2018
DOI: 10.1364/ol.43.004643
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All-solid-state multipass spectral broadening to sub-20  fs

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Cited by 113 publications
(63 citation statements)
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References 31 publications
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“…3(a)] with an average power of 70 W at a repetition rate of 28 MHz. The configuration of this system is very similar to the one published by Fritsch et al [28], but with only two Herriott cells for the spectral broadening instead of three. Both ZnSe and ZnS crystals were tested under an average input power of 4 and 6.5 W, respectively.…”
Section: Lettermentioning
confidence: 75%
“…3(a)] with an average power of 70 W at a repetition rate of 28 MHz. The configuration of this system is very similar to the one published by Fritsch et al [28], but with only two Herriott cells for the spectral broadening instead of three. Both ZnSe and ZnS crystals were tested under an average input power of 4 and 6.5 W, respectively.…”
Section: Lettermentioning
confidence: 75%
“…Ongoing efforts to improve the quality of this and other Yb-doped broadband gain materials are expected to bring further improvements to the achievable levels. In parallel to these efforts, large progress has been made in finding paths for efficient external pulse compression of these high-average power laser systems using hollow-core fibers [48], multi-pass cells [49][50][51][52], hybrid setups including multi-plate compressors [53], and even spectral broadening in the amplifier itself [54] bringing these applications one step closer. Additionally, as the pulse durations from these systems keeps getting shorter and approach the few-cycle regime, carrier-envelope phase control becomes increasingly relevant, in particular for high-power oscillators which can be used as powerful seeds for booster amplifiers [55,56].…”
Section: Resultsmentioning
confidence: 99%
“…Additionally, the high intracavity power in TDL oscillators can be leveraged to drive intracavity nonlinear-optics experiments [13]. Finally, the recent demonstrations of multi-pass cell compression at 375-W average output power to 170 fs [14] and at 60 W to 16 fs pulses [15], show the possibility to compress the high-power output of these oscillators in order to get the optimal peak power for many nonlinear optics applications.…”
Section: Introductionmentioning
confidence: 99%