2022
DOI: 10.1103/physreve.105.045208
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Suprathermal electrons from the anti-Stokes Langmuir decay instability cascade

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Cited by 5 publications
(4 citation statements)
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References 53 publications
(89 reference statements)
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“…It can also be seen that SRBS bursts at points a and d, wave-breaking and other nonlinear effects play a vital role in this phenomenon. The maximum value of the EPW field can be obtained by Coffey's warm nonrelativistic wave breaking limit, where β = 3v 2 te /v 2 ϕ , and v te , ω pe are the electron thermal velocity and plasma frequency, respectively [39]. From equation ( 11), E max depends on the plasma density and electron temperature, and becomes lower when the density decreases.…”
Section: Electric-field Characteristics Of Srsmentioning
confidence: 99%
“…It can also be seen that SRBS bursts at points a and d, wave-breaking and other nonlinear effects play a vital role in this phenomenon. The maximum value of the EPW field can be obtained by Coffey's warm nonrelativistic wave breaking limit, where β = 3v 2 te /v 2 ϕ , and v te , ω pe are the electron thermal velocity and plasma frequency, respectively [39]. From equation ( 11), E max depends on the plasma density and electron temperature, and becomes lower when the density decreases.…”
Section: Electric-field Characteristics Of Srsmentioning
confidence: 99%
“…It was found that the SRS rescattering can fill this phase velocity gap [23] and hot electrons can be produced through the interaction of a discrete spectrum of plasma waves generated from BSRS, FSRS, and rescattering. In addition, it was found that the LDI [24,25] and anti-Stokes LDI (ALDI) [26,27] following BSRS can heat electrons to higher energies because the EPW from the LDI has a slightly higher phase velocity. In order to provide overlapped trapping regions for different EPWs in their phase velocities, this cascade acceleration often imposes high demands on the electron density.…”
Section: Introductionmentioning
confidence: 99%
“…Two are currently the most actively pursued of many proposed routes to ICF: the indirect-drive approach [2], where the laser energy is first converted into x-rays that then go on to drive the compression of a spherical deuterium-tritium fuel capsule, and the direct drive scheme [3], where the laser beams irradiate and thereby compress, the fuel capsule directly. Both systems depend heavily on laser-plasma interactions (LPI) [4,5], which can degrade implosion output by lowering laser coupling to the target, increasing drive asymmetries, and preheating the fuel by producing and depositing suprathermal electrons. Cross-beam energy transfer (CBET), stimulated Brillouin scattering (SBS) [5][6][7][8], and stimulated Raman scattering (SRS) [9][10][11] are examples of laser plasma instabilities that prevent the development of the necessary time-dependent drivesymmetry in ICF.…”
Section: Introductionmentioning
confidence: 99%