Pulse Shape 22: Audiovisual Performance and Data Transmutation

Leonardo ◽  
2016 ◽  
Vol 49 (4) ◽  
pp. 317-323
Author(s):  
Mark Cetilia

Pulse Shape 22 is an improvisational audiovisual performance featuring shortwave radio transmissions as the sole source material for real-time audio processing alongside video of the sun projected through cast-glass lenses designed specifically for this piece. The structure of the piece is derived from metrics on energy accumulation over a period of 2.2 nanoseconds resulting from the targeting of 60 laser beams on a single tetrahedral hohlraum in weapons testing experiments as carried out by the Los Alamos Inertial Confinement Fusion unit, at the Omega Laser Facility at the University of Rochester. Pulse Shape 22 is an exploration of architectural space through the use of site- and time-specific information found in regions of the electromagnetic spectrum outside the reaches of the human sensory apparatus. It is an attempt to alter the audience’s perceptions of their surroundings and create a moment of rupture from hidden worlds found in our local environment.

2011 ◽  
Vol 39 (4) ◽  
pp. 1007-1014 ◽  
Author(s):  
P B Radha ◽  
R Betti ◽  
T R Boehly ◽  
J A Delettrez ◽  
D H Edgell ◽  
...  

1993 ◽  
Vol 11 (2) ◽  
pp. 317-321 ◽  
Author(s):  
J.M. Soures ◽  
R.L. McCrory ◽  
T.R. Boehly ◽  
R.S. Craxton ◽  
S.D. Jacobs ◽  
...  

Validation of the direct-drive approach to inertial confinement fusion requires the development of a 351-nm wavelength, 30-kJ, 50-TW laser system with flexible pulse shaping and irradiation uniformity approaching 1%. An upgrade of the existing OMEGA direct-drive facility at Rochester is planned to meet these objectives. In this article, we review the design rationale and specifications of the OMEGA Upgrade laser with particular emphasis on techniques planned to achieve the required degree of beam smoothing, temporal pulse shape, and beam-to-beam power balance.


2014 ◽  
Vol 31 (4) ◽  
pp. 045201 ◽  
Author(s):  
Li-Feng Wang ◽  
Jun-Feng Wu ◽  
Wen-Hua Ye ◽  
Zheng-Feng Fan ◽  
Xian-Tu He

2009 ◽  
Vol 27 (1) ◽  
pp. 123-127 ◽  
Author(s):  
A. Seifter ◽  
G.A. Kyrala ◽  
S.R. Goldman ◽  
N.M. Hoffman ◽  
J.L. Kline ◽  
...  

AbstractImplosions using inertial confinement fusion must be highly symmetric to achieve ignition on the National Ignition Facility. This requires precise control of the drive symmetry from the radiation incident on the ignition capsule. For indirect drive implosions, low mode residual perturbations in the drive are generated by the laser-heated hohlraum geometry. To diagnose the drive symmetry, previous experiments used simulated capsules by which the self-emission X-rays from gas in the center of the capsule during the implosion are used to infer the shape of the drive. However, those experiments used hohlraum radiation temperatures higher than 200 eV (Hauer et al., 1995; Murphy et al., 1998a, 1998b) with small NOVA scale hohlraums under which conditions the symcaps produced large X-ray signals. At the foot of the NIF ignition pulse, where controlling the symmetry has been shown to be crucial for obtaining a symmetric implosion (Clark et al., 2008), the radiation drive is much smaller, reducing the X-ray emission from the imploded capsule. For the first time, the feasibility of using symcaps to diagnose the radiation drive for low radiation temperatures, <120 eV and large 0.7 linear scales NIF Rev3.1 (Haan et al., 2008) vacuum hohlraums is demonstrated. Here we used experiments at the Omega laser facility to demonstrate and develop the symcap technique for tuning the symmetry of the NIF ignition capsule in the foot of the drive pulse.


2012 ◽  
Vol 19 (5) ◽  
pp. 056306 ◽  
Author(s):  
M. Hohenberger ◽  
P.-Y. Chang ◽  
G. Fiksel ◽  
J. P. Knauer ◽  
R. Betti ◽  
...  

1991 ◽  
Vol 9 (2) ◽  
pp. 297-307 ◽  
Author(s):  
W. H. Lowdermilk

The design for an advanced, flash-lamp-pumped Nd: glass laser for inertial confinement fusion (ICF) research and applications is summarized. The laser consists of multiple beam lines, each of which delivers 145-kJ, O.35-μm, 8-ns laser pulses, with pulse shape and bandwidth capabilities consistent with requirements for driving ICF capsules to high gain.


Author(s):  
C. W. Price ◽  
E. F. Lindsey

Thickness measurements of thin films are performed by both energy-dispersive x-ray spectroscopy (EDS) and x-ray fluorescence (XRF). XRF can measure thicker films than EDS, and XRF measurements also have somewhat greater precision than EDS measurements. However, small components with curved or irregular shapes that are used for various applications in the the Inertial Confinement Fusion program at LLNL present geometrical problems that are not conducive to XRF analyses but may have only a minimal effect on EDS analyses. This work describes the development of an EDS technique to measure the thickness of electroless nickel deposits on gold substrates. Although elaborate correction techniques have been developed for thin-film measurements by x-ray analysis, the thickness of electroless nickel films can be dependent on the plating bath used. Therefore, standard calibration curves were established by correlating EDS data with thickness measurements that were obtained by contact profilometry.


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