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000473562 1001_ $$0P:(DE-H253)PIP1017401$$aMurari, Krishna$$b0$$eCorresponding author
000473562 245__ $$aSub-50 fs pulses at 2050 nm from a picosecond Ho:YLF laser using a two-stage Kagome-fiber-based compressor
000473562 260__ $$aWashington, DC$$bOSA$$c2022
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000473562 520__ $$aThe high-energy few-cycle mid-infrared laser pulse beyond 2 μm is of immense importance for attosecond science and strong-field physics. However, the limited gain bandwidth of laser crystals such as Ho:YLF and Ho:YAG allows the generation of picosecond (ps) long pulses and, hence, makes it challenging to generate few-cycle pulse at 2 μm without utilizing an optical parametric chirped-pulse amplifier (OPCPA). Moreover, the exclusive use of the near-infrared wavelength has limited the generation of wavelengths beyond 4 μm (OPCPA). Furthermore, high harmonic generation (HHG) conversion efficiency reduces dramatically when driven by a long-wavelength laser. Novel schemes such as multi-color HHG have been proposed to enhance the harmonic flux. Therefore, it is highly desirable to generate few-cycle to femtosecond pulses from a 2 μm laser for driving these experiments. Here, we utilize two-stage nonlinear spectral broadening and pulse compression based on the Kagome-type hollow-core photonic crystal fiber (HC-PCF) to compress few-ps pulses to sub-50 fs from a Ho:YLF amplifier at 2 μm at 1 kHz repetition rate. We demonstrate both experimentally and numerically the compression of 3.3 ps at 140 μJ pulses to 48 fs at 11 μJ with focal intensity reaching 10$^{13}$ W/cm$^2$. Thereby, this system can be used for driving HHG in solids at 2 μm. In the first stage, the pulses are spectrally broadened in Kagome fiber and compressed in a silicon-based prism compressor to 285 fs at a pulse energy of 90 μJ. In the second stage, the 285 fs pulse is self-compressed in air-filled HC-PCF. With fine-tuning of the group delay dispersion (GDD) externally in a 3 mm window, a compressed pulse of 48 fs is achieved. This leads to a 70-fold compression of the ps pulses at 2050 nm. We further used the sub-50 fs laser pulses to generate white light by focusing the pulse into a thin medium of YAG.
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000473562 693__ $$0EXP:(DE-H253)AXSIS-20200101$$1EXP:(DE-H253)SINBAD-20200101$$5EXP:(DE-H253)AXSIS-20200101$$aSINBAD$$eAXSIS: Frontiers in Attosecond X-ray Science, Imaging and Spectroscopy$$x1
000473562 7001_ $$0P:(DE-H253)PIP1015912$$aCirmi, Giovanni$$b1
000473562 7001_ $$0P:(DE-H253)PIP1015195$$aCankaya, Huseyin$$b2
000473562 7001_ $$0P:(DE-HGF)0$$aSTEIN, GREGORY J.$$b3
000473562 7001_ $$0P:(DE-HGF)0$$aDEBORD, BENOIT$$b4
000473562 7001_ $$0P:(DE-HGF)0$$aGÉRÔME, FREDERIC$$b5
000473562 7001_ $$0P:(DE-H253)PIP1085492$$aRitzkowsky, Felix$$b6
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000473562 7001_ $$0P:(DE-H253)PIP1013198$$aKärtner, Franz$$b8
000473562 773__ $$0PERI:(DE-600)2724783-1$$a10.1364/PRJ.441674$$gVol. 10, no. 3, p. 637 -$$n3$$p637 - 645$$tPhotonics research$$v10$$x2327-9125$$y2022
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