2009
DOI: 10.1007/s00340-009-3425-z
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High-repetition-rate femtosecond optical parametric chirped-pulse amplifier in the mid-infrared

Abstract: We discuss a dual-stage optical parametric chirped-pulse amplifier generating sub-100-fs pulses in the mid-infrared at a repetition rate of 100 kHz. The system is based on a 1064 nm pump laser and a 3-4 µm difference frequency generation seed source derived from the output of a femtosecond fiber laser amplifier. Both lasers are commercially available, are diode-pumped, compact, and allow for turn-key operation. Here, we focus our discussion on the design and dimensioning of the optical parametric chirpedpulse … Show more

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Cited by 24 publications
(12 citation statements)
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“…The resulting 6 ps pulse width is well matched to the pump pulse width [116,117]. The OPCPA consists of two stages, both using MgO:PPLN crystals, and produces 100 mW average power, corresponding to 1 μJ per pulse.…”
Section: High Repetition Rate Cep-stable Pulses From a Fiber-format Omentioning
confidence: 99%
“…The resulting 6 ps pulse width is well matched to the pump pulse width [116,117]. The OPCPA consists of two stages, both using MgO:PPLN crystals, and produces 100 mW average power, corresponding to 1 μJ per pulse.…”
Section: High Repetition Rate Cep-stable Pulses From a Fiber-format Omentioning
confidence: 99%
“…Recently, however, a number of strong-field ionization phenomena has been revealed which are caused by non-perturbative influence of the Coulomb field of the atomic core [5]: doublehump and interference structures [6,7] in the momentum distribution of photoelectrons near ionization threshold, frustrated tunneling ionization [8], and multiphoton assisted recombination [9]. With the advent and further improvement of intense femtosecond mid-infrared laser sources [10], the classical regime of strong-field ionization, when the Keldysh parameter γ ≪ 1 and one expects the SFA to provide an adequate description, has been subjected to more attentive investigation. Here, γ = I p /2U p , I p is the ionization potential, and U p the ponderomotive energy.…”
mentioning
confidence: 99%
“…Although fine-tuning the GDD is possible using Si prisms [6,17,18], adding a Si wafer to the optical beam path is significantly simpler. Since Si wafers of various thicknesses are readily available commercially, the addition of the Si wafer provides a simple, practical solution for dispersion compensation at 1,700 nm.…”
Section: Discussionmentioning
confidence: 99%