Conference on Lasers and Electro-Optics 2012 2012
DOI: 10.1364/cleo_si.2012.cth1n.6
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High efficiency, multi-mJ, sub 10 fs, optical parametric amplifier at 3 kHz

Abstract: Abstract:We present a short-pulse pumped optical parametric amplifier (OPA) with a broadband spectrum from 670 nm to 1000 nm, supporting 5.7 fs pulses with > 32 % pump-to-signal conversion efficiency resulting in pulse energies of 2.5 mJ.

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Cited by 10 publications
(14 citation statements)
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“…For pump pulses with picosecond duration, the seed pulse was typically chosen to fit. Re-using of the pump was previously reported by focusing the amplified signal and the depleted pump into an additional nonlinear crystal [13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…For pump pulses with picosecond duration, the seed pulse was typically chosen to fit. Re-using of the pump was previously reported by focusing the amplified signal and the depleted pump into an additional nonlinear crystal [13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Optical parametric chirped pulse amplification (OPCPA) represents the most promising route to simultaneously achieving high pulse energies and large amplification bandwidths supporting intense, few-cycle pulses [4]. To push the frontiers of ultrafast pulse generation, pump lasers delivering sub-10 ps, highenergy pulses with near diffraction limited beam quality, ideally at repetition rates in the kHz to MHz range, are required [2,5].…”
Section: Introductionmentioning
confidence: 99%
“…Ultrafast optical parametric chirped pulse amplifiers (OPCPA) [11] have hitherto proven to be the only method for scaling few-cycle pulses to the multi-mJ energy level [12,13]. In particular <2 ps short-pulse-pumped OPCPAs [10] allow for highly efficient and ultrabroadband laser sources [14,15] and exhibit the following key advantages: The reduced stretching ratio simplifies the dispersion management and enables the stretching of the seed pulses by a few mm short glass plate and recompression by a few highly efficient chirped multilayer mirrors [16]. The increased damage threshold for transparent optical materials for pulse durations <10 ps [16] permits higher pump intensities, hence the use of a few mm thin OPA crystals resulting in ultrabroadband amplification due to reduced phase matching issues.…”
Section: Introductionmentioning
confidence: 99%
“…The increased damage threshold for transparent optical materials for pulse durations <10 ps [16] permits higher pump intensities, hence the use of a few mm thin OPA crystals resulting in ultrabroadband amplification due to reduced phase matching issues. The <2 ps short-pulse-pump approach and the resulting applicable high intensities result in large pump-to-signal conversion efficiencies >30 % [14]. Furthermore the ~1 ps short pump window leads to an inherently excellent temporal pulse contrast.…”
Section: Introductionmentioning
confidence: 99%