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Dive into the research topics where Ryan Rygg is active.

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Featured researches published by Ryan Rygg.


Nuclear Fusion | 2013

Diagnosing implosion performance at the National Ignition Facility (NIF) by means of neutron spectrometry

J. A. Frenje; R. Bionta; E. Bond; J. A. Caggiano; D. T. Casey; Charles Cerjan; J. Edwards; M. J. Eckart; D. N. Fittinghoff; S. Friedrich; V. Yu. Glebov; S. H. Glenzer; Gary P. Grim; S. W. Haan; R. Hatarik; S. P. Hatchett; M. Gatu Johnson; O. S. Jones; J. D. Kilkenny; J. P. Knauer; O. L. Landen; R. J. Leeper; S. Le Pape; R. A. Lerche; C. K. Li; A. J. Mackinnon; J. M. McNaney; F. E. Merrill; M. J. Moran; David H. Munro

The neutron spectrum from a cryogenically layered deuterium?tritium (dt) implosion at the National Ignition Facility (NIF) provides essential information about the implosion performance. From the measured primary-neutron spectrum (13?15?MeV), yield (Yn) and hot-spot ion temperature (Ti) are determined. From the scattered neutron yield (10?12?MeV) relative to Yn, the down-scatter ratio, and the fuel areal density (?R) are determined. These implosion parameters have been diagnosed to an unprecedented accuracy with a suite of neutron-time-of-flight spectrometers and a magnetic recoil spectrometer implemented in various locations around the NIF target chamber. This provides good implosion coverage and excellent measurement complementarity required for reliable measurements of Yn, Ti and ?R, in addition to ?R asymmetries. The data indicate that the implosion performance, characterized by the experimental ignition threshold factor, has improved almost two orders of magnitude since the first shot taken in September 2010. ?R values greater than 1?g?cm?2 are readily achieved. Three-dimensional semi-analytical modelling and numerical simulations of the neutron-spectrometry data, as well as other data for the hot spot and main fuel, indicate that a maximum hot-spot pressure of ?150?Gbar has been obtained, which is almost a factor of two from the conditions required for ignition according to simulations. Observed Yn are also 3?10 times lower than predicted. The conjecture is that the observed pressure and Yn deficits are partly explained by substantial low-mode ?R asymmetries, which may cause inefficient conversion of shell kinetic energy to hot-spot thermal energy at stagnation.


Physics of Plasmas | 2016

The near vacuum hohlraum campaign at the NIF: A new approach

S. Le Pape; L. Berzak Hopkins; L. Divol; N. B. Meezan; D. Turnbull; A. J. Mackinnon; D. Ho; J. S. Ross; S. F. Khan; A. Pak; E. Dewald; L.R. Benedetti; S. R. Nagel; J. Biener; D. A. Callahan; C. B. Yeamans; P. Michel; M. B. Schneider; B. J. Kozioziemski; T. Ma; A. G. MacPhee; S. W. Haan; N. Izumi; R. Hatarik; P. A. Sterne; Peter M. Celliers; J. E. Ralph; Ryan Rygg; D. J. Strozzi; J. D. Kilkenny

The near vacuum campaign on the National Ignition Facility has concentrated its efforts over the last year on finding the optimum target geometry to drive a symmetric implosion at high convergence ratio (30×). As the hohlraum walls are not tamped with gas, the hohlraum is filling with gold plasma and the challenge resides in depositing enough energy in the hohlraum before it fills up. Hohlraum filling is believed to cause symmetry swings late in the pulse that are detrimental to the symmetry of the hot spot at high convergence. This paper describes a series of experiments carried out to examine the effect of increasing the distance between the hohlraum wall and the capsule (case to capsule ratio) on the symmetry of the hot spot. These experiments have shown that smaller Case to Capsule Ratio (CCR of 2.87 and 3.1) resulted in oblate implosions that could not be tuned round. Larger CCR (3.4) led to a prolate implosion at convergence 30× implying that inner beam propagation at large CCR is not impeded by the expanding hohlraum plasma. A Case to Capsule ratio of 3.4 is a promising geometry to design a round implosion but in a smaller hohlraum where the hohlraum losses are lower, enabling a wider cone fraction range to adjust symmetry.


international conference on plasma science | 2016

Temporal evolution of the two-shock implosion on the National Ignition Facility

T. Ma; S. A. MacLaren; J. D. Salmonson; S. F. Khan; J. Pino; J. E. Ralph; Ryan Rygg; J. E. Field; R. Tommasini; D. Turnbull; A. J. Mackinnon; K. L. Baker; L. R. Benedetti; Peter M. Celliers; E. Dewald; T. R. Dittrich; L. Berzak Hopkins; N. Izumi; P. Kervin; S. R. Nagel; A. Pak; Robert Tipton; G. A. Kyrala; J. L. Kline

Summary form only given. The HED 2-Shock implosion campaign was developed on the National Ignition Facility as a relatively robust and well-beha ved nearly one-dimensional, low convergence, symmetric platform by employing a very high foot temperature and a large case-to-capsule (hohlraum-to-capsule) ratio. The results of these experiments investigating capsule implosion phenomena such as interface hydrodynamic mixing, convergence effects, and shape effects are being used for the validation of hydro-c odes and to develop a systematic understanding of performance degradation mechanisms. A sequence of experiments was initially completed to tune the 2-Shock implosion round, with little shape swing from in-flight to stagnation. Then, hohlraum size and hohlraum gas fill were systematically changed to study the effect on shape and symmetry evolution. Details and results of these experiments are described.


Bulletin of the American Physical Society | 2017

Experimental Measurements of Carbon Dioxide Shock and Reshock Equation of State to 10 Mbar

Tom Zick; Marius Millot; Ryan Rygg; Dylan K. Spaulding; Peter M. Celliers; G. W. Collins; Jon H. Eggert; Raymond Jeanloz


Bulletin of the American Physical Society | 2017

Double shocks on precompressed deuterium near the plasma phase transition

S. Brygoo; Marius Millot; Paul Loubeyre; Peter M. Celliers; G. W. Collins; Jon H. Eggert; Ryan Rygg; Damian C. Swift; Raymond Jeanloz


Bulletin of the American Physical Society | 2017

The Shock and Release Behaviors of Diamond at Terapascal Pressures

M.C. Gregor; D. E. Fratanduono; Peter M. Celliers; Tom Braun; Jon H. Eggert; D. N. Polsin; Andrew Sorce; Ryan Rygg; G. W. Collins; Thomas R. Boehly; Chad McCoy; D. D. Meyerhofer


Bulletin of the American Physical Society | 2017

The first observation of the bcc phase in aluminum compressed to 559 GPa

D. N. Polsin; D. E. Fratanduono; Ryan Rygg; A. Jenei; Raymond F. Smith; Jon H. Eggert; Michelle Gregor; B. Henderson; J. A. Delettrez; Richard Kraus; Peter M. Celliers; Federica Coppari; Damian C. Swift; Chad McCoy; Christopher T. Seagle; Jean-Paul Davis; Stephen Burns; Thomas R. Boehly; G. W. Collins


Bulletin of the American Physical Society | 2016

Measurements of Hard X-Ray Emission Suggest Absorption Along the Path of the Inner Beams in High Foot Implosion Experiments on the NIF

J. E. Ralph; A. Pak; Landen Otto; A. L. Kritcher; T. Ma; Jarrott Charles; D. A. Callahan; D. E. Hinkel; Laura Berzak Hopkins; John Moody; S. F. Khan; T. Doeppner; Ryan Rygg; Omar Hurricane


Bulletin of the American Physical Society | 2016

A platform for detecting material melting from shock compression using the NIF x-ray diffraction diagnostic TARDIS

Christopher Wehrenberg; Richard Kraus; Dave Braun; Ryan Rygg; Federica Coppari; Amy Lazicki; J. M. McNaney; Jon H. Eggert


Bulletin of the American Physical Society | 2015

High Foot Implosion Experiments in Rugby Hohlraums

J. E. Ralph; J.-P. Leidinger; D. A. Callahan; P. Kaiser; O. Morice; D. Marion; J. D. Moody; J. S. Ross; Peter A. Amendt; A. L. Kritcher; J. L. Milovich; D. J. Strozzi; D. E. Hinkel; P. Michel; L. Berzak Hopkins; A. Pak; E. L. Dewald; L. Divol; S. F. Khan; Ryan Rygg; O. A. Hurricane

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Jon H. Eggert

Lawrence Livermore National Laboratory

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G. W. Collins

Lawrence Livermore National Laboratory

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Amy Lazicki

Carnegie Institution for Science

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Peter M. Celliers

Lawrence Livermore National Laboratory

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Raymond F. Smith

Lawrence Livermore National Laboratory

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D. E. Fratanduono

Lawrence Livermore National Laboratory

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Federica Coppari

Lawrence Livermore National Laboratory

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A. J. Mackinnon

Lawrence Livermore National Laboratory

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Damian C. Swift

Lawrence Livermore National Laboratory

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S. F. Khan

Lawrence Livermore National Laboratory

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