2005
DOI: 10.1063/1.2133903
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X-ray imaging of cryogenic deuterium-tritium layers in a beryllium shell

Abstract: Solid deuterium-tritium (D-T) fuel layers inside copper-doped beryllium shells are robust inertial confinement fusion fuel pellets. This paper describes the first characterization of such layers using phase-contrast x-ray imaging. Good agreement is found between calculation and experimental contrast at the layer interfaces. Uniform solid D-T layers and their response to thermal asymmetries were measured in the Be(Cu) shell. The solid D-T redistribution time constant was measured to be 28 min in the Be(Cu) shel… Show more

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Cited by 39 publications
(18 citation statements)
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“…The direct-detection imaging using a micro-focus Cu anode x-ray source greatly improved upon earlier results using a scintillator for the imaging. [17] These recent images demonstrate that the surface roughness of the D-T layer can be accurately characterized using the x-ray phase-contrast enhanced imaging.…”
Section: Discussionmentioning
confidence: 99%
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“…The direct-detection imaging using a micro-focus Cu anode x-ray source greatly improved upon earlier results using a scintillator for the imaging. [17] These recent images demonstrate that the surface roughness of the D-T layer can be accurately characterized using the x-ray phase-contrast enhanced imaging.…”
Section: Discussionmentioning
confidence: 99%
“…A previous study with the same shell and a smaller epoxy joint had less power in the low modes. [17] The slope of the roughness power spectrum changes between modes 5 and 7 in the current data and indicates roughness dominated by the epoxy joint transitioning to the inherent surface roughness. Therefore, only modes greater than 7 will be included in the RMS sum and analysis.…”
Section: D-t Layer Roughnessmentioning
confidence: 99%
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“…Согласно измерениям [111] характерная константа времени выравнивания DT-слоя по толщине (в области, близкой к тройной точке) составляет 28 мин. Однако поскольку процесс выравнивания слоя происходит с экспоненциальным затуханием, то полное время получения слоя с разнотолщинностью менее 1% составляет около суток.…”
Section: проблема сохранения качества топливной мишениunclassified