2010
DOI: 10.1088/1742-6596/244/3/032003
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Progress on converting a NIF quad to eight, petawatt beams for advanced radiography

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Cited by 70 publications
(22 citation statements)
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“…Such a laser would produce about 100 times more positrons and 10 times more electrons than current facilities, and these higher yields would be comparable to those needed for laboratory astrophysics experiments. And in fact, a new generation of intense high energy lasers, including NIF ARC, 43 Gekko LFEX, 44 and LMJ PETAL, 45 is being constructed to deliver about 10 kJ at 1-10 ps pulse durations. These are expected to be available for experiments in the next few years.…”
Section: Future Researchmentioning
confidence: 99%
“…Such a laser would produce about 100 times more positrons and 10 times more electrons than current facilities, and these higher yields would be comparable to those needed for laboratory astrophysics experiments. And in fact, a new generation of intense high energy lasers, including NIF ARC, 43 Gekko LFEX, 44 and LMJ PETAL, 45 is being constructed to deliver about 10 kJ at 1-10 ps pulse durations. These are expected to be available for experiments in the next few years.…”
Section: Future Researchmentioning
confidence: 99%
“…Figure 6 shows a possible implementation of implosion transmission radiography on NIF using twin ARIANE detectors to record signals from two backlight sources separated by 200ps along with simulated radiographs assuming 20µm spatial resolution, 10ps temporal resolution, and expected noise. The backlighters will be produced by the NIF Advanced Radiographic Capability (ARC), a dedicated subset of beams that will have capability of generating intensities of 10 18 W/cm 2 [23]. A collimator will be used to isolate x-rays from each of the two backlight sources, and an ARIANE detector with a single-strip MCP will be located along each of the two lines of sight.…”
Section: Areal Density Measurements With Transmission Compton Radiogrmentioning
confidence: 99%
“…The longitudinal spatial shifts between the gratings of the independent compressors [6] avoid spectral coupling between gratings. In this scheme, the beam shaping (band gap without energy to avoid spectral coupling) is limited compared to mosaic gratings [12,13]. This beam shaping is only made to limit energy on the edge of the components.…”
Section: Specificitions For the Petal Schemementioning
confidence: 99%