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CO 2 LaserThe ATF is one of the only two facilities worldwide operating picosecond, terawatt-class CO2 lasers. Our laser system consists of a picoseconds pulse-injector based on fast optical switching from the output of a conventional CO2 laser oscillator, and a chain of high-pressure laser amplifiers. It starts with a wavelength converter wherein a near-IR picosecond solid-state laser with l»1 mm produces a mid-IR 10-mm pulse. This process employs two methods; semiconductor optical switching, and the Kerr effect. First, we combine the outputs from a multi-nanosecond CO2 laser oscillator with a picosecond Nd:YAG laser on a germanium Brewster-plate to produce an ~200 ps, 10 mm pulse by semiconductor optical switching. Co-propagating this pulse with a Nd:YAG’s 2nd harmonic in a Kerr cell filled with an optically active CS2 fluid, we slice out a 5 ps, 10 mm pulse at the ~0.1 MW peak power-level. Immediately after a low-power
l»10
mm seed pulse is produced, it
is amplified in a chain of high pressure (~10 atm.) CO2
laser-amplifiers. At the first
stage, the pulse is seeded into an isotope-filled CO2
regenerative amplifier where it is trapped for 10-12 round trips and then
released on reaching the ~1 GW level. A final high-pressure, large-aperture (10 cm) amplifier boosts the
laser pulse to 1 TW for use in the experiments discussed above. Fig. 1 is a principle diagram of the ATF laser system; Fig.
2 illustrates the ATF’s assembly of high-pressure laser amplifiers. For more
technical details, refer to
Optics Express, Vol. 19, Issue 8, pp. 7717-7725 (2011) or call
Pogorelsky. Presently we
implement a major CO2 laser upgrade
to the multi-terawatt ultra-fast regime.
Last Modified: November 14, 2012 |