Nonlinear Optics 2011
DOI: 10.1364/nlo.2011.nthc1
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Femtosecond operation and self-doubling of Cr:ZnS laser

Abstract: Prismless dispersion-controlled Cr:ZnS laser generates first femtosecond (110 fs) pulses at 180 MHz repetition rate around 2400 nm with average power 200 mW. Co-propagating secondharmonic pulse at 1200 nm is simultaneously generated in ceramic sample.

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Cited by 9 publications
(9 citation statements)
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“…The setup is distinguished from the existing similar measurement systems [16], [18] by using new broadband light sources, such as superluminescent Tm-doped fiber based source and a recently developed in our lab mode-locked femtosecond Cr:ZnS oscillator [19], [20]. These sources allow achieving broad spectral coverage with the higher output power and with a high signal/noise ratio.…”
Section: Introductionmentioning
confidence: 99%
“…The setup is distinguished from the existing similar measurement systems [16], [18] by using new broadband light sources, such as superluminescent Tm-doped fiber based source and a recently developed in our lab mode-locked femtosecond Cr:ZnS oscillator [19], [20]. These sources allow achieving broad spectral coverage with the higher output power and with a high signal/noise ratio.…”
Section: Introductionmentioning
confidence: 99%
“…Nevertheless, subject to a proper orientation, the CW output power of 700 mW at 2.35 m with 700 nm wavelength tuning were demonstrated using Cr:ZnS single crystal as a laser active element [14]. Subsequently, the laser action in microchip configuration [15], picosecond passive mode-locking [16] and finally, femtosecond SESAM-initiated mode-locking was obtained in 2011 with 1.2 nJ 110 fs pulses [17]. The CW output power of 10 W was obtained recently using polycrystalline Cr:ZnS as an active element [18].…”
mentioning
confidence: 99%
“…In this work we demonstrate the first fiber delivery of the high energy femtosecond mid-IR laser pulses (70 fs), produced by the recently developed in our group femtosecond mid-IR Cr:ZnS laser [11,12]. By changing the launched pulse energy we are able to observe a transition from strongly chirped linear to solitonic propagation at launched energies below 2 nJ.…”
Section: Introductionmentioning
confidence: 93%