Flashlamp Pumped Laser Technology 1986
DOI: 10.1117/12.966624
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Optimized Flashlamp Pumping of Disc Amplifiers

Abstract: Disk amplifier design for inertial fusion lasers has evolved with changing fusiondriver requirements from a primary emphasis on gain to a primary emphasis on efficiency. In this paper we compare Shiva and Nova amplifiers to a developmental amplifier (SSA) and show greater than a two -fold improvement in efficiency over past designs under all operating conditions. Experiments to optimize the efficiency of the SSA show that preionization of the flashlamps produces significant benefits and that the packing fracti… Show more

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“…Combining our results of i~eal single~pass flashlamp pumping and ASE decay, we can construct a differential equation to describe the energy density p* = N*hu of excited Nd .ions stored in the glass: (4) . .where Pout is the output flashlamp power per unit bore area, Tcav is the cavity transfer efficiency from lamps to the disks, AL is the lamp bore area, Vd is the disk volume, and 1:-1 is .the ASE-enhanced excited state decay rate, ko •+ kASE• The functions TlNd(Pout) and 't-1 (p*) are defined according to Eqn.…”
Section: Amplifier Pumping Modelmentioning
confidence: 99%
“…Combining our results of i~eal single~pass flashlamp pumping and ASE decay, we can construct a differential equation to describe the energy density p* = N*hu of excited Nd .ions stored in the glass: (4) . .where Pout is the output flashlamp power per unit bore area, Tcav is the cavity transfer efficiency from lamps to the disks, AL is the lamp bore area, Vd is the disk volume, and 1:-1 is .the ASE-enhanced excited state decay rate, ko •+ kASE• The functions TlNd(Pout) and 't-1 (p*) are defined according to Eqn.…”
Section: Amplifier Pumping Modelmentioning
confidence: 99%