L. Masse
Lawrence Livermore National Laboratory
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Featured researches published by L. Masse.
Physics of Plasmas | 2012
A. Casner; V. A. Smalyuk; L. Masse; I. Igumenshchev; S. Liberatore; L. Jacquet; C. Chicanne; P. Loiseau; O. Poujade; D. K. Bradley; H.-S. Park; B. A. Remington
We present two designs relevant to ablative Rayleigh-Taylor instability in transition from weakly nonlinear to highly nonlinear regimes at the National Ignition Facility [E. I. Moses, J. Phys.: Conf. Ser. 112, 012003 (2008)]. The sensitivity of nonlinear Rayleigh-Taylor instability physics to ablation velocity is addressed with targets driven by indirect drive, with stronger ablative stabilization, and by direct drive, with weaker ablative stabilization. The indirect drive design demonstrates the potential to reach a two-dimensional bubble-merger regime with a 20 ns duration drive at moderate radiation temperature. The direct drive design achieves a 3 to 5 times increased acceleration distance for the sample in comparison to previous experiments allowing at least 2 more bubble generations when starting from a three-dimensional broadband spectrum.
Physics of Plasmas | 2018
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 | 2017
M. Gatu Johnson; A. Zylstra; A. Bacher; C. R. Brune; D. T. Casey; C.J. Forrest; H. W. Herrmann; M. Hohenberger; D. B. Sayre; R. Bionta; J.-L. Bourgade; J. A. Caggiano; Charles Cerjan; R. S. Craxton; D. Dearborn; M. Farrell; J. A. Frenje; E. M. Garcia; V. Yu. Glebov; Gerald M. Hale; Edward P. Hartouni; R. Hatarik; M. Hohensee; D. M. Holunga; M. L. Hoppe; R. Janezic; S. F. Khan; J. D. Kilkenny; Y. Kim; J. P. Knauer
This paper describes the development of a platform to study astrophysically relevant nuclear reactions using inertial-confinement fusion implosions on the OMEGA and National Ignition Facility laser facilities, with a particular focus on optimizing the implosions to study charged-particle-producing reactions. Primary requirements on the platform are high yield, for high statistics in the fusion product measurements, combined with low areal density, to allow the charged fusion products to escape. This is optimally achieved with direct-drive exploding pusher implosions using thin-glass-shell capsules. Mitigation strategies to eliminate a possible target sheath potential which would accelerate the emitted ions are discussed. The potential impact of kinetic effects on the implosions is also considered. The platform is initially employed to study the complementary T(t,2n)α, T(3He,np)α and 3He(3He,2p)α reactions. Proof-of-principle results from the first experiments demonstrating the ability to accurately measur...
Physics of Plasmas | 2015
A. Casner; L. Masse; S. Liberatore; P. Loiseau; P. E. Masson-Laborde; L. Jacquet; D. Martinez; A. S. Moore; R. Seugling; S. Felker; S. W. Haan; B. A. Remington; V. A. Smalyuk; M. Farrell; E. Giraldez; A. Nikroo
Academic tests in physical regimes not encountered in Inertial Confinement Fusion will help to build a better understanding of hydrodynamic instabilities and constitute the scientifically grounded validation complementary to fully integrated experiments. Under the National Ignition Facility (NIF) Discovery Science program, recent indirect drive experiments have been carried out to study the ablative Rayleigh-Taylor Instability (RTI) in transition from weakly nonlinear to highly nonlinear regime [A. Casner et al., Phys. Plasmas 19, 082708 (2012)]. In these experiments, a modulated package is accelerated by a 175 eV radiative temperature plateau created by a room temperature gas-filled platform irradiated by 60 NIF laser beams. The unique capabilities of the NIF are harnessed to accelerate this planar sample over much larger distances ( ≃1.4 mm) and longer time periods ( ≃12 ns) than previously achieved. This extended acceleration could eventually allow entering into a turbulent-like regime not precluded by...
Physics of Plasmas | 2018
M. Gatu Johnson; D. T. Casey; M. Hohenberger; A. Zylstra; Andrew Bacher; C. R. Brune; R. Bionta; R. S. Craxton; C. L. Ellison; M. Farrell; J. A. Frenje; Warren Garbett; E. M. Garcia; G. P. Grim; Edward P. Hartouni; R. Hatarik; H. W. Herrmann; M. Hohensee; D. M. Holunga; M. L. Hoppe; M. C. Jackson; N. Kabadi; S. F. Khan; J. D. Kilkenny; T. R. Kohut; B. Lahmann; Hai P. Le; C. K. Li; L. Masse; P.W. McKenty
Polar-direct-drive exploding pushers are used as a high-yield, low-areal-density fusion product source at the National Ignition Facility with applications including diagnostic calibration, nuclear security, backlighting, electron-ion equilibration, and nucleosynthesis-relevant experiments. In this paper, two different paths to improving the performance of this platform are explored: (i) optimizing the laser drive, and (ii) optimizing the target. While the present study is specifically geared towards nucleosynthesis experiments, the results are generally applicable. Example data from T2/3He-gas-filled implosions with trace deuterium are used to show that yield and ion temperature (Tion) from 1.6 mm-outer-diameter thin-glass-shell capsule implosions are improved at a set laser energy by switching from a ramped to a square laser pulse shape, and that increased laser energy further improves yield and Tion, although by factors lower than predicted by 1 D simulations. Using data from D2/3He-gas-filled implosion...
Physics of Plasmas | 2018
E. N. Loomis; S. A. Yi; G. A. Kyrala; J. L. Kline; Andrei N. Simakov; J. E. Ralph; M. Millot; E. Dewald; A. Zylstra; J. R. Rygg; Peter M. Celliers; C. Goyon; B. Lahmann; H. Sio; S. A. MacLaren; L. Masse; D. A. Callahan; O. A. Hurricane; D. C. Wilson; N. Rice; H. Huang; C. Kong; J. Bae; A. Nikroo; S. H. Batha
Experiments at the National Ignition Facility (NIF) show that the implosion shape of inertial confinement fusion ablators is a key factor limiting performance. To achieve more predictable, shape tunable implosions, we have designed and fielded a large 4.2 case-to-capsule ratio target at the NIF using 6.72 mm diameter Au hohlraums and 1.6 mm diameter Cu-doped Be capsules. Simulations show that at these dimensions during a 10 ns 3-shock laser pulse reaching 275 eV hohlraum temperatures, the plasma flow from the hohlraum wall and ablator is not significant enough to impede beam propagation. Experiments measuring the shock symmetry and in-flight shell symmetry closely matched the simulations. Most notably, in two experiments, we demonstrated symmetry control from negative to positive Legendre P2 space by varying the inner to total laser power cone fraction by 5% below and above the predicted symmetric value. Some discrepancies found in 1st shock arrival times that could affect agreement in late time implosion symmetry suggest hohlraum and capsule modeling uncertainties do remain, but this target design reduces sensitivities to them.Experiments at the National Ignition Facility (NIF) show that the implosion shape of inertial confinement fusion ablators is a key factor limiting performance. To achieve more predictable, shape tunable implosions, we have designed and fielded a large 4.2 case-to-capsule ratio target at the NIF using 6.72 mm diameter Au hohlraums and 1.6 mm diameter Cu-doped Be capsules. Simulations show that at these dimensions during a 10 ns 3-shock laser pulse reaching 275 eV hohlraum temperatures, the plasma flow from the hohlraum wall and ablator is not significant enough to impede beam propagation. Experiments measuring the shock symmetry and in-flight shell symmetry closely matched the simulations. Most notably, in two experiments, we demonstrated symmetry control from negative to positive Legendre P2 space by varying the inner to total laser power cone fraction by 5% below and above the predicted symmetric value. Some discrepancies found in 1st shock arrival times that could affect agreement in late time implosion...
Physics of Plasmas | 2018
G. A. Kyrala; J. Pino; S. F. Khan; S. A. MacLaren; J. D. Salmonson; T. Ma; L. Masse; Robert Tipton; P. A. Bradley; J. R. Rygg; J. E. Field; R. Tommasini; J. E. Ralph; D. Turnbull; A. J. Mackinnon; L. R. Benedetti; D. K. Bradley; S. R. Nagel; Peter M. Celliers; E. Dewald; T. R. Dittrich; L. Berzak Hopkins; N. Izumi; M. L. Kervin; J. L. Kline; C. B. Yeamans; R. Hatarik; D. B. Sayre; Edward P. Hartouni; A. Pak
We describe the use of a robust new 1-D like implosion platform at the National Ignition Facility [G. H. Miller et al., Opt. Eng. 43, 2841 (2004)] to study the effect of convergence on mix and shape. Previous experiments suggest that nuclear yields and ion temperature degrade with increased convergence [M. D. Cable et al., Phys. Rev. Lett. 73, 2316 (1994)] due to enhanced perturbation growth and mix, but little has been reported on the distortion of the shape with time. The 2-shock platform was developed [S. F. Khan et al., Phys. Plasmas 23, 042708 (2016)] to maintain a high degree of sphericity during the whole implosion phase and has a thick, uniformly doped (1% Si) plastic CH shell to minimize the effect of mixing due to hydrodynamic feed-through from the outer ablator surface. An inner layer of deuterated plastic (CD) and hydrogen-tritium (DT) gas fill allows for the measurement of DT neutrons produced by the mix between the gas and ablator. DD neutrons provide information about the hot, unmixed CD region. By changing the fill gas density while keeping the capsule diameter, ablator thickness, and Au hohlraum conditions fixed, the x-ray hot spot convergence ratio was varied from 14 to 22. We find that the atomic mix (DT yield) grows linearly as a function of convergence, but since Tion changes as well, it does not necessarily mean that the amount or extent of mix grows linearly as well. We also find the DD yield, which is a measurement of the shell heating, saturates above a certain convergence. We describe the use of a robust new 1-D like implosion platform at the National Ignition Facility [G. H. Miller et al., Opt. Eng. 43, 2841 (2004)] to study the effect of convergence on mix and shape. Previous experiments suggest that nuclear yields and ion temperature degrade with increased convergence [M. D. Cable et al., Phys. Rev. Lett. 73, 2316 (1994)] due to enhanced perturbation growth and mix, but little has been reported on the distortion of the shape with time. The 2-shock platform was developed [S. F. Khan et al., Phys. Plasmas 23, 042708 (2016)] to maintain a high degree of sphericity during the whole implosion phase and has a thick, uniformly doped (1% Si) plastic CH shell to minimize the effect of mixing due to hydrodynamic feed-through from the outer ablator surface. An inner layer of deuterated plastic (CD) and hydrogen-tritium (DT) gas fill allows for the measurement of DT neutrons produced by the mix between the gas and ablator. DD neutrons provide information about the hot, unmixed CD r...
Physics of Plasmas | 2018
S. A. MacLaren; L. Masse; C. E. Czajka; S. F. Khan; G. A. Kyrala; T. Ma; J. E. Ralph; J. D. Salmonson; B. Bachmann; L. R. Benedetti; S. Bhandarkar; P. A. Bradley; R. Hatarik; H. W. Herrmann; D. A. Mariscal; M. Millot; P. K. Patel; J. Pino; M. Ratledge; N. Rice; Robert Tipton; R. Tommasini; C. B. Yeamans
Inertial confinement fusion cryogenic-layered implosions at the National Ignition Facility, while successfully demonstrating self-heating due to alpha-particle deposition, have fallen short of the performance predicted by one-dimensional (1D) multi-physics implosion simulations. The current understanding, from experimental evidence as well as simulations, suggests that engineering features such as the capsule tent and fill tube, as well as time-dependent low-mode asymmetry, are to blame for the lack of agreement. A short series of experiments designed specifically to avoid these degradations to the implosion are described here in order to understand if, once they are removed, a high-convergence cryogenic-layered deuterium-tritium implosion can achieve the 1D simulated performance. The result is a cryogenic layered implosion, round at stagnation, that matches closely the performance predicted by 1D simulations. This agreement can then be exploited to examine the sensitivity of approximations in the model t...
Physics of Plasmas | 2018
A. Zylstra; S. A. Yi; S. A. MacLaren; J. L. Kline; G. A. Kyrala; J. E. Ralph; J. Bae; S. H. Batha; D. A. Callahan; K. A. Flippo; H. Huang; O. A. Hurricane; S. F. Khan; N. Kabadi; C. Kong; L. Kot; B. Lahmann; E. N. Loomis; L. Masse; M. Millot; A. S. Moore; A. Nikroo; T. S. Perry; N. Rice; J. D. Salmonson; R. C. Shah; H. Sio; Michael Stadermann; D. J. Strozzi; Robert Tipton
Beryllium is a candidate ablator material for indirect-drive inertial confinement fusion experiments, motivated by its high mass ablation rate, which is advantageous for implosion coupling efficiency and stabilization of the ablation-front instability growth. We present new data on the shock propagation, in-flight shape, and hot spot self-emission shape from gas-filled capsules that demonstrate the feasibility of predictable, symmetric, controllable beryllium implosions at a case-to-capsule ratio of 3.7. The implosions are round (Legendre mode 2 amplitude ≲5%) at an inner beam power and the energy fraction of 26%–28% of the total, indicating that larger beryllium capsules could be driven symmetrically using the National Ignition Facility.Beryllium is a candidate ablator material for indirect-drive inertial confinement fusion experiments, motivated by its high mass ablation rate, which is advantageous for implosion coupling efficiency and stabilization of the ablation-front instability growth. We present new data on the shock propagation, in-flight shape, and hot spot self-emission shape from gas-filled capsules that demonstrate the feasibility of predictable, symmetric, controllable beryllium implosions at a case-to-capsule ratio of 3.7. The implosions are round (Legendre mode 2 amplitude ≲5%) at an inner beam power and the energy fraction of 26%–28% of the total, indicating that larger beryllium capsules could be driven symmetrically using the National Ignition Facility.
Physics of Plasmas | 2017
D. Martinez; V. A. Smalyuk; Igor V. Igumenshchev; B. Delorme; A. Casner; L. Masse; H.-S. Park; B. A. Remington; M. Olazabal-Loumé
Experiments were performed to investigate the ablative Richtmyer-Meshkov (RM) instability in plastic (CH2) foils. The two-dimensional (2-D) perturbations were created by laser imprinting using a special phase plate with a 2-D single mode, ∼70 μm wavelength sinusoidal intensity pattern on the plastic foil. The growth of imprinted perturbations was measured by face-on, X-ray radiography using Sm and Ta backlighters in 30-μm and 50-μm thick plastic foils, respectively. After the initial imprinting phase, the 2-D perturbations grew due to ablative RM instability before the onset of foil acceleration when they were further amplified by Rayleigh-Taylor instability. Experimental results agree reasonably well with 2-D hydrodynamic simulations and analytic models showing that the modulation growth in areal density is due to ablative RM instability.