2005
DOI: 10.1016/j.optcom.2005.04.027
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Characteristics of a stable, injection Q-switched Nd:phosphate glass regenerative amplifier for a chirped pulse amplification based Table Top Terawatt laser system

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Cited by 17 publications
(5 citation statements)
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“…Required tolerance on inter-grating groove density errors and aberrations to achieve desired pulsed beam parameters are discussed latter in this section. Regenerative amplifier [32], basically a Q-switched and cavity dumped (QS&CD) laser oscillator consists of cavity formed using ~100% reflectivity plane and curved mirror with radius of curvature of 6 m, includes two electromagnetic interference (emi) noise shielded 40 mm long deuterated potassium di-hydrogen phosphate (DKDP) crystal based single Pockels cells [33] together with 3 mm thick thin film polarizer to act as pulse injector and ejector to avoid a dedicated advanced switching electronics required for a single electro-optic unit.…”
Section: Description and Characteristics Of Laser Systemmentioning
confidence: 99%
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“…Required tolerance on inter-grating groove density errors and aberrations to achieve desired pulsed beam parameters are discussed latter in this section. Regenerative amplifier [32], basically a Q-switched and cavity dumped (QS&CD) laser oscillator consists of cavity formed using ~100% reflectivity plane and curved mirror with radius of curvature of 6 m, includes two electromagnetic interference (emi) noise shielded 40 mm long deuterated potassium di-hydrogen phosphate (DKDP) crystal based single Pockels cells [33] together with 3 mm thick thin film polarizer to act as pulse injector and ejector to avoid a dedicated advanced switching electronics required for a single electro-optic unit.…”
Section: Description and Characteristics Of Laser Systemmentioning
confidence: 99%
“…Output pulse energy is stabilized below pump pulse energy fluctuations [32] via interplay of gain and loss of amplifier cavity and is achieved by ejecting amplified pulse at post peak buildup with re-optimized laser system and compressor parameters owing to accumulated nonlinear phase. While enhanced nonlinear phase help to minimize gain-narrowing of pre-amplifier, curvature of the amplified pulsed beam is also increased necessitating re-optimization of beam expander for faithful amplification of laser pulses in the power amplifier.…”
Section: For Clearer Illustration For Each Compressor Grating; (C) Va...mentioning
confidence: 99%
“…The double pass arrangement increases the pulse stretching by twofold. This type of dispersive pulse stretcher was used to temporally stretch laser pulses of duration 250 fs (FWHM) from a Nd:flouro phosphate glass oscillator to 240 ps (FWHM) by placing a pair of identical holographic gratings (groove density = 1740 l/mm) symmetrically outside of two identical achromatic lenses (focal length = 500 mm) at a distance of 250 mm and using a retro-reflector to obtain a linear chirp of 44 ps/nm at central wavelength of 1054 nm (Sharma et al, 2005).…”
Section: Pulse Stretching By Dispersionmentioning
confidence: 99%
“…However, the repetition rate of PAMs is low due to the poor heat conductivity coefficient of Nd:glass. Tens of minutes are usually required per shoot for heat recovery (Orth et al 1996;Peng et al 2014;Sharma et al 2005). Good beam quality is another important factor required in PAM, which is the premise of stable and safe amplification by the subsequent main amplifier.…”
Section: Introductionmentioning
confidence: 99%