Nanosecond switching and amplification of multiline HF laser pulses

Abstract

Electrooptic gating and amplification of Pulses with durations from 1 to 5 ns were accomplished with a pulsed HF chemical laser system using SF <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">6</inf> -hydrocarbon media and transverse-discharge energization. The system comprised an apertured, pin-discharge multiline oscillator, a MgF <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> Rochon prism polarizer, a Pockels-effect, fast electrooptic switch, a 5:1 magnifying telescope, and a 22-mm diam, ∼ 5-MW TEA amplifier, together with several arrangements of polarization analyzer elements. A 5-mm, square-sectioned electrooptic crystal of CdTe or LiNbO <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">3</inf> yielded polarization contrast ratios of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">\sim 80:1</tex> under zero and half-wave electric fields. Without other measures, this contrast in gated amplitude was diminished in passage through the partially gain-saturated amplifier. However, 80:1 amplitude contrast in the gated, amplified pulse was preserved when file full oscillator beam intensity was used continuously to control the amplifier gain. This was done either with a polarization discriminator placed downstream of the amplifier, or with the two polarized components from the gate taking separate directions, intersecting within the amplifier.