2016
DOI: 10.1364/oe.24.007224
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Supercontinuum generation in a multi-plate medium

Abstract: We analyze femtosecond supercontinuum generation in a distribution of thin solid plates to show that the distributed scheme inhibits processes leading to pulse breakup while allowing spectral expansion to proceed as desired. We introduce basic criteria for setting the plate thickness or initial laser intensity and the location of each plate in the laser beam path and confirm that under these conditions a fully-coherent and intense supercontinuum can be generated for input peak power of as much as two thousand … Show more

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Cited by 67 publications
(36 citation statements)
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“…A different approach is to omit the waveguide and achieve spectral broadening at free propagation through a bulk dielectric [10][11][12][13]. This allows using peak powers well above the critical power for self-focusing, accessing the energy range 3-100 µJ.…”
Section: Introductionmentioning
confidence: 99%
“…A different approach is to omit the waveguide and achieve spectral broadening at free propagation through a bulk dielectric [10][11][12][13]. This allows using peak powers well above the critical power for self-focusing, accessing the energy range 3-100 µJ.…”
Section: Introductionmentioning
confidence: 99%
“…For comparison, we assume that the 971 J input have a square aperture of 980 mm × 980 mm and the 1,358 J input has a linearly increased square aperture of 1160 mm × 1160 mm (for the same energy fluence), all with flat-top beams but different spectra. The input intensity at the fused silica thin wafer cannot be too high (lead to conical emission and even dielectric breakdown) or too low (weaken spectral broadening), and here it is kept at around 10 TW/cm 2 , because at this intensity the multiphoton-induced plasma density in fused silica is safely below the documented avalanche plasma density 57 . The spectrum of WNOPCPA is shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Behind the focus another plate is placed into the divergent beam which will be refocused again by the self-focusing effect inside the next plate. As each plate can introduce a B-integral of 4-5 [54,55], a sequence of such refocusing thin plates can result in supercontinuum ( Figure 3(b)) and very large compression factors down to the singlecycle limit [56]. The downside of this technique is the poor energy scalability (sub-mJ regime), as it inherently relies on condensed materials with high nonlinearity, and a small amount of remaining spatial chirp of the output beam [57].…”
Section: Multiple-plate Continuum Generationmentioning
confidence: 99%