHG although they have been investigated widely in particle acceleration [40,41], pair production [42], and even gaseous high-order harmonic generation [43,44].…”
Section: Introductionmentioning
confidence: 99%