N. Rice
General Atomics
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Featured researches published by N. Rice.
Physics of Plasmas | 2017
L. Divol; A. Pak; L. Berzak Hopkins; S. Le Pape; N. B. Meezan; E. L. Dewald; D. Ho; S. F. Khan; A. J. Mackinnon; J. S. Ross; D. P. Turnbull; C. R. Weber; Peter M. Celliers; M. Millot; L. R. Benedetti; J. E. Field; N. Izumi; G. A. Kyrala; T. Ma; S. R. Nagel; J. R. Rygg; D. H. Edgell; A. G. MacPhee; C. Goyon; M. Hohenberger; B. J. MacGowan; P. Michel; D. J. Strozzi; W. S. Cassata; D. T. Casey
We report on the most recent and successful effort at controlling the trajectory and symmetry of a high density carbon implosion at the National Ignition Facility. We use a low gasfill (0.3 mg/cc He) bare depleted uranium hohlraum with around 1 MJ of laser energy to drive a 3-shock-ignition relevant implosion. We assess drive performance and we demonstrate symmetry control at convergence 1, 3–5, 12, and 27 to better than ±5 μm using a succession of experimental platforms. The symmetry control was maintained at a peak fuel velocity of 380 km/s. Overall, implosion symmetry measurements are consistent with the pole-equator symmetry of the X-ray drive on the capsule being better than 5% in the foot of the drive (when shocks are launched) and better than 1% during peak drive (main acceleration phase). This level of residual asymmetry should have little impact on implosion performance.
Physics of Plasmas | 2016
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 | 2017
C. R. Weber; D. T. Casey; D. S. Clark; B. A. Hammel; A. G. MacPhee; J. L. Milovich; D. Martinez; H. F. Robey; V. A. Smalyuk; Michael Stadermann; Peter A. Amendt; S. Bhandarkar; B. Chang; C. Choate; J. Crippen; S. Felker; J. E. Field; S. W. Haan; S. Johnson; J. J. Kroll; O. L. Landen; M. M. Marinak; M. Mcinnis; A. Nikroo; N. Rice; S. M. Sepke
The thin membrane that holds the capsule in-place in the hohlraum is recognized as one of the most significant contributors to reduced performance in indirect drive inertial confinement fusion (ICF) experiments on the National Ignition Facility. This membrane, known as the “tent,” seeds a perturbation that is amplified by Rayleigh-Taylor and can rupture the capsule. A less damaging capsule support mechanism is under development. Possible alternatives include the micron-scale rods spanning the hohlraum width and supporting either the capsule or stiffening the fill-tube, a larger fill-tube to both fill and support the capsule, or a low-density foam layer that protects the capsule from the tent impact. Experiments are testing these support features to measure their imprint on the capsule. These experiments are revealing unexpected aspects about perturbation development in indirect drive ICF, such as the importance of shadows coming from bright spots in the hohlraum. Two dimensional and 3D models are used to ...
Physics of Plasmas | 2017
V. A. Smalyuk; C. R. Weber; H. F. Robey; D. T. Casey; K. C. Chen; D. S. Clark; M. Farrell; S. Felker; J. E. Field; S. W. Haan; B. A. Hammel; Alex V. Hamza; D. Hoover; J. J. Kroll; O. L. Landen; A. G. MacPhee; D. Martinez; A. Nikroo; N. Rice
Hydrodynamic instability growth has been studied using three-dimensional (3-D) broadband modulations by comparing “high-foot” and “low-foot” spherical plastic (CH) capsule implosions at the National Ignition Facility (NIF) [E. M. Campbell et al., AIP Conf. Proc. 429, 3 (1998)]. The initial perturbations included capsule outer-surface roughness and capsule-mounting membranes (“tents”) that were similar to those used in a majority of implosions on NIF. The tents with thicknesses of 31-nm, 46-nm, and 109-nm were used in the experiments. The outer-surface roughness in the “low-foot” experiment was similar to the standard specification, while it was increased by ∼4 times in the “high-foot” experiment to compensate for the reduced growth. The ablation-front instability growth was measured using a Hydrodynamic Growth Radiography platform at a convergence ratio of ∼3. The dominant capsule perturbations, generated by the tent mountings, had measured perturbation amplitudes comparable to the capsule thickness with ...
Physics of Plasmas | 2017
D. Martinez; V. A. Smalyuk; A. G. MacPhee; J. L. Milovich; D. T. Casey; C. R. Weber; H. F. Robey; K. C. Chen; D. S. Clark; J. Crippen; M. Farrell; S. Felker; J. E. Field; S. W. Haan; B. A. Hammel; Alex V. Hamza; Michael Stadermann; W. W. Hsing; J. J. Kroll; O. L. Landen; A. Nikroo; L. A. Pickworth; N. Rice
Hydrodynamic instability growth of the capsule support membranes (or “tents”) and fill tubes has been studied in spherical, glow discharge polymer plastic capsule implosions at the National Ignition Facility (NIF) [Campbell et al., AIP Conf. Proc. 429, 3 (1998)]. In NIF implosions, the capsules are supported by tents because the nominal 10-μm thick fill tubes are not strong enough to support capsules by themselves. After it was recognized that the tents had a significant impact of implosion stability, new support methods were investigated, including thicker, 30-μm diameter fill tubes and cantilevered fill tubes, as described in this article. A new “sub-scale” version of the existing x-ray radiography platform was developed for measuring growing capsule perturbations in the acceleration phase of implosions. It was calibrated using hydrodynamic growth measurements of pre-imposed capsule modulations with Legendre modes of 60, 90, 110, and 140 at convergence ratios up to ∼2.4. Subsequent experiments with 3-D ...
Physics of Plasmas | 2017
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...
Physics of Plasmas | 2018
D. T. Casey; C. A. Thomas; K. L. Baker; B. K. Spears; M. Hohenberger; S. F. Khan; R. Nora; C. R. Weber; D. T. Woods; O. A. Hurricane; D. A. Callahan; R. L. Berger; J. L. Milovich; P. K. Patel; T. Ma; A. Pak; L. R. Benedetti; M. Millot; C. Jarrott; O. L. Landen; R. Bionta; B. J. MacGowan; D. J. Strozzi; Michael Stadermann; Juergen Biener; A. Nikroo; Clement Goyon; N. Izumi; S. R. Nagel; B. Bachmann
The Bigfoot approach is to intentionally trade off high convergence, and therefore areal-density, in favor of high implosion velocity and good coupling between the laser, hohlraum, shell, and hotspot. This results in a short laser pulse that improves hohlraum symmetry and predictability, while the reduced compression reduces hydrodynamic instability growth. The results thus far include demonstrated low-mode symmetry control at two different hohlraum geometries (5.75 mm and 5.4 mm diameters) and at two different target scales (5.4 mm and 6.0 mm hohlraum diameters) spanning 300–405 TW in laser power and 0.8–1.6 MJ in laser energy. Additionally, by carefully scaling the 5.4 mm design to 6.0 mm, an increase in target scale of 13%, equivalent to 40% increase in laser energy, has been demonstrated.
Physics of Plasmas | 2018
A. G. MacPhee; V. A. Smalyuk; O. L. Landen; C. R. Weber; H. F. Robey; E. L. Alfonso; Juergen Biener; T. Bunn; J. Crippen; M. Farrell; S. Felker; J. E. Field; W. W. Hsing; C. Kong; J. L. Milovich; A. S. Moore; A. Nikroo; N. Rice; Michael Stadermann; C. Wild
We report a reduced X-ray shadow imprint of hydrodynamic instabilities on the high-density carbon ablator surface of inertial confinement fusion (ICF) capsules using a reduced diameter fuel fill tube on the National Ignition Facility (NIF). The perturbation seed mass from hydrodynamic instabilities was reduced by approximately an order of magnitude by reducing both the diameter and wall thickness of the fill tube by ∼2×, consistent with analytical estimates. This work demonstrates a successful mitigation strategy for engineered features for ICF implosions on the NIF.
Fusion Science and Technology | 2018
N. Rice; Matthew Vu; C. Kong; M. P. Mauldin; A. Tambazidis; M. L. Hoppe; P. Fitzsimmons; M. Farrell; D. S. Clark; E. L. Dewald; V. A. Smalyuk
Abstract Capsule drive in National Ignition Facility indirect-drive implosions is generated by X-ray illumination from cylindrical hohlraums. The cylindrical hohlraum geometry is axially symmetric but not spherically symmetric, causing capsule–fuel drive asymmetries. It is hypothesized that fabricating capsules asymmetric in wall thickness (shimmed) may compensate for drive asymmetries and improve implosion symmetry. Simulations suggest that for high-compression implosions, Legendre mode P4 hohlraum flux asymmetries are the most detrimental to implosion performance. General Atomics has developed a diamond-turning method to form a glow discharge polymer capsule outer surface to a Legendre mode P4 profile. The P4 shape requires full capsule surface coverage. As a result, in order to avoid tool-lathe interference, flipping the capsule part way through the machining process is required. This flipping process risks misalignment of the capsule, causing a vertical step feature on the capsule surface. Recent trials have proven this step feature height can be minimized to ~0.25 µm.
Fusion Science and Technology | 2016
E. Giraldez; M. L. Hoppe; D. E. Hoover; A. Q. L. Nguyen; N. Rice; A. M. Garcia; H. Huang; M. P. Mauldin; M. Farrell; A. Nikroo; V. A. Smalyuk
Abstract Hydrodynamic instability growth and its effects on capsule implosion performance are being studied at the National Ignition Facility (NIF). Experimental results have shown that low-mode instabilities are the primary culprit for yield degradation. Ignition-type capsules with machined two-dimensional (2-D) sinusoidal defects were used to measure low-mode hydrodynamic instability growth in the acceleration phase of the capsule implosion. The capsules were imploded using ignition-relevant laser pulses and the ablation-front modulation growth was measured using X-ray radiography. The experimentally measured growth was in good agreement with simulations. Fabrication of the preimposed 2-D sinusoidal defects of different wavelengths and amplitudes on the surfaces of ignition-type capsules was accomplished by General Atomics leading up to and during the Hydro-Growth Radiography campaign for the hydrodynamic instability growth experiments conducted at NIF between 2013 and 2014. The 2-D sinusoidal defects were imposed on ignition-type capsules by machining the surface of the capsule. The fabrication trials showed that there are six parameters that can affect the ripple form, wall thickness, and the extent of the pattern about the equator of the capsule: (1) knowing accurately the outer diameter of the capsule, (2) the roundness of the capsule (modal content), (3) the cutting tool alignment with respect to the surface of the capsule, (4) the radius and form of the cutting tool, (5) tool touch-off, and (6) the runout of the capsule center with respect to the axis of rotation of the lathe’s spindle. In this paper, we will describe the importance of these parameters on the machining of uniform 2-D sinusoidal defects.