2012
DOI: 10.1364/ol.37.000933
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High-average-power, carrier-envelope phase-stable, few-cycle pulses at 21 μm from a collinear BiB_3O_6 optical parametric amplifier

Abstract: We generate self-carrier-to-envelope phase-stable, 630 μJ pulses, centered at 2.1 μm, with 42 fs (6 cycle) duration based on collinear optical parametric amplification in BiB(3)O(6) at 3 kHz. These pulses are generated through a traveling wave amplifier scheme, and the bandwidth supports 28 fs (4 cycle) pulse duration. Carrier-to-envelope phase stability was measured to be 410 mrad over 10 min or 260 mrad over 35 s.

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Cited by 47 publications
(31 citation statements)
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“…Due to their simple setup and spectral versatility, they have many advantages over optical parametric oscillators (OPOs) [2][3][4]. However, they require rather high pump energies, typically provided by amplified laser systems, limiting the repetition rate to a few hundred kilohertz [5][6][7]. Recently, the repetition rate of OPAs has been pushed to the MHz range by using laser oscillators with cavity dumping [8][9][10] or fiber amplifiers [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…Due to their simple setup and spectral versatility, they have many advantages over optical parametric oscillators (OPOs) [2][3][4]. However, they require rather high pump energies, typically provided by amplified laser systems, limiting the repetition rate to a few hundred kilohertz [5][6][7]. Recently, the repetition rate of OPAs has been pushed to the MHz range by using laser oscillators with cavity dumping [8][9][10] or fiber amplifiers [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…High peak power pulses at 2 µm wavelength combined with the characteristic advantages of fiber lasers, such as high beam quality, compactness and the potential for maintenance-free operation, are particularly beneficial from an applications point of view and enable, for example, coherent nonlinear frequency conversion further into the mid-infrared waveband, material or medical tissue ablation, and high-intensity physics [3,[6][7][8][9][10]. Table 1 gives an overview of the current maximum peak power levels reported for the different pulse regimes of TDFA systems.…”
Section: Introductionmentioning
confidence: 99%
“…BiBO was reported by Silva et al generating CEP-stable pulses at 2.1 µm [200]. Cascaded high-energy OPA-systems have nonetheless been implemented in which a second stage of parametric frequency conversion (mostly DFG) enables reaching the mid-IR spectral range at the expense of efficiency and simplicity [201,202,203].…”
mentioning
confidence: 99%