2019
DOI: 10.1038/s41567-019-0725-z
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Impact of the Langdon effect on crossed-beam energy transfer

Abstract: The prediction that laser plasma heating distorts the electron distribution function away from Maxwellian and towards a super-Gaussian distribution dates back four decades [1]. In conditions relevant to inertial confinement fusion, however, no direct evidence of this so-called "Langdon effect" has previously been observed. Here, measurements of the spatially and temporally resolved Thomson scattering spectrum indicate the presence of super-Gaussian electron distribution functions that are consistent with exist… Show more

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Cited by 49 publications
(15 citation statements)
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“…K designates a kinetic plasma response function that depends on the k-vectors of the respective ray fields, the hydrodynamic parameters, and the total laser intensity through the Langdon parameter α in case of non-Maxwellian distribution functions (see Refs. [9] and [18]). The χ i, j coefficient in Eq.…”
Section: Cross Beam Energy Transfer Modelingmentioning
confidence: 98%
“…K designates a kinetic plasma response function that depends on the k-vectors of the respective ray fields, the hydrodynamic parameters, and the total laser intensity through the Langdon parameter α in case of non-Maxwellian distribution functions (see Refs. [9] and [18]). The χ i, j coefficient in Eq.…”
Section: Cross Beam Energy Transfer Modelingmentioning
confidence: 98%
“…While these techniques are still under development, they are already implemented in three-dimensional hydrodynamic codes and used for interpretation of experiments [24]. The latter approach shows a significant improvement in description of the cross beam energy transfer [25]. Other processes such as temporal and spatial laser beam smoothing in plasma, resonance absorption, excitation of SRS and TPD instabilities and generation of hot electrons can be also accounted for [26].…”
Section: (A) Physics Of Laser Plasma Interaction Under Shock Ignitionmentioning
confidence: 99%
“…In addition to the plasma source, a tunable (351 nm ± 1.5 nm) independent beam from OMEGA EP has been transported to the OMEGA-60 target chamber [46]. Initial experiments have used this tunable OMEGA Port 9 (TOP9) beam to study CBET in a stationary plasma [47]. This novel experimental platform is shown in figure 16.…”
Section: Laser–plasma Interaction Researchmentioning
confidence: 99%