

Observations of rad-hydro-burn simulations of high-gain
direct-drive and NIF ignition targets show that the common
wisdom of isobaric (constant pressure) conditions around
stagnation is incorrect. In particular, at ignition: (a)
hotspot and cold fuel are not in pressure equilibrium, (b)
fusion alpha energy produced up to this time can exceed the
PdV work from the stagnating shell, (c) the cold fuel
partitions into a stagnated tamp mass and a still-ingoing
unstagnated portion that contains a substantial fraction of
the fuel mass [Betti et al, Phys Plas. 9, 2277 (2002)], and
(d) the hotspot criterion for ignition, rho-R*T, is not
fixed but depends on the tamp conditions. We infer that
hotspot formation, ignition and propagating burn is a
dynamic process that necessitates a time-dependent
description and, accordingly, have formulated a fully
dynamic 0-D model based on six coupled ODEs that describe
energy, momentum and mass balances across the hotspot/cold
fuel system. We obtain fast (\sim10s) accounting of the
processes through stagnation, ignition and burn, including
full thermonuclear energy production under burn disassembly.
Good agreement with 1-D simulations is obtained for integral
quantities such as gain, yield and ignition margins.
[CO1.002] Sensitivity of NIF ignition capsules to hot electron preheat
D. J. Meeker, N. Meezan, L. J. Suter, S. Haan (Lawrence Livermore National Laboratory)
In indirect drive inertial confinement fusion, a fraction of
the laser’s energy may be transferred to super thermal
electrons through stimulated Raman scattering. These hot
electrons can irreversibly deposit energy in the cryogenic
DT fuel, raising the isentrope of the fuel (also known as
“preheat”). We explore the sensitivity of potential NIF
ignition capsules to hot electron preheat and discuss how a
given amount of hot electron production raises the minimum
energy of ignition and, consequently, affects the margin.
This work was performed under the auspices of the U.S.
Department of Energy by the University of California,
Lawrence Livermore National Laboratory under contract No.
W-7405-Eng-48.
[CO1.003] High-Areal-Density Cryogenic D_2 Implosions on OMEGA
T.C. Sangster, J.A. Delettrez, V.Yu. Glebov, V.N. Goncharov, D.R. Harding, J.P. Knauer, F.J. Marshall, P.W. McKenty, D.D. Meyerhofer, P.B. Radha, S.P. Regan, S. Skupsky, S. Smalyuk, C. Stoeckl (Laboratory for Laser Energetics, U. of Rochester), J.A. Frenje, C.K. Li, R.D. Petrasso, F.H. Séguin (PSFC, MIT)
Direct-drive implosions of cryogenic D_2-filled capsules
are being performed on the OMEGA laser. The targets and
drive pulses are energy scaled from the baseline
direct-drive ignition design developed for the NIF. The
cold-fuel areal density (\rhoR) achieved during the
burn phase is an important measure of target performance:
adequate fuel \rhoR is one of the prerequisites for
``hot-spot'' ignition. On OMEGA, \rhoR's are
inferred from the energy loss of D^3He protons.
Low-\alpha implosions have produced \rhoR's in
excess of 100 mg/cm^2, while high-\alpha experiments
have produced yields in excess of 2 \times 10^11.
Higher \rhoR's are observed in capsules with
smoother inner ice surfaces, and, in general, the inferred
\rhoR's agree with 1-D predictions. This talk will
summarize the results of several-dozen implosions. This work
was supported by the U.S. Department of Energy Office of
Inertial Confinement Fusion under Cooperative Agreement No.
DE-FC52-92SF19460.
[CO1.004] Effects of the Low-\ell-Mode Irradiation Nonuniformities on the Performance of Direct-Drive Spherical Implosions
S.P. Regan, J.A. Delettrez, V.Yu. Glebov, V.N. Goncharov, J.A. Marozas, F.J. Marshall, P.W. McKenty, D.D. Meyerhofer, P.B. Radha, T.C. Sangster, V.A. Smalyuk, C. Stoeckl (Laboratory for Laser Energetics, U. of Rochester), J.A. Frenje, C.K. Li, R.D. Petrasso, F.H. Séguin (PSFC, MIT)
The low-\ell-mode laser irradiation nonuniformity was
recently reduced on the 60 beam OMEGA laser system with a
new phase-plate design along with improvements in beam
pointing, beam balance, and target positioning accuracy. The
target performance is quantified by the ratio of the
measured primary neutron yield to the 1-D predicted yield
(YOC). The YOC's for high-adiabat (\alpha \sim 5, where
\alpha is defined as the ratio of the shell pressure to
the Fermi-degenerate pressure), D_2-filled-plastic-shell
implosions with predicted convergence ratios ranging from 15
to 40 will be compared with the calculated improvements in
the on-target laser irradiation nonuniformity levels. This
work was supported by the U.S. Department of Energy Office
of Inertial Confinement Fusion under Cooperative Agreement
No. DE-FC52-92SF19460.
[CO1.005] Effects of Dopant Radiative Cooling in Indirect-Drive Capsule Implosion Experiments
J.J. MacFarlane, I.E. Golovkin, P.R. Woodruff (Prism Computational Sciences), R.C. Mancini, L.A. Welser (Univ. of Nevada-Reno), G.A. Rochau, J.E. Bailey, T.A. Mehlhorn (Sandia National Laboratories), J.A. Koch (LLNL)
We present results from simulations performed to investigate
the effects of dopant radiative cooling in inertial
confinement fusion indirect-drive capsule implosion
experiments. Using a 1-D radiation-hydrodynamics code that
includes inline collisional-radiative modeling (HELIOS-CR),
we compute in detail the non-LTE atomic kinetics and
spectral characteristics for the Ar-doped DD fuel. We
examine the sensitivity of the fuel temperature and neutron
yield to the Ar dopant concentration. Simulation results
with 0.1% Ar are compared with electron temperature and
density distributions inferred from data obtained in OMEGA
indirect-drive experiments. The incident radiation drive on
the capsule is computed with a 3-D view factor code (VISRAD)
using the laser beam pointings and powers from the OMEGA
experiments. We also examine the sensitivity of the
calculated compressed core electron temperatures and neutron
yields to the radiation drive on the capsule, and to the
radiation and atomic modeling in the simulations.
[CO1.006] Direct drive double shell target implosion hydrodynamics on OMEGA using offset pointing
G. Kyrala, N. Delamater, D. Wilson, J. Guzik, D. Haynes, M. Gunderson, K. Klare, W. Varnum (Los Alamos National Lab), W. Garbett (AWE, Aldermaston, UK)
Imploding direct-drive double shell targets may provide an
alternative, non-cryogenic path to ignition on the National
Ignition Facility (NIF) and the Laser Megajoule (LMJ).
Experiments are being pursued at OMEGA to understand the
hydrodynamics of these implosions and the possibility of
scaling to NIF designs. We have used 40 beams from the OMEGA
laser to directly drive the capsules, and we have used the
remaining 20 beams to backlight the imploding shells from
two different directions at multiple times. Because the
number of beams was fewer than the 60 normally used to drive
a capsule symmetrically at OMEGA, we use offset pointing to
produce relatively uniform drive. Offset pointing may also
be used at other lasers not normally designed for uniformly
driven direct drive targets, such as the NIF an LMJ. We will
review the recent experiments to measure the zero-order
hydrodynamics of the targets, and the symmetry of the drive.
We use two-view x-ray radiography of the capsules.
Experiments were pursued using direct drive in which the
M-band effect, experienced in the indirect drive
experiments, could be eliminated or controlled. We will
review the method used to radiograph the targets and the
techniques used to extract useful information to compare
with calculations. The effect of imperfections in the target
construction will be shown to be minimal during the initial
stage of the implosion. (LA-UR-04-4939) This work was
performed at Los Alamos National Lab under the auspices of
the US DOE under contract No. W-7405-ENG-36
[CO1.007] Integrated 2D simulations of dynamic hohlraum driven inertial fusion capsule implosions
S.A. Slutz, R.A. Vesey, R.W. Lemke, J.E. Bailey, T.A. Mehlhorn, C.L. Ruiz, G.W. Cooper, G.A. Chandler (Sandia National Laboratories, Albuquerque, N.M.)
Simulations have been useful for improving the design of
dynamic hohlraums for the purpose of imploding inertial
fusion capsules [S. A. Slutz, J.E. Bailey, G.A. Chandler et
al Phys. Plas. 10, 1875, 2003]. These design changes, which
have resulted in capsule implosions with hot dense cores
[J.E. Bailey, G.A.Chandler, S.A. Slutz et al PRL 92,
085002-1, 2004] and the production of thermonuclear neutrons
[C.L. Ruiz, G. Cooper, S.A. Slutz, et al. PRL, 93,
015001-1], were based primarily on a series of 1D numerical
simulations, which treated the dynamic hohlraum and the
capsule implosion separately. This was appropriate for thin
walled capsules, but is not suitable for higher performance
capsules that are ablatively driven, since there can be a
significant interaction between the z-pinch driven shock in
the convertor material and the ablative blow off from the
capsule. 2D simulations will be presented which include the
implosion of wire arrays onto foam convertors, the capsule
imbedded in the foam, and the absorption of radiation into
the electrodes. These simulations are in good agreement with
most of the quantities that have been measured
experimentally. Simulations indicate that appropriately
shaping the convertors, should improved radiation symmetry
and produce larger neutron yields.
[CO1.008] Measurements of hot spot energy in capsule implosions driven by dynamic hohlraum x-rays
J.E. Bailey, G.A. Chandler, S.A. Slutz, P.W. Lake, R.J. Leeper, T.A. Mehlhorn, T.J. Nash, K. Peterson, G.A. Rochau, C.L. Ruiz, W.S. Varnum (Sandia National Laboratories, Albuquerque, NM, 87185-1196), R.C. Mancini, T.J. Buris-Mog (U. of Nevada, Reno, NV), I. Golovkin, J.J. MacFarlane (Prism Computational Sciences, Madison, WI), G.S. Dunham, T.C. Moore (K-Tech Corp., Albu., NM), G. Cooper (U. of New Mexico, Albu., NM), D.G. Schroen (Schafer Corp., Livermore, CA)
The hot spot energy in ICF implosions can be estimated from
measurements of the temperature, density, and volume
provided by time- and space-resolved Ar tracer spectroscopy.
The method is applied to experiments using 2-mm-diameter
40-80-micron-thick CH wall capsules filled with 10-25 atm D_2
+ 0.085 atm Ar. The capsules implode when they absorb 20-40
kJ of x-rays in a dynamic hohlraum configuration.
Preliminary analysis using a uniform core approximation
indicates that the hot spot energy is 300-800 J in these
relatively thin wall capsule experiments. Refinement to
include spatial core gradients, simulation comparisons, and
the possibility of increasing the efficiency will be
discussed. Sandia is a multiprogram laboratory operated by
Sandia Corporation, a Lockheed Martin Company, for the U.S.
Dept. of Energy under contract No. DE-AC04-94AL85000.
[CO1.009] Measurements of Time Evolution of Ion Temperature of D^3He Implosions on OMEGA
J.A. Frenje, C.K. Li, F.H. Seguin, J. L. DeCiantis, J. R. Rygg, M. Falk, R.D. Petrasso (MIT), J. A. Delettrez, V. Yu. Glebov, C. Stoeckl, F. J. Marshall, D. D. Meyerhofer, T. C. Sangster, V. A. Smalyuk, J. M. Soures (Laboratory for Laser Energetics, U. of Rochester)
We report here the first measurements of time evolution of ion temperature T_i(t) during the shock-burn and compression-burn phases of direct-drive D^3He implosions on the 60-beam, UV OMEGA laser system. The experiments were accomplished using a proton temporal diagnostic (PTD) to measure the D^3He-reaction rate, and a neutron temporal diagnostic (NTD) to measure the DD-reaction rate. By taking the ratio of the measured burn histories, and initially assuming n_i and T_i profiles upon which we iterate, a final T_i(t) can be inferred for the entire burn. The results from these measurements are compared to numerical simulations.
This work was performed in part at the LLE NLUF, and
supported in part by the U.S. Department of Energy
(DE-FG03-03SF22691, DE-FG03-03NA00058, and Cooperative
Agreement DE-FC52-92SF19460), LLE (412160-001G), and LLNL
(B504974).
[CO1.010] Inference of Imprint at Onset of Deceleration Phase Using Shock-Burn Measurements
J.R. Rygg, F.H. Seguin, C.K. Li, J.A. Frenje, J.L. DeCiantis, R.D. Petrasso (MIT), J.A. Delettrez, V.Yu. Glebov, V.N. Goncharov, D.D. Meyerhofer, P.B. Radha, S.P. Regan, T.C. Sangster (Laboratory for Laser Energetics, U. of Rochester)
A vital concern for ICF is the premature quenching of the nuclear burn due to mixing of cold shell material into the hot spot. This mixing is caused largely by Rayleigh-Taylor growth during the deceleration phase of modulations imprinted into the shell at earlier times. Spectral, spatial, and temporal measurements of nuclear products emitted during the shock-burn phase of the implosion, which occurs just before the onset of the deceleration phase, can put useful constraints on the amplitude of imprinted areal-density variations at this time. Another indicator of shell integrity is the shell areal density at shock-burn time, which we can also infer from the nuclear measurements. Results from recent experiments will be presented.
This work was supported in part by the U.S. Department of
Energy (DE-FG03-03SF22691, DE-FG03-03NA00058, and
Cooperative Agreement DE-FC52-92SF19460), LLE (412160-001G),
and LLNL (B504974).
[CO1.011] Studying the Burn Region in ICF Implosions with Proton Emission Imaging
J.L. DeCiantis, F.H. Seguin, J.A. Frenje, J.R. Rygg, C.D. Chen, C.K. Li, R.D. Petrasso (MIT), J.A. Delettrez, J.P. Knauer, F.J. Marshall, D.D. Meyerhofer, S. Roberts, T.C. Sangster, V.A. Smalyuk (Laboratory for Laser Energetics, U. of Rochester)
Proton core imaging spectroscopy (PCIS) is being used to study the effects of fuel shell mix in implosions of D^3He-filled capsules at OMEGA. Penumbral imaging of fusion products is used to obtain the size and shape of the nuclear burn region. Experimental differences in the D^3He burn region will be explored for varying laser conditions and for different shell types (2 to 3 mm glass and 17, 20, 24 and 27 mm CH). Secondary D^3He proton production profiles from a D_2-filled-capsule implosion will be examined to explore the feasibility of imaging cryogenic implosions. Measured burn profiles will be compared to predictions of clean 1-D simulations and to x-ray images.
This work was supported in part by the U.S. Department of
Energy (DE-FG03-03SF22691, DE-FG03-03NA00058, and
Cooperative Agreement DE-FC52-92SF19460), LLE (412160-001G),
and LLNL (B504974).
[CO1.012] Relationship of Asymmetries in Fusion Burn and Areal Density to Asymmetries in Laser Drive for ICF Implosions at OMEGA
F.H. Seguin, J.L. DeCiantis, J.A. Frenje, C.K. Li, J.R. Rygg, C.D. Chen, R.D. Petrasso (MIT), V.A. Smalyuk, F.J. Marshall, J.A. Delettrez, J.P. Knauer, P.W. McKenty, D.D. Meyerhofer, S. Roberts, T.C. Sangster (Laboratory for Laser Energetics, U. of Rochester), K. Mikaelian, H.S. Park (LLNL)
The physical characteristics of asymmetric ICF implosions, and their relationship to laser drive asymmetry, are being studied on OMEGA using capsules with D3He fill and diagnostics that detect D3He protons. The spatial distribution of D3He burn is measured with three orthogonally oriented proton imaging cameras, while the angular distribution of areal density is studied with multiple proton spectrometers. Results from experiments involving imposed drive asymmetry will be discussed, along with comparisons of data with x-ray images and with 2-D simulations.
This work was supported in part by the U.S. Department of
Energy (DE-FG03-03SF22691, DE-FG03-03NA00058, and
Cooperative Agreement DE-FC52-92SF19460), LLE (412160-001G),
and LLNL (B504974).
[CO1.013] Shock-Timing Experiments in Planar Cryogenic Deuterium Targets
T.R. Boehly, E. Vianello, J. Miller, R.S. Craxton, V.N. Goncharov, I.V. Igumenshchev, D.D. Meyerhofer (Laboratory for Laser Energetics, U. of Rochester), D.G. Hicks, P.M. Celliers (LLNL)
Direct-drive ICF target designs use multiple shocks to
stabilize and condition the imploding shell. The magnitude
and timing of these shocks are critical to optimization of
those designs. We present results from planar cryogenic
D_2 experiments that use two 100-ps pulses to produce
two shocks at various conditions. The velocity profiles of
these shocks (from VISAR) and self-emission are used to
investigate the coupling of multiple beams to the targets
and to demonstrate the ability of hydrodynamic codes to
model multiple shocks in cryogenic D_2. This work was
supported by the U.S. Department of Energy Office of
Inertial Confinement Fusion under Cooperative Agreement No.
DE-FC52-92SF19460.
[CO1.014] The Effect of Incidence Angle on Laser-Driven Shocks
E. Vianello, T.R. Boehly, R.S. Craxton, V.N. Goncharov, J. Miller, I.V. Igumenshchev, D.D. Meyerhofer, T.C. Sangster (Laboratory for Laser Energetics, U. of Rochester), D.G. Hicks, P.M. Celliers (LLNL)
The proper timing of shocks is essential for inertial
confinement fusion ignition targets and to the development
of polar direct drive. The effect of the angle of incidence
on energy coupling and the production of laser-driven shocks
are measured in planar target experiments. Two 100-ps pulses
produce a pair of shocks with various strengths and relative
delays. Velocity profiles (from VISAR) and self-emission
from these shocks are compared to one-dimensional
hydrodynamic simulations. A simple refraction model
adequately treats the coupling of high-angle beams to the
target. This work was supported by the U.S. Department of
Energy Office of Inertial Confinement Fusion under
Cooperative Agreement No. DE-FC52-92SF19460 and Lawrence
Livermore National Laboratory under contract
No.W-7405-Eng-48.
[CO1.015] Streaked Optical Pyrometer for Shock Wave and EOS Studies
J. Miller, T.R. Boehly, E. Vianello, W.J. Armstrong, C. Sorce, W. Theobald, D.D. Meyerhofer (Laboratory for Laser Energetics, U. of Rochester), J. Eggert, D.G. Hicks (LLNL)
The optical self-emission from laser-driven shock waves provides important information about the strength of a shock and the EOS of the shocked material. A streak camera was used to temporally and spatially resolve emission from shocks in transparent targets. A NIST traceable lamp was used to calibrate the device to provide brightness temperatures. Various shock-timing and EOS experiments demonstrate the relationship between shock velocity (strength) and optical emission. The coalescence of two shocks and their arrival at the rear surface are observed, providing valuable shock-timing data. Temperature measurements in \alpha-quartz samples are used to evaluate various EOS models. This work was supported by the U.S. Department of Energy Office of Inertial Confinement Fusion under Cooperative Agreement No. DE-FC52-92SF19460.