Spectroscopic studies of shell mix in directly driven implosion on SGIII prototype laser facility

We study shell mix during implosion using a capsule with a Cl-doped gas-shell interface that is also filled with Ar-doped deuterium gas. The Ar and Cl K-shell emissions are recorded with a flat crystal spectrometer. The He-β complex is analyzed to infer the electron temperature and density in the ho...

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Veröffentlicht in:Physics of plasmas 2014-12, Vol.21 (12)
Hauptverfasser: Pu, Yudong, Huang, Tianxuan, Wei, Minxi, Tang, Qi, Song, Zifeng, Yang, Jiamin, Liu, Shenye, Jiang, Shaoen, Ding, Yongkun
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container_end_page
container_issue 12
container_start_page
container_title Physics of plasmas
container_volume 21
creator Pu, Yudong
Huang, Tianxuan
Wei, Minxi
Tang, Qi
Song, Zifeng
Yang, Jiamin
Liu, Shenye
Jiang, Shaoen
Ding, Yongkun
description We study shell mix during implosion using a capsule with a Cl-doped gas-shell interface that is also filled with Ar-doped deuterium gas. The Ar and Cl K-shell emissions are recorded with a flat crystal spectrometer. The He-β complex is analyzed to infer the electron temperature and density in the hotspot. Two regions of different hydrodynamic states are observed: a region of Te ∼ 1.2 ± 0.2 keV and ne ∼ (4 ± 0.5) × 1023 cm−3 and another of Te ∼ 0.6 ± 0.2 keV and ne ∼ (4 ± 0.5) × 1022 cm−3 probed by Ar and Cl ions, respectively. The neutron yield was also recorded and found to have reduced by a factor of ten for the Cl-doped capsule. By attributing the degradation of the neutron yield to the enhanced radiation loss due to the presence of mixed Cl ions and using the conservation of hotspot internal energy, the amount of mixed Cl ions is estimated to be ∼1.4 × 1014, corresponding to a 0.1 μm thickness of the initial shell material and a mixing width of about 16 μm.
doi_str_mv 10.1063/1.4904041
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The Ar and Cl K-shell emissions are recorded with a flat crystal spectrometer. The He-β complex is analyzed to infer the electron temperature and density in the hotspot. Two regions of different hydrodynamic states are observed: a region of Te ∼ 1.2 ± 0.2 keV and ne ∼ (4 ± 0.5) × 1023 cm−3 and another of Te ∼ 0.6 ± 0.2 keV and ne ∼ (4 ± 0.5) × 1022 cm−3 probed by Ar and Cl ions, respectively. The neutron yield was also recorded and found to have reduced by a factor of ten for the Cl-doped capsule. By attributing the degradation of the neutron yield to the enhanced radiation loss due to the presence of mixed Cl ions and using the conservation of hotspot internal energy, the amount of mixed Cl ions is estimated to be ∼1.4 × 1014, corresponding to a 0.1 μm thickness of the initial shell material and a mixing width of about 16 μm.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.4904041</doi></addata></record>
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subjects 70 PLASMA PHYSICS AND FUSION TECHNOLOGY
ARGON IONS
CAPSULES
CHLORINE IONS
DEUTERIUM
DOPED MATERIALS
Electron energy
ELECTRON TEMPERATURE
Energy conservation
ENERGY LOSSES
HELIUM COMPLEXES
IMPLOSIONS
Internal energy
K SHELL
KEV RANGE
LASERS
NEUTRONS
Plasma physics
SPECTROMETERS
SPECTROSCOPY
THICKNESS
title Spectroscopic studies of shell mix in directly driven implosion on SGIII prototype laser facility
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