A. Warrick
Lawrence Livermore National Laboratory
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Physics of Plasmas | 2010
N. B. Meezan; L. J. Atherton; D. A. Callahan; E. L. Dewald; S. Dixit; E. G. Dzenitis; M. J. Edwards; C. A. Haynam; D. E. Hinkel; O. S. Jones; O. L. Landen; Richard A. London; P. Michel; J. D. Moody; J. L. Milovich; M. B. Schneider; C. A. Thomas; R. P. J. Town; A. Warrick; S. V. Weber; K. Widmann; S. H. Glenzer; L. J. Suter; B. J. MacGowan; J. L. Kline; George A. Kyrala; A. Nikroo
The first series of experiments of the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)] tested ignition Hohlraum “energetics,” a term described by four broad goals: (1) measurement of laser absorption by the Hohlraum; (2) measurement of the x-ray radiation flux (TRAD4) on the surrogate ignition capsule; (3) quantitative understanding of the laser absorption and resultant x-ray flux; and (4) determining whether initial Hohlraum performance is consistent with requirements for ignition. This paper summarizes the status of NIF Hohlraum energetics experiments. The Hohlraum targets and experimental design are described, as well as the results of the initial experiments. The data demonstrate low backscattered energy (<10%) for Hohlraums filled with helium gas. A discussion of our current understanding of NIF Hohlraum x-ray drive follows, including an overview of the computational tools, i.e., radiation-hydrodynamics codes that have been used to design the Hohlraums. The perf...
Review of Scientific Instruments | 2010
J. L. Kline; K. Widmann; A. Warrick; R.E. Olson; C. A. Thomas; A. S. Moore; L. J. Suter; O. L. Landen; D. A. Callahan; S. Azevedo; J. Liebman; S. H. Glenzer; A. D. Conder; S. Dixit; P. Torres; V. Tran; E. L. Dewald; J. Kamperschroer; L. J. Atherton; R. Beeler; L. V. Berzins; J. Celeste; C. A. Haynam; W. W. Hsing; D. W. Larson; B. J. MacGowan; D. E. Hinkel; D. H. Kalantar; R. L. Kauffman; J. D. Kilkenny
The first 96 and 192 beam vacuum Hohlraum target experiments have been fielded at the National Ignition Facility demonstrating radiation temperatures up to 340 eV and fluxes of 20 TW/sr as viewed by DANTE representing an ∼20u2002times flux increase over NOVA/Omega scale Hohlraums. The vacuum Hohlraums were irradiated with 2 ns square laser pulses with energies between 150 and 635 kJ. They produced nearly Planckian spectra with about 30±10% more flux than predicted by the preshot radiation hydrodynamic simulations. To validate these results, careful verification of all component calibrations, cable deconvolution, and software analysis routines has been conducted. In addition, a half Hohlraum experiment was conducted using a single 2 ns long axial quad with an irradiance of ∼2×10(15)u2002W/cm(2) for comparison with NIF Early Light experiments completed in 2004. We have also completed a conversion efficiency test using a 128-beam nearly uniformly illuminated gold sphere with intensities kept low (at 1×10(14)u2002W/cm(2) over 5 ns) to avoid sensitivity to modeling uncertainties for nonlocal heat conduction and nonlinear absorption mechanisms, to compare with similar intensity, 3 ns OMEGA sphere results. The 2004 and 2009 NIF half-Hohlraums agreed to 10% in flux, but more importantly, the 2006 OMEGA Au Sphere, the 2009 NIF Au sphere, and the calculated Au conversion efficiency agree to ±5% in flux, which is estimated to be the absolute calibration accuracy of the DANTEs. Hence we conclude that the 30±10% higher than expected radiation fluxes from the 96 and 192 beam vacuum Hohlraums are attributable to differences in physics of the larger Hohlraums.
Review of Scientific Instruments | 2010
M. B. Schneider; O. S. Jones; N. B. Meezan; J. L. Milovich; R. P. J. Town; S. S. Alvarez; R. G. Beeler; D. K. Bradley; J. Celeste; S. Dixit; M. J. Edwards; M. J. Haugh; D. H. Kalantar; J. L. Kline; G. A. Kyrala; O. L. Landen; B. J. MacGowan; P. Michel; J. D. Moody; S. K. Oberhelman; K. Piston; Michael J. Pivovaroff; L. J. Suter; A. Teruya; C. A. Thomas; Stephen P. Vernon; A. Warrick; K. Widmann; R. D. Wood; B. K. Young
The static x-ray imager at the National Ignition Facility is a pinhole camera using a CCD detector to obtain images of Hohlraum wall x-ray drive illumination patterns seen through the laser entrance hole (LEH). Carefully chosen filters, combined with the CCD response, allow recording images in the x-ray range of 3-5 keV with 60u2002μm spatial resolution. The routines used to obtain the apparent size of the backlit LEH and the location and intensity of beam spots are discussed and compared to predictions. A new soft x-ray channel centered at 870 eV (near the x-ray peak of a 300 eV temperature ignition Hohlraum) is discussed.
Physics of Plasmas | 2012
R. E. Olson; L. J. Suter; J. L. Kline; D. A. Callahan; M. D. Rosen; S. N. Dixit; O. L. Landen; N. B. Meezan; J. D. Moody; C. A. Thomas; A. Warrick; K. Widmann; E. A. Williams; S. H. Glenzer
X-ray fluxes measured in the first 96 and 192 beam vacuum hohlraum experiments at the National Ignition Facility (NIF) were significantly higher than predicted by computational simulations employing XSN average atom atomic physics and highly flux-limited electron heat conduction. For agreement with experimental data, it was found that the coronal plasma emissivity must be simulated with a detailed configuration accounting model that accounts for x-ray emission involving all of the significant ionization states. It was also found that an electron heat conduction flux limit of f = 0.05 is too restrictive, and that a flux limit of f = 0.15 results in a much better match with the NIF vacuum hohlraum experimental data. The combination of increased plasma emissivity and increased electron heat conduction in this new high flux hohlraum model results in a reduction in coronal plasma energy and, hence, an explanation for the high (∼85%-90%) x-ray conversion efficiencies observed in the 235u2009<u2009Tru2009<u2009345 eV NIF vacuum...
Physics of Plasmas | 2005
D. E. Hinkel; M. B. Schneider; H. A. Baldis; G. Bonanno; Dan E. Bower; K. M. Campbell; J. Celeste; S. Compton; R. Costa; E. L. Dewald; S. Dixit; Mark J. Eckart; David C. Eder; M. J. Edwards; A.D. Ellis; J.A. Emig; D. H. Froula; S. H. Glenzer; D. Hargrove; C. A. Haynam; R. F. Heeter; M.A. Henesian; J. P. Holder; G. Holtmeier; L. James; D. H. Kalantar; J. Kamperschroer; R. L. Kauffman; J. R. Kimbrough; R. K. Kirkwood
A platform for analysis of material properties under extreme conditions, where a sample is bathed in radiation with a high temperature, is under development. Depositing maximum laser energy into a small, high-Z enclosure produces this hot environment. Such targets were recently included in an experimental campaign using the first four of the 192 beams of the National Ignition Facility [J. A. Paisner, E. M. Campbell, and W. J. Hogan, Fusion Technol. 26, 755 (1994)], under construction at the University of California Lawrence Livermore National Laboratory. These targets demonstrate good laser coupling, reaching a radiation temperature of 340 eV. In addition, there is a unique wavelength dependence of the Raman backscattered light that is consistent with Brillouin backscatter of Raman forward scatter [A. B. Langdon and D. E. Hinkel, Phys. Rev. Lett. 89, 015003 (2002)]. Finally, novel diagnostic capabilities indicate that 20% of the direct backscatter from these reduced-scale targets is in the polarization or...
Review of Scientific Instruments | 2004
Dan E. Bower; T. McCarville; S. S. Alvarez; L. E. Ault; M. D. Brown; M. Chrisp; C. M. Damian; W. J. DeHope; D. H. Froula; S. H. Glenzer; S. Grace; K. Gu; F. R. Holdener; C. K. Huffer; J. Kamperschroer; T. Kelleher; J. R. Kimbrough; R. K. Kirkwood; D. W. Kurita; A. Lee; F. D. Lee; I. T. Lewis; F. J. Lopez; B. J. MacGowan; M. Poole; M. Rhodes; M. B. Schneider; Noel R. Sewall; F. Y. Shimamoto; S. Shiromizu
A full aperture backscatter station (FABS) target diagnostic has been activated on the first four beams of the National Ignition Facility. FABS measures both stimulated Brillouin scattering and stimulated Raman scattering with a suite of measurement instruments. Digital cameras and spectrometers record spectrally resolved energy for both P and S polarized light. Streaked spectrometers measure the spectral and temporal behavior of the backscattered light. Calorimeters and fast photodetectors measure the integrated energy and temporal behavior of the light, respectively. This article provides an overview of the FABS measurement system and detailed descriptions of the diagnostic instruments and the optical path.
Journal of Physics: Conference Series | 2010
R.E. Olson; L. J. Suter; J. L. Kline; D. A. Callahan; M. D. Rosen; K. Widmann; E. A. Williams; D. E. Hinkel; N. B. Meezan; G. A. Rochau; A. Warrick; S. H. Langer; C. A. Thomas; S. Dixit; E. L. Dewald; M. B. Schneider; J. D. Moody; P. Michel; R. J. Wallace; O. L. Landen; John Edwards; B. J. MacGowan; S. H. Glenzer
Lasnex calculations and x-ray flux measurements are presented for a series of NIF vacuum hohlraum experiments that were among the first targets shot on NIF as part of the facility commissioning. An important result is that the hohlraum x-ray fluxes are significantly higher than predicted by pre-shot Lasnex calculations employing the baseline configuration managed physics packages used in the NIF ignition target calculations. A possible explanation for the high-flux vacuum hohlraum result has been explored via post-shot calculations in which non-baseline emissivity and heat conduction models are used.
international conference on plasma science | 2005
M. B. Schneider; D. E. Hinkel; Dan E. Bower; H.C. Bruns; K. M. Campbell; J. Celeste; S. Compton; R. Costa; E. L. Dewald; S. Dixit; Mark J. Eckart; David C. Eder; M. J. Edwards; A.D. Ellis; J.A. Emig; D. H. Froula; S. H. Glenzer; D. Hargrove; C. A. Haynam; R. F. Heeter; M.A. Henesian; J. P. Holder; G. Holtmeier; D.L. James; D. H. Kalantar; J. Kamperschroer; R. L. Kauffman; J. R. Kimbrough; R. K. Kirkwood; A.E. Koniges
Summary form only given. An experimental campaign to study radiation drive in small-scale halfraums has been carried out using the first four beams of the National Ignition Facility (NIF) at the Lawerence Livermore National Laboratory (Livermore, CA). The targets fill with plasma so quickly that, late in time, most of the laser energy is deposited at the laser entrance hole. Experiments have shown the effect of laser beam conditioning, laser power, and target size on hohlraum performance. The experimental results on X-radiation drive, laser backscatter, hard X-rays, hard X-ray imaging, and X-ray burnthrough are discussed
Physical Review Letters | 2011
J. L. Kline; S. H. Glenzer; R.E. Olson; L. J. Suter; K. Widmann; D. A. Callahan; S. Dixit; C. A. Thomas; D. E. Hinkel; E. A. Williams; A. S. Moore; J. Celeste; E. Dewald; W. W. Hsing; A. Warrick; J. Atherton; S. Azevedo; R. Beeler; R. L. Berger; A. D. Conder; L. Divol; C. A. Haynam; D. H. Kalantar; R. L. Kauffman; G. A. Kyrala; J. D. Kilkenny; J. Liebman; S. Le Pape; D. W. Larson; N. B. Meezan
Physics of Plasmas | 2010
N. B. Meezan; L. J. Atherton; E. Bond; D. A. Callahan; E. L. Dewald; S. Dixit; E. G. Dzenitis; M. J. Edwards; C. A. Haynam; D. E. Hinkel; O. S. Jones; O. L. Landen; Richard A. London; P. Michel; J. D. Moody; J. L. Milovich; M. B. Schneider; C. A. Thomas; R. P. J. Town; A. Warrick; S. V. Weber; K. Widmann; S. H. Glenzer; L. J. Suter; B. J. MacGowan; J. L. Kline; G. A. Kyrala; A. Nikroo