D. Turnbull
Lawrence Livermore National Laboratory
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Featured researches published by D. Turnbull.
Physics of Plasmas | 2016
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.
Physics of Plasmas | 2016
D. Turnbull; L. Berzak Hopkins; S. Le Pape; L. Divol; N. B. Meezan; O. L. Landen; D. Ho; A. J. Mackinnon; Alex Zylstra; H. G. Rinderknecht; H. Sio; R. D. Petrasso; J. S. Ross; S. F. Khan; A. Pak; E. L. Dewald; D. A. Callahan; O. A. Hurricane; W. W. Hsing; M. J. Edwards
Controlling the symmetry of indirect-drive inertial confinement fusion implosions remains a key challenge. Increasing the ratio of the hohlraum diameter to the capsule diameter (case-to-capsule ratio, or CCR) facilitates symmetry tuning. By varying the balance of energy between the inner and outer cones as well as the incident laser pulse length, we demonstrate the ability to tune from oblate, through round, to prolate at a CCR of 3.2 in near-vacuum hohlraums at the National Ignition Facility, developing empirical playbooks along the way for cone fraction sensitivity of various laser pulse epochs. Radiation-hydrodynamic simulations with enhanced inner beam propagation reproduce most experimental observables, including hot spot shape, for a majority of implosions. Specular reflections are used to diagnose the limits of inner beam propagation as a function of pulse length.
Physics of Plasmas | 2016
V. A. Smalyuk; H. F. Robey; T. Döppner; D. T. Casey; D. S. Clark; O. S. Jones; J. L. Milovich; J. L. Peterson; B. Bachmann; K. L. Baker; L. R. Benedetti; L. Berzak Hopkins; R. Bionta; E. Bond; D. K. Bradley; D. A. Callahan; Peter M. Celliers; C. Cerjan; K. C. Chen; C. Goyon; G. P. Grim; S. Dixit; M. J. Eckart; M. J. Edwards; M. Farrell; D. N. Fittinghoff; J. A. Frenje; M. Gatu-Johnson; N. Gharibyan; S. W. Haan
Radiation-driven, layered deuterium-tritium (DT) implosions were carried out using 3-shock and 4-shock “adiabat-shaped” drives and plastic ablators on the National Ignition Facility (NIF) [E. M. Campbell et al., AIP Conf. Proc. 429, 3 (1998)]. The purpose of these shots was to gain further understanding on the relative performance of the low-foot implosions of the National Ignition Campaign [M. J. Edwards et al., Phys. Plasmas 20, 070501 (2013)] versus the subsequent high-foot implosions [T. Doppner et al., Phys. Rev. Lett. 115, 055001 (2015)]. The neutron yield performance in the experiment with the 4-shock adiabat-shaped drive was improved by factors ∼3 to ∼10, compared to five companion low-foot shots despite large low-mode asymmetries of DT fuel, while measured compression was similar to its low-foot companions. This indicated that the dominant degradation source for low-foot implosions was ablation-front instability growth, since adiabat shaping significantly stabilized this growth. For the experiment with the low-power 3-shock adiabat-shaped drive, the DT fuel compression was significantly increased, by ∼25% to ∼36%, compared to its companion high-foot implosions. The neutron yield increased by ∼20%, lower than the increase of ∼50% estimated from one-dimensional scaling, suggesting the importance of residual instabilities and asymmetries. For the experiment with the high-power, 3-shock adiabat-shaped drive, the DT fuel compression was slightly increased by ∼14% compared to its companion high-foot experiments. However, the compression was reduced compared to the lower-power 3-shock adiabat-shaped drive, correlated with the increase of hot electrons that hypothetically can be responsible for reduced compression in high-power adiabat-shaped experiments as well as in high-foot experiments. The total neutron yield in the high-power 3-shock adiabat-shaped shot N150416 was 8.5 × 1015 ± 0.2 × 1015, with the fuel areal density of 0.90 ± 0.07 g/cm2, corresponding to the ignition threshold factor parameter IFTX (calculated without alpha heating) of 0.34 ± 0.03 and the yield amplification due to the alpha heating of 2.4 ± 0.2. The performance parameters were among the highest of all shots on NIF and the closest to ignition at this time, based on the IFTX metric. The follow-up experiments were proposed to continue testing physics hypotheses, to measure implosion reproducibility, and to improve quantitative understanding on present implosion results.
Journal of Physics: Conference Series | 2016
O. S. Jones; C. A. Thomas; Peter A. Amendt; G. Hall; N. Izumi; M. A. Barrios Garcia; L. Berzak Hopkins; H. Chen; E. L. Dewald; D. E. Hinkel; A. L. Kritcher; M. M. Marinak; N. B. Meezan; J. L. Milovich; J. D. Moody; A. S. Moore; Mehul Patel; J. E. Ralph; S. P. Regan; M. D. Rosen; M. B. Schneider; S. M. Sepke; D. J. Strozzi; D. Turnbull
We have found that radiation-hydrodynamic calculations that use the high flux model assumptions [1] can accurately predict the radiation drive produced by a laser-heated hohlraum under certain conditions, but can not predict drive over a broad range of parameters (pulse energy, hohlraum gas fill density, hohlraum case-to-capsule ratio). In particular, the model is accurate for ~7 ns long laser pulses used to implode capsules with high density carbon (HDC) ablators in hohlraums with helium fill gas densities of 0-0.6 mg/cc. By systematically varying the gas fill density from 0 to 1.6 mg/cc we found that the agreement with drive begins to diverge for fills > 0.85 mg/cc. This divergence from the model coincides with the onset of measureable SRS backscatter. In this same set of experiments the radiation drive symmetry inferred from the imploded shape of a gas-filled capsule is not predicted with this model. Finally, several possible fixes to the model to reduce the observed discrepancies are considered.
Physics of Plasmas | 2017
G. Hall; O. S. Jones; D. J. Strozzi; J. D. Moody; D. Turnbull; J. E. Ralph; P. Michel; M. Hohenberger; A. S. Moore; O. L. Landen; L. Divol; David K. Bradley; D. E. Hinkel; A. J. Mackinnon; R. P. J. Town; N. B. Meezan; L. Berzak Hopkins; N. Izumi
Indirect drive inertial confinement fusion experiments were conducted at the National Ignition Facility to investigate the performance of the hohlraum drive as a function of hohlraum gas fill density by imploding high-density-carbon capsules using a 2-shock laser pulse. Measurements characterized the backscatter behavior, the production of hot electrons, the motion and brightness of the laser spots on the hohlraum wall, and the efficiency of the hohlraum x-ray drive as a function of gas fill density ρgf between 0.03 mg/cc (“near vacuum”) and 1.6 mg/cc. For hohlraums with ρgf up to 0.85 mg/cc, very little stimulated Raman backscatter (SRS) was observed. For higher ρgf, significant SRS was produced and was observed to occur during the rise to peak laser power and throughout the main pulse. The efficiency with which laser energy absorbed by the hohlraum is converted into drive energy was measured to be the same for ρgf ≥ 0.6 mg/cc once the laser reached peak power. However, for the near vacuum case, the abso...
Physics of Plasmas | 2016
S. F. Khan; S. A. MacLaren; J. D. Salmonson; T. Ma; G. A. Kyrala; J. Pino; J. R. Rygg; J. E. Field; R. Tommasini; J. E. Ralph; D. Turnbull; A. J. Mackinnon; K. L. Baker; L. R. Benedetti; D. K. Bradley; Peter M. Celliers; E. L. Dewald; T. R. Dittrich; L. Berzak Hopkins; N. Izumi; M. L. Kervin; J. L. Kline; S. R. Nagel; A. Pak; Robert Tipton
We introduce a new quasi 1-D implosion experimental platform at the National Ignition Facility designed to validate physics models as well as to study various Inertial Confinement Fusion aspects such as implosion symmetry, convergence, hydrodynamic instabilities, and shock timing. The platform has been developed to maintain shell sphericity throughout the compression phase and produce a round hot core at stagnation. This platform utilizes a 2-shock 1 MJ pulse with 340 TW peak power in a near-vacuum Au Hohlraum and a CH ablator capsule uniformly doped with 1% Si. We have performed several inflight radiography, symmetry capsule, and shock timing experiments in order to tune the symmetry of the capsule to near round throughout several epochs of the implosion. Adjusting the relative powers of the inner and outer cones of beams has allowed us to control the drive at the poles and equator of the capsule, thus providing the mechanism to achieve a spherical capsule convergence. Details and results of the tuning e...
Physical Review Letters | 2016
D. Turnbull; P. Michel; T. Chapman; E. Tubman; B. B. Pollock; C. Y. Chen; Clement Goyon; J. S. Ross; L. Divol; N. Woolsey; J. D. Moody
We report the first experimental demonstration of a plasma wave plate based on laser-induced birefringence. An elliptically polarized input was converted into a nearly ideal circularly polarized beam using an optical system composed of a second laser beam and a plasma. The results are in excellent agreement with linear theory and three-dimensional simulations up to phase delays exceeding π/4, thus establishing the feasibility of laser-plasma photonic devices that are ultrafast, damage-resistant, and easily tunable.
Physics of Plasmas | 2014
T. Ma; L. B. Fletcher; A. Pak; D. A. Chapman; R. W. Falcone; C. Fortmann; E. Galtier; Dirk O. Gericke; G. Gregori; J. B. Hastings; O. L. Landen; S. Le Pape; H. J. Lee; B. Nagler; P. Neumayer; D. Turnbull; Jan Vorberger; T. G. White; Kathrin Wünsch; U. Zastrau; Siegfried H. Glenzer; T. Döppner
Using simultaneous spectrally, angularly, and temporally resolved x-ray scattering, we measure the pronounced ion-ion correlation peak in a strongly coupled plasma. Laser-driven shock-compressed aluminum at ∼3× solid density is probed with high-energy photons at 17.9 keV created by molybdenum He-α emission in a laser-driven plasma source. The measured elastic scattering feature shows a well-pronounced correlation peak at a wave vector of k=4A−1. The magnitude of this correlation peak cannot be described by standard plasma theories employing a linear screened Coulomb potential. Advanced models, including a strong short-range repulsion due to the inner structure of the aluminum ions are however in good agreement with the scattering data. These studies have demonstrated a new highly accurate diagnostic technique to directly measure the state of compression and the ion-ion correlations. We have since applied this new method in single-shot wave-number resolved S(k) measurements to characterize the physical pro...
Physical Review Letters | 2018
J.A. Marozas; M. Hohenberger; M. Rosenberg; D. Turnbull; T.J.B. Collins; P. B. Radha; P.W. McKenty; Jonathan D. Zuegel; F. J. Marshall; S. P. Regan; T. C. Sangster; W. Seka; E. M. Campbell; V.N. Goncharov; M. W. Bowers; J. M. G. Di Nicola; Gaylen V. Erbert; B. J. MacGowan; L. J. Pelz; Steven T. Yang
Cross-beam energy transfer (CBET) results from two-beam energy exchange via seeded stimulated Brillouin scattering, which detrimentally reduces ablation pressure and implosion velocity in direct-drive inertial confinement fusion. Mitigating CBET is demonstrated for the first time in inertial-confinement implosions at the National Ignition Facility by detuning the laser-source wavelengths (±2.3 Å UV) of the interacting beams. We show that, in polar direct-drive, wavelength detuning increases the equatorial region velocity experimentally by 16% and alters the in-flight shell morphology. These experimental observations are consistent with design predictions of radiation-hydrodynamic simulations that indicate a 10% increase in the average ablation pressure.
Physical Review Letters | 2017
D. Turnbull; Clement Goyon; G.E. Kemp; B. B. Pollock; D. Mariscal; L. Divol; J. S. Ross; S. Patankar; J. D. Moody; P. Michel
We report the first complete set of measurements of a laser-plasma optical systems refractive index, as seen by a second probe laser beam, as a function of the relative wavelength shift between the two laser beams. Both the imaginary and real refractive index components are found to be in good agreement with linear theory using plasma parameters measured by optical Thomson scattering and interferometry; the former is in contrast to previous work and has implications for crossed-beam energy transfer in indirect-drive inertial confinement fusion, and the latter is measured for the first time. The data include the first demonstration of a laser-plasma polarizer with 85%-87% extinction for the particular laser and plasma parameters used in this experiment, complementing the existing suite of high-power, tunable, and ultrafast plasma-based photonic devices.