S. Skupsky
University of Rochester
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Featured researches published by S. Skupsky.
Physics of Plasmas | 2004
S. Skupsky; J.A. Marozas; R. S. Craxton; R. Betti; T.J.B. Collins; J. A. Delettrez; V.N. Goncharov; P. W. McKenty; P. B. Radha; T. R. Boehly; J. P. Knauer; F. J. Marshall; D. R. Harding; J. D. Kilkenny; D. D. Meyerhofer; T. C. Sangster; R. L. McCrory
Three recent developments in direct-drive target design have enhanced the possibility of achieving high target gain on the National Ignition Facility (NIF): (1) Laser absorption was increased by almost 50% using wetted-foam targets. (2) Adiabat shaping significantly increased the hydrodynamic stability of the target during the acceleration phase of the implosion without sacrificing target gain. (3) Techniques to reduce laser imprint using pulse shaping and radiation preheat were developed. These design features can be employed for direct-drive-ignition experiments while the NIF is in the x-ray-drive configuration. This involves repointing some of the beams toward the equator of the target to improve uniformity of target drive. This approach, known as polar direct drive (PDD), will enhance the capability of the NIF to explore ignition conditions. PDD will couple more energy to the fuel than x-ray drive. The compressed fuel core can be more easily accessed for high-ρR diagnostic development and for fast-ign...
Physics of Plasmas | 2005
P. B. Radha; V.N. Goncharov; T.J.B. Collins; J. A. Delettrez; Y. Elbaz; V. Yu. Glebov; R. L. Keck; D. E. Keller; J. P. Knauer; J.A. Marozas; F. J. Marshall; P. W. McKenty; D. D. Meyerhofer; S. P. Regan; T. C. Sangster; D. Shvarts; S. Skupsky; Y. Srebro; R. P. J. Town; C. Stoeckl
Multidimensional hydrodynamic properties of high-adiabat direct-drive plastic-shell implosions on the OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] are investigated using the multidimensional hydrodynamic code, DRACO [D. Keller et al., Bull. Am. Phys. Soc. 44, 37 (1999)]. Multimode simulations including the effects of nonuniform illumination and target roughness indicate that shell stability during the acceleration phase plays a critical role in determining target performance. For thick shells that remain integral during the acceleration phase, target yields are significantly reduced by the combination of the long-wavelength (l<10) modes due to surface roughness and beam imbalance and the intermediate modes (20⩽l⩽50) due to single-beam nonuniformities. The neutron-production rate for these thick shells truncates relative to one-dimensional (1D) predictions. The yield degradation in the thin shells is mainly due to shell breakup at short wavelengths (λ∼Δ, where Δ is the in-flight s...
Physics of Plasmas | 2005
P. B. Radha; T.J.B. Collins; J. A. Delettrez; Y. Elbaz; R. Epstein; V. Yu. Glebov; V.N. Goncharov; R. L. Keck; J. P. Knauer; J.A. Marozas; F. J. Marshall; R. L. McCrory; P.W. McKenty; D. D. Meyerhofer; S. P. Regan; T. C. Sangster; W. Seka; D. Shvarts; S. Skupsky; Y. Srebro; C. Stoeckl
Direct-drive, plastic shells imploded on the OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)] with a 1ns square pulse are simulated using the multidimensional hydrodynamic code DRACO in yield degradation in “thin” shells is primarily caused by shell breakup during the acceleration phase due to short-wavelength (l>50, where l is the Legendre mode number) perturbation growth, whereas “thick” shell performance is influenced primarily by long and intermediate modes (l⩽50). Simulation yields, temporal history of neutron production, areal densities, and x-ray images of the core compare well with experimental observations. In particular, the thin-shell neutron production history falls off less steeply than one-dimensional predictions due to shell-breakup-induced undercompression and delayed stagnation. Thicker, more-stable shells show burn truncation due to instability-induced mass flow into the colder bubbles. Estimates of small-scale mix indicate that turbulent mixing does not influence p...
Physics of Plasmas | 2006
J.A. Marozas; F. J. Marshall; R. S. Craxton; Igor V. Igumenshchev; S. Skupsky; M.J. Bonino; T.J.B. Collins; R. Epstein; V. Yu. Glebov; D. Jacobs-Perkins; J. P. Knauer; R. L. McCrory; P. W. McKenty; D. D. Meyerhofer; S.G. Noyes; P. B. Radha; T. C. Sangster; W. Seka; V. A. Smalyuk
Polar direct drive (PDD) [S. Skupsky et al., Phys. Plasmas 11, 2763 (2004)] will allow direct-drive ignition experiments on the National Ignition Facility (NIF) [J. Paisner et al., Laser Focus World 30, 75 (1994)] as it is configured for x-ray drive. Optimal drive uniformity is obtained via a combination of beam repointing, pulse shapes, spot shapes, and∕or target design. This article describes progress in the development of standard and “Saturn” [R. S. Craxton and D. W. Jacobs-Perkins, Phys. Rev. Lett. 94, 0952002 (2005)] PDD target designs. Initial evaluation of experiments on the OMEGA Laser System [T. R. Boehly et al., Rev. Sci. Instrum. 66, 508 (1995)] and simulations were carried out with the two-dimensional hydrodynamics code SAGE [R. S. Craxton et al., Phys. Plasmas 12, 056304 (2005)]. This article adds to this body of work by including fusion particle production and transport as well as radiation transport within the two-dimensional DRACO [P. B. Radha et al., Phys. Plasmas 12, 032702 (2005)] hydr...
Physics of Plasmas | 2005
R. Betti; Karen S. Anderson; J. P. Knauer; T.J.B. Collins; R. L. McCrory; P. W. McKenty; S. Skupsky
The theory of the adiabat shaping induced by a strong shock propagating through a relaxed density profile is carried out for inertial confinement fusion (ICF) capsules. The relaxed profile is produced through a laser prepulse, while the adiabat-shaping shock is driven by the foot of the main laser pulse. The theoretical adiabat profiles accurately reproduce the simulation results. ICF capsules with a shaped adiabat are expected to benefit from improved hydrodynamic stability while maintaining the same one-dimensional performances as flat-adiabat shells.
Physics of Plasmas | 2005
R. S. Craxton; F. J. Marshall; M. J. Bonino; R. Epstein; P.W. McKenty; S. Skupsky; J. A. Delettrez; Igor V. Igumenshchev; D. Jacobs-Perkins; J. P. Knauer; J.A. Marozas; P. B. Radha; W. Seka
Polar direct drive (PDD) [S. Skupsky et al., Phys. Plasmas 11 2763 (2004)] shows promise for achieving direct-drive ignition while the National Ignition Facility (NIF) [E. M. Campbell and W. J. Hogan, Plasma Phys. Control. Fusion 41 B39 (1999)] is initially configured for indirect drive. Experiments have been carried out using 40 repointed beams of the 60-beam OMEGA laser system [T. R. Boehly et al., Rev. Sci. Instrum. 66 508 (1995)] to approximate the NIF PDD configuration. Backlit x-ray framing-camera images of D2-filled spherical CH capsules show a characteristic nonuniformity pattern that is in close agreement with predictions. Saturn targets (similar capsules surrounded by a plastic ring) increase the drive on the equator, suggesting that highly symmetric PDD implosions may be possible with appropriate tuning. Two-dimensional (2D) simulations reproduced the approximately threefold reduction in yield found for the non-Saturn PDD capsules. Preliminary simulations for a NIF Saturn design predict a high ...
Physics of Plasmas | 2005
F. J. Marshall; R. S. Craxton; J. A. Delettrez; D. H. Edgell; L. M. Elasky; R. Epstein; V. Yu. Glebov; V.N. Goncharov; D. R. Harding; R. Janezic; R. L. Keck; J.D. Kilkenny; J. P. Knauer; S. J. Loucks; L. D. Lund; R. L. McCrory; P.W. McKenty; D. D. Meyerhofer; P. B. Radha; S. P. Regan; T. C. Sangster; W. Seka; V. A. Smalyuk; J. M. Soures; C. Stoeckl; S. Skupsky; J. A. Frenje; C. K. Li; R. D. Petrasso; F. H. Séguin
Direct-drive spherical implosions of cryogenic, D2-filled capsules are performed on the 60-beam OMEGA laser system [T. R. Boehly, D. L. Brown, R. S. Craxton, R. L. Keck, J. P. Knauer, J. H. Kelly, T. J. Kessler, S. A. Kumpan, S. J. Loucks, S. A. Letzring, F. J. Marshall, R. L. McCrory, S. F. B. Morse, W. Seka, J. M. Soures, and C. P. Verdon, Opt. Commun. 133, 495 (1997)]. The targets are energy scaled from the base line ignition design developed for the National Ignition Facility [W. J. Hogan et al., Nucl. Fusion 41, 567 (2001)]. Thin-walled (∼4μm), ∼860μm diam deuterated polymer shells are permeation filled with D2 gas and cooled to the triple point (∼18.7K). Cryogenic ice layers with a uniformity of ∼2μm rms are formed and maintained. The targets are imploded with high-contrast pulse shapes with full single-beam smoothing (1THz bandwidth, two-dimensional smoothing by spectral dispersion with polarization smoothing) to study the effects of the acceleration- and deceleration-phase Rayleigh–Taylor growth o...
Physics of Plasmas | 2003
P. W. McKenty; T. C. Sangster; M. Alexander; R. Betti; R. S. Craxton; J. A. Delettrez; L. M. Elasky; R. Epstein; A. Frank; V. Yu. Glebov; V.N. Goncharov; D. R. Harding; S. Jin; J. P. Knauer; R. L. Keck; S. J. Loucks; L. D. Lund; R. L. McCrory; F. J. Marshall; D. D. Meyerhofer; S. P. Regan; P. B. Radha; S. Roberts; W. Seka; S. Skupsky; V. A. Smalyuk; J. M. Soures; K. A. Thorp; M. Wozniak; J. A. Frenje
Journal De Physique Iv | 2006
F. J. Marshall; R. S. Craxton; M.J. Bonino; R. Epstein; V. Yu. Glebov; D. Jacobs-Perkins; J. P. Knauer; J.A. Marozas; P. W. McKenty; S.G. Noyes; P. B. Radha; W. Seka; S. Skupsky; V. A. Smalyuk
Journal De Physique Iv | 2006
S. Skupsky; R. S. Craxton; F. J. Marshall; R. Betti; T.J.B. Collins; R. Epstein; V.N. Goncharov; Igor V. Igumenshchev; J.A. Marozas; P. W. McKenty; P. B. Radha; J.D. Kilkenny; D. D. Meyerhofer; T. C. Sangster; R. L. McCrory