T. C. Moore
Sandia National Laboratories
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Featured researches published by T. C. Moore.
Physical Review Letters | 2004
J. E. Bailey; Gordon Andrew Chandler; Stephen A. Slutz; Igor E. Golovkin; P. Lake; J. J. MacFarlane; R. C. Mancini; T.J. Burris-Mog; G. W. Cooper; R. J. Leeper; Thomas Alan Mehlhorn; T. C. Moore; T. J. Nash; Nielsen Ds; C. L. Ruiz; D. G. Schroen; W. Varnum
Hot dense capsule implosions driven by Z-pinch x rays have been measured using a approximately 220 eV dynamic Hohlraum to implode 1.7-2.1 mm diameter gas-filled CH capsules. The capsules absorbed up to approximately 20 kJ of x rays. Argon tracer atom spectra were used to measure the T(e) approximately 1 keV electron temperature and the n(e) approximately 1-4 x 10(23) cm(-3) electron density. Spectra from multiple directions provide core symmetry estimates. Computer simulations agree well with the peak emission values of T(e), n(e), and symmetry, indicating reasonable understanding of the Hohlraum and implosion physics.
Physics of Plasmas | 2003
Stephen A. Slutz; J. E. Bailey; Gordon Andrew Chandler; Guy R. Bennett; G. W. Cooper; Joel Staton Lash; S. Lazier; P. Lake; R.W. Lemke; Thomas Alan Mehlhorn; T. J. Nash; D. S. Nielson; J. McGurn; T. C. Moore; C. L. Ruiz; Diana Grace Schroen; J. Torres; W. Varnum; Roger Alan Vesey
A dynamic hohlraum is formed when an imploding annular cylindrical Z-pinch driven plasma collides with an internal low density convertor. This collision generates an inward traveling shock wave that emits x rays, which are trapped by the optically thick Z-pinch plasma and can be used to drive an inertial fusion capsule embedded in the convertor. This scheme has the potential to efficiently drive high yield capsules due to the close coupling between the intense radiation generation and the capsule. In prior dynamic hohlraum experiments [J. E. Bailey et al., Phys. Rev Lett. 89, 095004 (2002)] the convertor shock wave has been imaged with gated x-ray pinhole cameras. The shock emission was observed to be very circular and to be quite narrow in the radial direction. This implies that there is minimal Rayleigh–Taylor imprinting on the shock wave. Thus, the dominant source of radiation asymmetry is not random and in principle could be significantly decreased by proper design. Due to the closed geometry of the d...
Physics of Plasmas | 2006
J. E. Bailey; Gordon Andrew Chandler; R. C. Mancini; Stephen A. Slutz; Gregory A. Rochau; M. Bump; T. J. Buris-Mog; G. W. Cooper; G. Dunham; Igor E. Golovkin; J. D. Kilkenny; P. Lake; R. J. Leeper; R.W. Lemke; J. J. MacFarlane; Thomas Alan Mehlhorn; T. C. Moore; T. J. Nash; A. Nikroo; Dan S. Nielsen; K. L. Peterson; C. L. Ruiz; D. G. Schroen; D. Steinman; W. Varnum
Z-pinch dynamic hohlraums are a promising indirect-drive inertial confinement fusion approach. Comparison of multiple experimental methods with integrated Z-pinch∕hohlraum∕capsule computer simulations builds understanding of the hohlraum interior conditions. Time-resolved x-ray images determine the motion of the radiating shock that heats the hohlraum as it propagates toward the hohlraum axis. The images also measure the radius of radiation-driven capsules as they implode. Dynamic hohlraum LASNEX [G. Zimmerman and W. Kruer, Comments Plasma Phys. Control. Fusion 2, 85 (1975)] simulations are found to overpredict the shock velocity by ∼20–40%, but simulated capsule implosion trajectories agree reasonably well with the data. Measurements of the capsule implosion core conditions using time- and space-resolved Ar tracer x-ray spectroscopy and the fusion neutron yield provide additional tests of the integrated hohlraum-implosion system understanding. The neutron yield in the highest performing CH capsule implos...
Review of Scientific Instruments | 2004
P. Lake; J. E. Bailey; G. A. Rochau; T. C. Moore; D. Petmecky; P. Gard
X-ray spectrometers used in high energy density plasma experiments must provide high time, space, and spectral resolution while overcoming the difficulties imposed by x-ray background, debris, and mechanical shocks. At the Z facility these problems are addressed using a suite of elliptical crystal spectrometers. The elliptical geometry isolates the detector from the line of sight with a slit placed at the elliptical focus, while the sensitivity enables locating the crystal 2–4 m from the plasma source. Space and time resolution are obtained by using an array of slits to project one dimensional plasma images onto the crystal and recording the spectrally dispersed images with a gated microchannel plate detector.
Physics of Plasmas | 2004
T. J. Nash; C. Deeney; Gordon Andrew Chandler; Daniel Brian Sinars; M. E. Cuneo; E.M. Waisman; W. A. Stygar; David Franklin Wenger; S. Speas; R. J. Leeper; J. F. Seaman; J. McGurn; J. Torres; D. Jobe; T. Gilliland; Dan S. Nielsen; R. Hawn; H. Seaman; K. Keller; T. C. Moore; Tim C. Wagoner; P. D. LePell; J. Lucas; Diana Grace Schroen; C. Russell; M. Kernaghan
Results from the first solid foil implosion on the 18-MA Z accelerator are reported. The foil implosion is compared to a 300-wire-array implosion with the same material and the same diameter, height, and total mass. Though both the foil and the array produced comparable x-ray yields, the array’s radiation burst was twice as powerful and half as long as the foil’s. These data along with x-ray backlighting images and inductance measurements suggest that the foil implosion was more unstable than the wire-array implosion.
Physics of Plasmas | 2004
T. J. Nash; M. E. Cuneo; Rick B. Spielman; Gordon Andrew Chandler; R. J. Leeper; J. F. Seaman; J. McGurn; S. Lazier; J. Torres; D. Jobe; T. Gilliland; Dan S. Nielsen; R. Hawn; J. E. Bailey; P. Lake; A.L. Carlson; Hans Seamen; T. C. Moore; R. Smelser; J. Pyle; Tim C. Wagoner; P. D. LePell; C. Deeney; M.R. Douglas; D. H. McDaniel; K.W. Struve; M.G. Mazarakis; W. A. Stygar
In order to estimate the radiated power that can be expected from the next-generation Z-pinch driver such as ZR at 28 MA, current-scaling experiments have been conducted on the 20 MA driver Z. We report on the current scaling of single 40 mm diameter tungsten 240 wire arrays with a fixed 110 ns implosion time. The wire diameter is decreased in proportion to the load current. Reducing the charge voltage on the Marx banks reduces the load current. On one shot, firing only three of the four levels of the Z machine further reduced the load current. The radiated energy scaled as the current squared as expected but the radiated power scaled as the current to the 3.52±0.42 power due to increased x-ray pulse width at lower current. As the current is reduced, the rise time of the x-ray pulse increases and at the lowest current value of 10.4 MA, a shoulder appears on the leading edge of the x-ray pulse. In order to determine the nature of the plasma producing the leading edge of the x-ray pulse at low currents furt...
Review of Scientific Instruments | 2006
P. Lake; J. E. Bailey; G. A. Rochau; P. Gard; D. Petmecky; M. Bump; N. R. Joseph; T. C. Moore; L. B. Nielsen-Weber
Elliptical crystal spectrometers equipped with time-gated microchannel plate (MCP) detectors provide time-, space-, and spectrally resolved data. A common problem is that the number of time resolution elements is limited by the number of MCP frames. The number of frames that fit on a given MCP is limited by the image size and the alignment tolerance. At the Z facility these problems have been addressed with twin-elliptical-crystal spectrometers. Using two crystals and detectors doubles the number of frames available. This enables measurements with ∼350ps time resolution while still recording data from an ∼4ns wide time window. Alternatively, the twin crystal design allows simultaneous measurements with different crystals to investigate different spectral regimes.
Review of Scientific Instruments | 2006
T. J. Nash; Gordon Andrew Chandler; J. E. Bailey; G. A. Rochau; R. J. Leeper; Dan S. Nielsen; T. C. Moore
An on-axis time-resolved x-ray pinhole camera has been used on the 20MA 100ns driver Z to image the converging shock wave in dynamic Hohlraum experiments and to image pellet hot spots in inertial confinement fusion implosions. This instrument is susceptible to detecting significant amounts of pinch bremsstrahlung radiation with energies at hundreds of keV and yields of roughly 1kJ. Quite often the bremsstrahlung noise signals have overwhelmed the desired x-ray images. In an effort to eliminate this large source of noise we have incorporated a 6° gold-coated grazing incidence mirror into the time-resolved x-ray pinhole camera system. The mirror reflects soft x rays at energies under 2keV but does not reflect bremsstrahlung radiation at hundreds of keV. We will present data from the instrument without the mirror showing large amounts of bremsstrahlung noise contamination and data with the mirror in the system showing greatly reduced noise levels.
Physical Review Letters | 2007
J. E. Bailey; G. A. Rochau; Carlos A. Iglesias; J. Abdallah; J. J. MacFarlane; Igor E. Golovkin; P. Wang; R. C. Mancini; P. Lake; T. C. Moore; M. Bump; O. Garcia; S. Mazevet
Physical Review Letters | 2002
J. E. Bailey; Gordon Andrew Chandler; Stephen A. Slutz; Guy R. Bennett; G. W. Cooper; Joel Staton Lash; S. Lazier; R.W. Lemke; T. J. Nash; Nielsen Ds; T. C. Moore; C. L. Ruiz; D. G. Schroen; R. M. Smelser; J. Torres; Roger Alan Vesey