W. Stoeffl
Lawrence Livermore National Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by W. Stoeffl.
Physics of Plasmas | 2011
M. J. Edwards; J. D. Lindl; B. K. Spears; S. V. Weber; L. J. Atherton; D. L. Bleuel; David K. Bradley; D. A. Callahan; Charles Cerjan; D. S. Clark; G. W. Collins; J. Fair; R. J. Fortner; S. H. Glenzer; S. W. Haan; B. A. Hammel; Alex V. Hamza; S. P. Hatchett; N. Izumi; B. Jacoby; O. S. Jones; J. A. Koch; B. J. Kozioziemski; O. L. Landen; R. A. Lerche; B. J. MacGowan; A. J. Mackinnon; E. R. Mapoles; M. M. Marinak; M. J. Moran
Ignition requires precisely controlled, high convergence implosions to assemble a dense shell of deuterium-tritium (DT) fuel with ρR>∼1 g/cm2 surrounding a 10 keV hot spot with ρR ∼ 0.3 g/cm2. A working definition of ignition has been a yield of ∼1 MJ. At this yield the α-particle energy deposited in the fuel would have been ∼200 kJ, which is already ∼10 × more than the kinetic energy of a typical implosion. The National Ignition Campaign includes low yield implosions with dudded fuel layers to study and optimize the hydrodynamic assembly of the fuel in a diagnostics rich environment. The fuel is a mixture of tritium-hydrogen-deuterium (THD) with a density equivalent to DT. The fraction of D can be adjusted to control the neutron yield. Yields of ∼1014−15 14 MeV (primary) neutrons are adequate to diagnose the hot spot as well as the dense fuel properties via down scattering of the primary neutrons. X-ray imaging diagnostics can function in this low yield environment providing additional information about ...
Physical Review D | 2004
Stephen John Asztalos; Richard Bradley; L. D. Duffy; C. Hagmann; D. Kinion; D. M. Moltz; L.J. Rosenberg; P. Sikivie; W. Stoeffl; N. S. Sullivan; D. B. Tanner; K. van Bibber; D. B. Yu
The axion is a hypothetical elementary particle and cold dark matter candidate. In this RF cavity experiment, halo axions entering a resonant cavity immersed in a static magnetic field convert into microwave photons, with the resulting photons detected by a low-noise receiver. The ADMX Collaboration presents new limits on the axion-to-photon coupling and local axion dark matter halo mass density from a RF cavity axion search in the axion mass range 1.9-2.3 {micro}eV, broadening the search range to 1.9-3.3 {micro}eV. In addition, we report first results from an improved analysis technique.
Physical Review Letters | 1998
C. Hagmann; D. Kinion; W. Stoeffl; K. van Bibber; E. Daw; H. Peng; L. Rosenberg; J. Laveigne; P. Sikivie; N. S. Sullivan; D. B. Tanner; F.A. Nezrick; Michael S. Turner; D. M. Moltz; J. Powell; N.A. Golubev
We report the first results of a high-sensitivity
IEEE Transactions on Nuclear Science | 2009
Giulia Hull; Natalia P. Zaitseva; Nerine J. Cherepy; Jason Newby; W. Stoeffl; Stephen A. Payne
(\ensuremath{\sim}{10}^{\ensuremath{-}23}\mathrm{W})
Review of Scientific Instruments | 2010
V. Yu. Glebov; T. C. Sangster; C. Stoeckl; J. P. Knauer; W. Theobald; K. L. Marshall; M. J. Shoup; T. Buczek; M. Cruz; T. Duffy; M. Romanofsky; M. Fox; A. Pruyne; M. J. Moran; R. A. Lerche; J. M. McNaney; J. D. Kilkenny; M. J. Eckart; D. Schneider; D. H. Munro; W. Stoeffl; R. Zacharias; J. J. Haslam; T. J. Clancy; M. Yeoman; D. Warwas; C. J. Horsfield; J. L. Bourgade; O. Landoas; L. Disdier
search for light halo axions through their conversion to microwave photons. At the 90% confidence level, we exclude a Kim-Shifman-Vainshtein-Zakharov axion of mass
The Astrophysical Journal | 2002
S.J. Asztalos; E. Daw; H. Peng; L. Rosenberg; D. B. Yu; C. Hagmann; D. Kinion; W. Stoeffl; K. van Bibber; Joseph Donald Laveigne; P. Sikivie; N. S. Sullivan; D. B. Tanner; F.A. Nezrick; D. M. Moltz
2.9\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}
Review of Scientific Instruments | 2010
H. W. Herrmann; Nelson M. Hoffman; D. C. Wilson; W. Stoeffl; Lucile S. Dauffy; Y. Kim; A. McEvoy; C. S. Young; J. M. Mack; C. J. Horsfield; M. S. Rubery; E. K. Miller; Zaheer Ali
to
Physics of Plasmas | 2014
D. T. Casey; V. A. Smalyuk; Robert Tipton; J. Pino; Gary P. Grim; B. A. Remington; Dana P. Rowley; S. V. Weber; M. A. Barrios; L. R. Benedetti; D. L. Bleuel; E. Bond; David K. Bradley; J. A. Caggiano; D. A. Callahan; Charles Cerjan; K. C. Chen; D. H. Edgell; M. J. Edwards; D. N. Fittinghoff; J. A. Frenje; M. Gatu-Johnson; Vladimir Yu. Glebov; S. Glenn; N. Guler; S. W. Haan; Alex V. Hamza; R. Hatarik; H. W. Herrmann; D. Hoover
3.3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}\mathrm{eV}
Journal of Physics: Conference Series | 2010
H. W. Herrmann; C. S. Young; J. M. Mack; Y. Kim; A. McEvoy; S. C. Evans; T. J. Sedillo; S. H. Batha; M Schmitt; D. C. Wilson; J R Langenbrunner; Robert M. Malone; Morris I. Kaufman; Brian C. Cox; B. C. Frogget; E K Miller; Z A Ali; T. W. Tunnell; W. Stoeffl; C. J. Horsfield; M. S. Rubery
as the dark matter in the halo of our galaxy.
Review of Scientific Instruments | 2008
Robert M. Malone; H. W. Herrmann; W. Stoeffl; J. M. Mack; C. Young
Efficient, readily-available, low-cost, high-energy neutron detectors can play a central role in detecting illicit nuclear weapons since neutrons are a strong indication for the presence of fissile material such as Plutonium and Highly-Enriched Uranium. The main challenge in detecting fast neutrons consists in the discrimination of the signal from the gamma radiation background. At present, the only well-investigated organic crystal scintillator for fast neutron detection, in a n/gamma mixed field, is stilbene, which while offering good pulse shape discrimination, is not widely used because of its limited availability and high cost.