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New direct-drive laser target designs with KrF laser light take advantage of the shorter wavelength to lower the laser energy required for substantial gain (>30×) to sub-MJ level. These low lase...

Laser plasma instability experiments with KrF lasers

Phys. Plasmas 14, 056316 (2007); doi:10.1063/1.2672029

Published 18 May 2007

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J. L. Weaver,1 J. Oh,2 B. Afeyan,3 L. Phillips,4 J. Seely,5 U. Feldman,6 C. Brown,5 M. Karasik,1 V. Serlin,1 Y. Aglitskiy,7 A. N. Mostovych,8 G. Holland,9 S. Obenschain,1 L-Y. Chan,1 D. Kehne,1 R. H. Lehmberg,2 A. J. Schmitt,1 D. Colombant,1 and A. Velikovich1
1Plasma Physics Division, U.S. Naval Research Laboratory, Washington, DC 20375
2Research Support Instruments, Inc., Lanham, Maryland 20706
3Polymath Research, Inc., Pleasanton, California 94566
4Laboratory for Computational Physics & Fluid Dynamics, U.S. Naval Research Laboratory, Washington, DC 20375
5Space Science Division, U.S. Naval Research Laboratory, Washington, DC 20375
6ARTEP, Inc., Ellicott City, Maryland 21042
7SAIC, Inc., McLean, Virginia 22102
8Enterprise Sciences, Inc., Silver Spring, Maryland 20905
9SFA, Inc., Crofton, Maryland 21114

Deleterious effects of laser-plasma instability (LPI) may limit the maximum laser irradiation that can be used for inertial confinement fusion. The short wavelength (248  nm), large bandwidth, and very uniform illumination available with krypton-fluoride (KrF) lasers should increase the maximum usable intensity by suppressing LPI. The concomitant increase in ablation pressure would allow implosion of low-aspect-ratio pellets to ignition with substantial gain (>20) at much reduced laser energy. The proposed KrF-laser-based Fusion Test Facility (FTF) would exploit this strategy to achieve significant fusion power (150  MW) with a rep-rate system that has a per pulse laser energy well below 1 MJ. Measurements of LPI using the Nike KrF laser are presented at and above intensities needed for the FTF (I~2×1015  W/cm2). The results to date indicate that LPI is indeed suppressed. With overlapped beam intensity above the planar, single beam intensity threshold for the two-plasmon decay instability, no evidence of instability was observed via measurements of (3/2)omegao and (1/2)omegao harmonic emissions. ©2007 American Institute of Physics
History: Received 17 November 2006; accepted 22 January 2007; published 18 May 2007
Permalink: http://link.aip.org/link/?PHPAEN/14/056316/1
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KEYWORDS and PACS

Keywords
PACS
  • 52.35.Py
    Plasma macroinstabilities (hydromagnetic) e.g., kink, fire-hose, mirror, ballooning, tearing, trapped-particle, flute, Rayleigh-Taylor instabilities, etc
  • 52.38.Mf
    Laser ablation
  • 52.50.Lp
    Plasma production and heating by shock waves and compression
  • 52.50.Jm
    Plasma production and heating by laser beams including laser–foil, laser–cluster, etc
  • 52.57.Fg
    Implosion symmetry and hydrodynamic instability for laser ICF including Rayleigh-Taylor, Richtmyer-Meshkov, imprint, etc
  • 52.25.Os
    Emission, absorption, and scattering of electromagnetic radiation from plasmas
  • YEAR: 2007

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ISSN:
1070-664X (print)   1089-7674 (online)
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