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Ultrashort pulse CPA-free Ho:YLF linear amplifier
- Source :
- Solid State Lasers XXVII: Technology and Devices : 29 January-1 February 2018, San Francisco, California, United States, Proceedings of SPIE 10511 (2018)
- Publication Year :
- 2018
- Publisher :
- Bellingham, WA : S P I E - International Society for Optical Engineering, 2018.
-
Abstract
- We present CPA-free linear amplification of 6:3 ps pulses in Ho:YLF crystals up to 100 μJ pulse energy at 10 kHz repetition rate. The seed pulses at a wavelength of 2:05 μm are provided by a Ho-based all-fiber system consisting of a soliton oscillator and a subsequent pre-amplifier followed by a free-space AOM as pulse-picker. Considering the achieved pulse peak power at MW-level, this system is a powerful tool for efficient pumping of parametric amplifiers addressing the highly demanded mid-IR spectral region. In detailed numerical simulations we verified our experimental results and discuss scaling options for pulse duration and energy. © 2018 SPIE.
- Subjects :
- Optical pumping
Solid state lasers
Materials science
Dewey Decimal Classification::600 | Technik::620 | Ingenieurwissenschaften und Maschinenbau
Ultrashort Laser
Soliton (optics)
Pulse repetition rate
ultrashort lasers
Ultrashort pulses
Optics
Linear amplifier
Optical parametric amplifiers
Linear amplification
Linear amplifiers
All-fiber system
Konferenzschrift
Ultrafast lasers
infrared lasers
Laser amplifiers
Soliton oscillators
business.industry
Amplifier
Fiber amplifiers
Pulse duration
Pulse (physics)
mode-locked lasers
Parametric amplifiers
Wavelength
Amplifiers (electronic)
Mode-locked laser
IR spectral regions
solid-state lasers
ddc:620
business
Ultrashort pulse
Subjects
Details
- Language :
- English
- Database :
- OpenAIRE
- Journal :
- Solid State Lasers XXVII: Technology and Devices : 29 January-1 February 2018, San Francisco, California, United States, Proceedings of SPIE 10511 (2018)
- Accession number :
- edsair.doi.dedup.....4d152063b33c4a26d0105a3bd1d98e4d
- Full Text :
- https://doi.org/10.15488/3399