2011
DOI: 10.1103/physreva.84.063406
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High-order-harmonic generation in gas with a flat-top laser beam

Abstract: International audienceWe present experimental and numerical results on high-order-harmonic generation with a flat-top laser beam. We show that a simple binary tunable phase plate, made of two concentric glass plates, can produce a flat-top profile at the focus of a Gaussian infrared beam. Both experiments and numerical calculations show that there is a scaling law between the harmonic generation efficiency and the increase of the generation volume

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Cited by 37 publications
(29 citation statements)
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“…One SYLOS-driven beamline (GHHG SYLOS LONG) will employ an extremely loose focusing scheme, and will be coupled with a long interaction cell and very low gas pressures. This combination obeys geometrical scaling predictions and pressure related phase matching considerations governing GHHG in extended media [23][24][25]. The other SYLOS-driven beamline (GHHG SYLOS COMPACT) will also rely on loose focusing, but will utilize a high-pressure medium where phase matching is ensured by the short interaction length [26].…”
Section: Introductionmentioning
confidence: 99%
“…One SYLOS-driven beamline (GHHG SYLOS LONG) will employ an extremely loose focusing scheme, and will be coupled with a long interaction cell and very low gas pressures. This combination obeys geometrical scaling predictions and pressure related phase matching considerations governing GHHG in extended media [23][24][25]. The other SYLOS-driven beamline (GHHG SYLOS COMPACT) will also rely on loose focusing, but will utilize a high-pressure medium where phase matching is ensured by the short interaction length [26].…”
Section: Introductionmentioning
confidence: 99%
“…This analysis has been extremely successful for understanding spatio-spectral structures of the emitted harmonics driven by a single beam [36,37], and drives the design of efficient generating schemes (see e.g. [38][39][40][41][42][43]). Of particular interest are maps of the modulus of ∆ k + XU V , which inform us about the dominant generating regions of the gas target, while the direction of k q determines the emission direction.…”
Section: Structure Of a Two Beam Focusmentioning
confidence: 99%
“…In this way, it has been reported that some non-ideal focusing schemes improve the results in applications. For example, in the case of flat-top focal distributions in HHG [1], spatio-temporal couplings (e.g., with transversal spatial chirp to create attosecond lighthouses [2], angular chirp for angle-dependent emission of HHG [3], space-time focusing for microprocessing [4], or to control light velocity [5]). Also, beam aberrations are used to enhance nonlinear confocal microscopy [6], the filamentation process [7], or to generate a uniform ellipsoidal particle distribution [8].…”
Section: Introductionmentioning
confidence: 99%