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Magnetic field effects on laser energy deposition and filamentation in magneto-inertial fusion relevant plasmas

Physics of Plasmas

Lewis, S.M.; Weis, Matthew R.; Speas, Christopher S.; Kimmel, Mark W.; Bengtson, R.D.; Breizman, B.; Geissel, Matthias G.; Gomez, Matthew R.; Harvey-Thompson, Adam J.; Kellogg, Jeffrey W.; Long, Joel L.; Quevedo, H.J.; Rambo, Patrick K.; Riley, N.R.; Schwarz, Jens S.; Shores, Jonathon S.; Stahoviak, J.; Ampleford, David A.; Porter, John L.; Ditmire, T.; Looker, Quinn M.; Struve, Kenneth W.

We report on experimental measurements of how an externally imposed magnetic field affects plasma heating by kJ-class, nanosecond laser pulses. The experiments reported here took place in gas cells analogous to magnetized liner inertial fusion targets. We observed significant changes in laser propagation and energy deposition scale lengths when a 12T external magnetic field was imposed in the gas cell. We find evidence that the axial magnetic field reduces radial electron thermal transport, narrows the width of the heated plasma, and increases the axial plasma length. Reduced thermal conductivity increases radial thermal gradients. This enhances radial hydrodynamic expansion and subsequent thermal self-focusing. Our experiments and supporting 3D simulations in helium demonstrate that magnetization leads to higher thermal gradients, higher peak temperatures, more rapid blast wave development, and beam focusing with an applied field of 12T.

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X-Ray Diffraction Measurements on Laser-Compressed Polycrystalline Samples Using a Short-Pulse Laser Generated X-Ray Source

Schollmeier, Marius; Ao, Tommy A.; Field, Ella S.; Galloway, B.R.; Laros, James H.; Kimmel, Mark W.; Long, Joel L.; Morgan, Dane V.; Rambo, Patrick K.; Schwarz, Jens S.; Seagle, Christopher T.

Existing models for most materials do not describe phase transformations and associated lattice dy- namics (kinetics) under extreme conditions of pressure and temperature. Dynamic x-ray diffraction (DXRD) allows material investigations in situ on an atomic scale due to the correlation between solid-state structures and their associated diffraction patterns. In this LDRD project we have devel- oped a nanosecond laser-compression and picosecond-to-nanosecond x-ray diffraction platform for dynamically-compressed material studies. A new target chamber in the Target Bay in building 983 was commissioned for the ns, kJ Z-Beamlet laser (ZBL) and the 0.1 ns, 250 J Z-Petawatt (ZPW) laser systems, which were used to create 8-16 keV plasma x-ray sources from thin metal foils. The 5 ns, 15 J Chaco laser system was converted to a high-energy laser shock driver to load material samples to GPa stresses. Since laser-to-x-ray energy conversion efficiency above 10 keV is low, we employed polycapillary x-ray lenses for a 100-fold fluence increase compared to a conventional pinhole aperture while simultaneously reducing the background significantly. Polycapillary lenses enabled diffraction measurements up to 16 keV with ZBL as well as diffraction experiments with ZPW. This x-ray diffraction platform supports experiments that are complementary to gas guns and the Z facility due to different strain rates. Ultimately, there is now a foundation to evaluate DXRD techniques and detectors in-house before transferring the technology to Z. This page intentionally left blank.

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An overview of the ultra-fast X-ray imager (UXI) program at Sandia Labs

Proceedings of SPIE - The International Society for Optical Engineering

Claus, Liam D.; Fang, Lu F.; Kay, Randolph R.; Kimmel, Mark W.; Long, Joel L.; Porter, John L.; Robertson, Gideon R.; Sanchez, Marcos O.; Stahoviak, John W.; Trotter, Douglas C.

The Ultra-Fast X-ray Imager (UXI) program is an ongoing effort at Sandia National Laboratories to create high speed, multi-frame, time gated Read Out Integrated Circuits (ROICs), and a corresponding suite of photodetectors to image a wide variety of High Energy Density (HED) physics experiments on both Sandia's Z-Machine and the National Ignition Facility (NIF). The program is currently fielding a 1024 x 448 prototype camera with 25 μm pixel spatial resolution, 2 frames of in-pixel storage and the possibility of exchanging spatial resolution to achieve 4 or 8 frames of storage. The camera's minimum integration time is 2 ns. Minimum signal target is 1500 e-rms and full well is 1.5 million e-. The design and initial characterization results will be presented as well as a description of future imagers.

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12 Results
12 Results