1996
DOI: 10.1063/1.871863
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Energy transfer between crossing laser beams

Abstract: Induced scattering between crossing laser beams is considered, including the effects of long-wavelength modulations in the plasma. This fundamental process can impact the choice of beam-smoothing techniques for laser-driven hohlraums. Study of this process is an ideal way to quantify stimulated scattering instabilities, since one can independently vary the intensity, polarization, and frequency separation of the crossing beams.

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Cited by 181 publications
(109 citation statements)
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“…1a). This diagnostic captures time-integrated images of the interior of the hohlraum wall x-ray emission at [3][4][5] keV through the LEH. As the backscatter losses on the outer beams were negligible (<1%), SXI provides a direct measurement of the decrease of the laser energy deposited on the hohlraum wall by the outer beams.…”
Section: Inferring Srs On the 235 • Conementioning
confidence: 99%
See 1 more Smart Citation
“…1a). This diagnostic captures time-integrated images of the interior of the hohlraum wall x-ray emission at [3][4][5] keV through the LEH. As the backscatter losses on the outer beams were negligible (<1%), SXI provides a direct measurement of the decrease of the laser energy deposited on the hohlraum wall by the outer beams.…”
Section: Inferring Srs On the 235 • Conementioning
confidence: 99%
“…Laser plasma instabilities (LPI) determine the laser energy deposition into the hohlraum wall. In particular, forward-or side-scatter between laser beams crossing at the laser entrance holes (LEH) of the hohlraum can lead to transfer of energy between cones of beams and affect the hohlraum radiation symmetry [2][3][4][5][6], while backscatter instabilities can cause an energy loss as well as an imbalance of the energy deposited onto the wall [7].…”
Section: Introductionmentioning
confidence: 99%
“…Crossed-beam energy transfer from the outer cones of laser beams (angles to hohlraum axis θ = 44.5 • and 50 • ) to inner cones (θ = 23.5 • and 30 • ) is needed to control implosion symmetry [6]. CBET is a form of stimulated Brillouin scatter where two light waves beat to drive an ion acoustic wave (IAW) which transfers energy to the light wave with lower frequency in the plasma frame [7]. Shots with high fill density have high inner-beam backward stimulated Raman scatter, or decay of a laser into a scattered light wave and LW.…”
mentioning
confidence: 99%
“…This ability to vary the inner cone fraction was successfully used to tune the implosion symmetry of the capsule [24]. It was predicted by Kruer et al [25] A. In our post-shot simulations of these experiments we now take account of the predicted power transfer in the following manner.…”
Section: Symmetrymentioning
confidence: 99%