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Featured researches published by S. A. Yi.


Physics of Plasmas | 2016

First beryllium capsule implosions on the National Ignition Facility

J. L. Kline; S. A. Yi; Andrei N. Simakov; R. E. Olson; D. C. Wilson; G. A. Kyrala; T. S. Perry; S. H. Batha; A. Zylstra; E. L. Dewald; R. Tommasini; J. E. Ralph; D. J. Strozzi; A. G. MacPhee; D. A. Callahan; D. E. Hinkel; O. A. Hurricane; J. L. Milovich; J. R. Rygg; S. F. Khan; S. W. Haan; Peter M. Celliers; D. S. Clark; B. A. Hammel; B. J. Kozioziemski; M. B. Schneider; M. M. Marinak; H. G. Rinderknecht; H. F. Robey; J. D. Salmonson

The first indirect drive implosion experiments using Beryllium (Be) capsules at the National Ignition Facility confirm the superior ablation properties and elucidate possible Be-ablator issues such as hohlraum filling by ablator material. Since the 1990s, Be has been the preferred Inertial Confinement Fusion (ICF) ablator because of its higher mass ablation rate compared to that of carbon-based ablators. This enables ICF target designs with higher implosion velocities at lower radiation temperatures and improved hydrodynamic stability through greater ablative stabilization. Recent experiments to demonstrate the viability of Be ablator target designs measured the backscattered laser energy, capsule implosion velocity, core implosion shape from self-emission, and in-flight capsule shape from backlit imaging. The laser backscatter is similar to that from comparable plastic (CH) targets under the same hohlraum conditions. Implosion velocity measurements from backlit streaked radiography show that laser energy coupling to the hohlraum wall is comparable to plastic ablators. The measured implosion shape indicates no significant reduction of laser energy from the inner laser cone beams reaching the hohlraum wall as compared with plastic and high-density carbon ablators. These results indicate that the high mass ablation rate for beryllium capsules does not significantly alter hohlraum energetics. In addition, these data, together with data for low fill-density hohlraum performance, indicate that laser power multipliers, required to reconcile simulations with experimental observations, are likely due to our limited understanding of the hohlraum rather than the capsule physics since similar multipliers are needed for both Be and CH capsules as seen in experiments.


Physics of Plasmas | 2014

Hydrodynamic instabilities in beryllium targets for the National Ignition Facility

S. A. Yi; Andrei N. Simakov; D. C. Wilson; R. E. Olson; J. L. Kline; D. S. Clark; B. A. Hammel; J. L. Milovich; J. D. Salmonson; B. J. Kozioziemski; S. H. Batha

Beryllium ablators offer higher ablation velocity, rate, and pressure than their carbon-based counterparts, with the potential to increase the probability of achieving ignition at the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)]. We present here a detailed hydrodynamic stability analysis of low (NIF Revision 6.1) and high adiabat NIF beryllium target designs. Our targets are optimized to fully utilize the advantages of beryllium in order to suppress the growth of hydrodynamic instabilities. This results in an implosion that resists breakup of the capsule, and simultaneously minimizes the amount of ablator material mixed into the fuel. We quantify the improvement in stability of beryllium targets relative to plastic ones, and show that a low adiabat beryllium capsule can be at least as stable at the ablation front as a high adiabat plastic target.


Physical Review Letters | 2016

First Liquid Layer Inertial Confinement Fusion Implosions at the National Ignition Facility.

R.E. Olson; R. J. Leeper; J. L. Kline; A. Zylstra; S. A. Yi; Juergen Biener; T. Braun; B. J. Kozioziemski; J. Sater; P. A. Bradley; Robert R. Peterson; Brian M. Haines; L. Yin; L. Berzak Hopkins; N. B. Meezan; C. Walters; M. M. Biener; C. Kong; J. Crippen; G. A. Kyrala; R. C. Shah; H. W. Herrmann; D. C. Wilson; Alex V. Hamza; A. Nikroo; S. H. Batha

The first cryogenic deuterium and deuterium-tritium liquid layer implosions at the National Ignition Facility (NIF) demonstrate D_{2} and DT layer inertial confinement fusion (ICF) implosions that can access a low-to-moderate hot-spot convergence ratio (1230) DT ice layer implosions. Although high CR is desirable in an idealized 1D sense, it amplifies the deleterious effects of asymmetries. To date, these asymmetries prevented the achievement of ignition at the NIF and are the major cause of simulation-experiment disagreement. In the initial liquid layer experiments, high neutron yields were achieved with CRs of 12-17, and the hot-spot formation is well understood, demonstrated by a good agreement between the experimental data and the radiation hydrodynamic simulations. These initial experiments open a new NIF experimental capability that provides an opportunity to explore the relationship between hot-spot convergence ratio and the robustness of hot-spot formation during ICF implosions.


Physics of Plasmas | 2018

Exploring the limits of case-to-capsule ratio, pulse length, and picket energy for symmetric hohlraum drive on the National Ignition Facility Laser

D. A. Callahan; O. A. Hurricane; J. E. Ralph; C. A. Thomas; K. L. Baker; L. R. Benedetti; L. Berzak Hopkins; D. T. Casey; T. Chapman; C. E. Czajka; E. L. Dewald; L. Divol; T. Döppner; D. E. Hinkel; M. Hohenberger; L. C. Jarrott; S. F. Khan; A. L. Kritcher; O. L. Landen; S. LePape; S. A. MacLaren; L. Masse; N. B. Meezan; A. Pak; J. D. Salmonson; D. T. Woods; N. Izumi; T. Ma; D. A. Mariscal; S. R. Nagel

We present a data-based model for low mode asymmetry in low gas-fill hohlraum experiments on the National Ignition Facility {NIF [Moses et al., Fusion Sci. Technol. 69, 1 (2016)]} laser. This model is based on the hypothesis that the asymmetry in these low fill hohlraums is dominated by the hydrodynamics of the expanding, low density, high-Z (gold or uranium) “bubble,” which occurs where the intense outer cone laser beams hit the high-Z hohlraum wall. We developed a simple model which states that the implosion symmetry becomes more oblate as the high-Z bubble size becomes large compared to the hohlraum radius or the capsule size becomes large compared to the hohlraum radius. This simple model captures the trends that we see in data that span much of the parameter space of interest for NIF ignition experiments. We are now using this model as a constraint on new designs for experiments on the NIF.


Physics of Plasmas | 2018

Capsule physics comparison of National Ignition Facility implosion designs using plastic, high density carbon, and beryllium ablators

D. S. Clark; A. L. Kritcher; S. A. Yi; A. Zylstra; S. W. Haan; C. R. Weber

Indirect drive implosion experiments on the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)] have now tested three different ablator materials: glow discharge polymer plastic, high density carbon, and beryllium. How do these different ablators compare in current and proposed implosion experiments on NIF? What are the relative advantages and disadvantages of each? This paper compares these different ablator options in capsule-only simulations of current NIF experiments and potential future designs. The simulations compare the impact of the capsule fill tube, support tent, and interface surface roughness for each case, as well as all perturbations in combination. According to the simulations, each ablator is impacted by the various perturbation sources differently, and each material poses unique challenges in the pursuit of ignition on NIF.


Physics of Plasmas | 2017

Performance of beryllium targets with full-scale capsules in low-fill 6.72-mm hohlraums on the National Ignition Facility

Andrei N. Simakov; D. C. Wilson; S. A. Yi; E. N. Loomis; J. L. Kline; G. A. Kyrala; A. Zylstra; E. L. Dewald; R. Tommasini; J. E. Ralph; D. J. Strozzi; A. G. MacPhee; J. L. Milovich; J. R. Rygg; S. F. Khan; T. Ma; L. C. Jarrott; S. W. Haan; Peter M. Celliers; M. M. Marinak; H. G. Rinderknecht; H. F. Robey; J. D. Salmonson; Michael Stadermann; S. Baxamusa; C. S. Alford; Y. Wang; A. Nikroo; N. Rice; C. Kong

When used with 1.06-mm beryllium (Be) capsules on the National Ignition Facility, gold hohlraums with the inner diameter of 5.75 mm and helium gas fill density of 1.6 mg/cm3 exhibit significant drive degradation due to laser energy backscatter (of order 14%–17%) and “missing” X-ray drive energy (about 32% during the main pulse). Also, hard to simulate cross-beam energy transfer (CBET) must be used to control the implosion symmetry. Larger, 6.72-mm hohlraums with fill densities ≤0.6 mg/cm3 generally offer improved drive efficiency, reduced hot-electron preheat, and better control of the implosion symmetry without CBET. Recently, we carried out an exploratory campaign to evaluate performance of 1.06-mm Be capsules in such hohlraums and determine optimal hohlraum parameters. Specifically, we performed a hohlraum fill-density scan with a three-shock, 9.5-ns laser pulse and found that an appropriate axial laser repointing and azimuthal outer-quad splitting resulted in significantly improved hohlraum energetics...


Journal of Physics: Conference Series | 2016

Indirect-drive ablative Richtmyer Meshkov node scaling

O. L. Landen; K. L. Baker; D. S. Clark; V N Goncharov; B. A. Hammel; D. Ho; O. A. Hurricane; J. D. Lindl; E N Loomis; L Masse; C Mauche; J. L. Milovich; J. L. Peterson; V. A. Smalyuk; S. A. Yi; A L Velikovich; C. R. Weber

The ablation front Rayleigh Taylor hydroinstability growth dispersion curve for indirect-drive implosions has been shown to be dependent on the Richtmyer Meshkov growth during the first shock transit phase. In this paper, a simplified treatment of the first shock ablative Richtmyer-Meshkov (ARM) growth dispersion curve is used to extract differences in ablation front perturbation growth behavior as function of foot pulse shape and ablator material for comparing the merits of various ICF design option.


Physics of Plasmas | 2017

The effects of convergence ratio on the implosion behavior of DT layered inertial confinement fusion capsules

Brian M. Haines; S. A. Yi; R. E. Olson; S. F. Khan; G. A. Kyrala; A. Zylstra; P. A. Bradley; Robert R. Peterson; J. L. Kline; R. J. Leeper; R. C. Shah

The wetted foam capsule design for inertial confinement fusion capsules, which includes a foam layer wetted with deuterium-tritium liquid, enables layered capsule implosions with a wide range of hot-spot convergence ratios (CR) on the National Ignition Facility. We present a full-scale wetted foam capsule design that demonstrates high gain in one-dimensional simulations. In these simulations, increasing the convergence ratio leads to an improved capsule yield due to higher hot-spot temperatures and increased fuel areal density. High-resolution two-dimensional simulations of this design are presented with detailed and well resolved models for the capsule fill tube, support tent, surface roughness, and predicted asymmetries in the x-ray drive. Our modeling of these asymmetries is validated by comparisons with available experimental data. In 2D simulations of the full-scale wetted foam capsule design, jetting caused by the fill tube is prevented by the expansion of the tungsten-doped shell layer due to prehe...


Journal of Physics: Conference Series | 2016

Wetted foam liquid fuel ICF target experiments

R. E. Olson; R. J. Leeper; S. A. Yi; J. L. Kline; A. Zylstra; Robert R. Peterson; R. C. Shah; T. Braun; Juergen Biener; B. J. Kozioziemski; J. Sater; M. M. Biener; Alex V. Hamza; A. Nikroo; L. Berzak Hopkins; D. Ho; S. LePape; N. B. Meezan

We are developing a new NIF experimental platform that employs wetted foam liquid fuel layer ICF capsules. We will use the liquid fuel layer capsules in a NIF sub-scale experimental campaign to explore the relationship between hot spot convergence ratio (CR) and the predictability of hot spot formation. DT liquid layer ICF capsules allow for flexibility in hot spot CR via the adjustment of the initial cryogenic capsule temperature and, hence, DT vapor density. Our hypothesis is that the predictive capability of hot spot formation is robust and 1D-like for a relatively low CR hot spot (CR~15), but will become less reliable as hot spot CR is increased to CR>20. Simulations indicate that backing off on hot spot CR is an excellent way to reduce capsule instability growth and to improve robustness to low-mode x-ray flux asymmetries. In the initial experiments, we will test our hypothesis by measuring hot spot size, neutron yield, ion temperature, and burn width to infer hot spot pressure and compare to predictions for implosions with hot spot CRs in the range of 12 to 25. Larger scale experiments are also being designed, and we will advance from sub-scale to full-scale NIF experiments to determine if 1D-like behavior at low CR is retained as the scale-size is increased. The long-term objective is to develop a liquid fuel layer ICF capsule platform with robust thermonuclear burn, modest CR, and significant α-heating with burn propagation.


Physics of Plasmas | 2018

Comparison of plastic, high density carbon, and beryllium as indirect drive NIF ablators

A. L. Kritcher; D. S. Clark; S. W. Haan; S. A. Yi; A. Zylstra; D. A. Callahan; D. E. Hinkel; L. Berzak Hopkins; O. A. Hurricane; O. L. Landen; S. A. MacLaren; N. B. Meezan; P. K. Patel; J. E. Ralph; C. A. Thomas; R. P. J. Town; M. J. Edwards

Detailed radiation hydrodynamic simulations calibrated to experimental data have been used to compare the relative strengths and weaknesses of three candidate indirect drive ablator materials now tested at the NIF: plastic, high density carbon or diamond, and beryllium. We apply a common simulation methodology to several currently fielded ablator platforms to benchmark the model and extrapolate designs to the full NIF envelope to compare on a more equal footing. This paper focuses on modeling of the hohlraum energetics which accurately reproduced measured changes in symmetry when changes to the hohlraum environment were made within a given platform. Calculations suggest that all three ablator materials can achieve a symmetric implosion at a capsule outer radius of ∼1100 μm, a laser energy of 1.8 MJ, and a DT ice mass of 185 μg. However, there is more uncertainty in the symmetry predictions for the plastic and beryllium designs. Scaled diamond designs had the most calculated margin for achieving symmetry a...

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J. L. Kline

Los Alamos National Laboratory

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D. C. Wilson

Los Alamos National Laboratory

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S. H. Batha

Los Alamos National Laboratory

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G. A. Kyrala

Los Alamos National Laboratory

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A. Zylstra

Los Alamos National Laboratory

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Andrei N. Simakov

Los Alamos National Laboratory

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J. L. Milovich

Lawrence Livermore National Laboratory

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J. E. Ralph

Lawrence Livermore National Laboratory

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D. S. Clark

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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