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Dive into the research topics where N. B. Meezan is active.

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Featured researches published by N. B. Meezan.


Science | 2010

Symmetric Inertial Confinement Fusion Implosions at Ultra-High Laser Energies

S. H. Glenzer; B. J. MacGowan; P. Michel; N. B. Meezan; L. J. Suter; S. Dixit; J. L. Kline; G. A. Kyrala; D. K. Bradley; D. A. Callahan; E. L. Dewald; L. Divol; E. G. Dzenitis; M. J. Edwards; Alex V. Hamza; C. A. Haynam; D. E. Hinkel; D. H. Kalantar; J. D. Kilkenny; O. L. Landen; J. D. Lindl; S. LePape; J. D. Moody; A. Nikroo; T. Parham; M. B. Schneider; R. P. J. Town; Paul J. Wegner; K. Widmann; Pamela K. Whitman

Ignition Set to Go One aim of the National Ignition Facility is to implode a capsule containing a deuterium-tritium fuel mix and initiate a fusion reaction. With 192 intense laser beams focused into a centimeter-scale cavity, a major challenge has been to create a symmetric implosion and the necessary temperatures within the cavity for ignition to be realized (see the Perspective by Norreys). Glenzer et al. (p. 1228, published online 28 January) now show that these conditions can be met, paving the way for the next step of igniting a fuel-filled capsule. Furthermore, Li et al. (p. 1231, published online 28 January) show how charged particles can be used to characterize and measure the conditions within the imploding capsule. The high energies and temperature realized can also be used to model astrophysical and other extreme energy processes in a laboratory settings. Laser-driven temperatures and implosion symmetry are close to the requirements for inertial-fusion ignition. Indirect-drive hohlraum experiments at the National Ignition Facility have demonstrated symmetric capsule implosions at unprecedented laser drive energies of 0.7 megajoule. One hundred and ninety-two simultaneously fired laser beams heat ignition-emulate hohlraums to radiation temperatures of 3.3 million kelvin, compressing 1.8-millimeter-diameter capsules by the soft x-rays produced by the hohlraum. Self-generated plasma optics gratings on either end of the hohlraum tune the laser power distribution in the hohlraum, which produces a symmetric x-ray drive as inferred from the shape of the capsule self-emission. These experiments indicate that the conditions are suitable for compressing deuterium-tritium–filled capsules, with the goal of achieving burning fusion plasmas and energy gain in the laboratory.


Physics of Plasmas | 2010

Symmetry tuning via controlled crossed-beam energy transfer on the National Ignition Facilitya)

P. Michel; S. H. Glenzer; L. Divol; David K. Bradley; D. A. Callahan; S. Dixit; S. Glenn; D. E. Hinkel; R. K. Kirkwood; J. L. Kline; W. L. Kruer; G. A. Kyrala; S. Le Pape; N. B. Meezan; R. P. J. Town; K. Widmann; E. A. Williams; B. J. MacGowan; J. D. Lindl; L. Suter

The Hohlraum energetics experimental campaign started in the summer of 2009 on the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)]. These experiments showed good coupling of the laser energy into the targets [N. Meezan et al., Phys. Plasmas 17, 056304 (2010)]. They have also demonstrated controlled crossed-beam energy transfer between laser beams as an efficient and robust tool to tune the implosion symmetry of ignition capsules, as predicted by earlier calculations [P. Michel et al., Phys. Rev. Lett. 102, 025004 (2009)]. A new linear model calculating crossed-beam energy transfer between cones of beams on the NIF has been developed. The model has been applied to the subscale Hohlraum targets shot during the National Ignition Campaign in 2009. A good agreement can be found between the calculations and the experiments when the impaired propagation of the laser beams due to backscatter is accounted for.


Physics of Plasmas | 2011

Capsule implosion optimization during the indirect-drive National Ignition Campaign

O. L. Landen; John Edwards; S. W. Haan; H. F. Robey; J. L. Milovich; B. K. Spears; S. V. Weber; D. S. Clark; J. D. Lindl; B. J. MacGowan; E. I. Moses; J. Atherton; Peter A. Amendt; T. R. Boehly; David K. Bradley; David G. Braun; D. A. Callahan; Peter M. Celliers; G. W. Collins; E. L. Dewald; L. Divol; J. A. Frenje; S. H. Glenzer; Alex V. Hamza; B. A. Hammel; D. G. Hicks; Nelson M. Hoffman; N. Izumi; O. S. Jones; J. D. Kilkenny

Capsule performance optimization campaigns will be conducted at the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Nucl. Fusion 44, 228 (2004)] to substantially increase the probability of ignition. The campaigns will experimentally correct for residual uncertainties in the implosion and hohlraum physics used in our radiation-hydrodynamic computational models using a variety of ignition capsule surrogates before proceeding to cryogenic-layered implosions and ignition experiments. The quantitative goals and technique options and down selections for the tuning campaigns are first explained. The computationally derived sensitivities to key laser and target parameters are compared to simple analytic models to gain further insight into the physics of the tuning techniques. The results of the validation of the tuning techniques at the OMEGA facility [J. M. Soures et al., Phys. Plasmas 3, 2108 (1996)] under scaled hohlraum and capsule conditions relevant to the ignition design are shown ...


Physics of Plasmas | 2010

National Ignition Campaign Hohlraum energetics

N. B. Meezan; L. J. Atherton; D. A. Callahan; E. L. Dewald; S. Dixit; E. G. Dzenitis; M. J. Edwards; C. A. Haynam; D. E. Hinkel; O. S. Jones; O. L. Landen; Richard A. London; P. Michel; J. D. Moody; J. L. Milovich; M. B. Schneider; C. A. Thomas; R. P. J. Town; A. Warrick; S. V. Weber; K. Widmann; S. H. Glenzer; L. J. Suter; B. J. MacGowan; J. L. Kline; George A. Kyrala; A. Nikroo

The first series of experiments of the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)] tested ignition Hohlraum “energetics,” a term described by four broad goals: (1) measurement of laser absorption by the Hohlraum; (2) measurement of the x-ray radiation flux (TRAD4) on the surrogate ignition capsule; (3) quantitative understanding of the laser absorption and resultant x-ray flux; and (4) determining whether initial Hohlraum performance is consistent with requirements for ignition. This paper summarizes the status of NIF Hohlraum energetics experiments. The Hohlraum targets and experimental design are described, as well as the results of the initial experiments. The data demonstrate low backscattered energy (<10%) for Hohlraums filled with helium gas. A discussion of our current understanding of NIF Hohlraum x-ray drive follows, including an overview of the computational tools, i.e., radiation-hydrodynamics codes that have been used to design the Hohlraums. The perf...


Physics of Plasmas | 2011

Symmetry tuning for ignition capsules via the symcap techniquea)

G. A. Kyrala; J. L. Kline; S. Dixit; S. H. Glenzer; D. H. Kalantar; D. K. Bradley; N. Izumi; N. B. Meezan; O. L. Landen; D. A. Callahan; S. V. Weber; J. P. Holder; S. Glenn; M. J. Edwards; J. A. Koch; L. J. Suter; S. W. Haan; R. P. J. Town; P. Michel; O. S. Jones; S. H. Langer; J. D. Moody; E. L. Dewald; T. Ma; J. E. Ralph; Alex V. Hamza; E. G. Dzenitis; J. D. Kilkenny

Symmetry of an implosion is crucial to get ignition successfully. Several methods of control and measurement of symmetry have been applied on many laser systems with mm size hohlraums and ns pulses. On the National Ignition Facility [Moses et al., Phys. Plasmas 16, 041006 (2009)] we have large hohlraums of cm scale, long drive pulses of 10 s of ns, and a large number of beams with the option to tune their wavelengths. Here we discuss how we used the x-ray self-emission from imploding surrogates to ignition capsules (symcaps) to measure the symmetry of the implosion. We show that symcaps are good surrogates for low order symmetry, though having lower sensitivity to distortions than ignition capsules. We demonstrate the ability to transfer energy between laser beams in a gas-filled hohlraum using wavelength tuning, successfully tuning the lowest order symmetry of the symcaps in different size hohlraums at different laser energies within the specification established by calculations for successful ignition.


Physics of Plasmas | 2012

Implosion dynamics measurements at the National Ignition Facility

Damien G. Hicks; N. B. Meezan; E. L. Dewald; A. J. Mackinnon; R.E. Olson; D. A. Callahan; T. Döppner; L. R. Benedetti; D. K. Bradley; Peter M. Celliers; D. S. Clark; P. Di Nicola; S. N. Dixit; E. G. Dzenitis; J. E. Eggert; D. R. Farley; J. A. Frenje; S. Glenn; S. H. Glenzer; Alex V. Hamza; R. F. Heeter; J. P. Holder; N. Izumi; D. H. Kalantar; S. F. Khan; J. L. Kline; J. J. Kroll; G. A. Kyrala; T. Ma; A. G. MacPhee

Measurements have been made of the in-flight dynamics of imploding capsules indirectly driven by laser energies of 1–1.7 MJ at the National Ignition Facility [Miller et al., Nucl. Fusion 44, 228 (2004)]. These experiments were part of the National Ignition Campaign [Landen et al., Phys. Plasmas 18, 051002 (2011)] to iteratively optimize the inputs required to achieve thermonuclear ignition in the laboratory. Using gated or streaked hard x-ray radiography, a suite of ablator performance parameters, including the time-resolved radius, velocity, mass, and thickness, have been determined throughout the acceleration history of surrogate gas-filled implosions. These measurements have been used to establish a dynamically consistent model of the ablative drive history and shell compressibility throughout the implosion trajectory. First results showed that the peak velocity of the original 1.3-MJ Ge-doped polymer (CH) point design using Au hohlraums reached only 75% of the required ignition velocity. Several capsu...


Physics of Plasmas | 2012

A high-resolution integrated model of the National Ignition Campaign cryogenic layered experiments

O. S. Jones; C. Cerjan; M. M. Marinak; J. L. Milovich; H. F. Robey; P. T. Springer; L. R. Benedetti; D. L. Bleuel; E. Bond; D. K. Bradley; D. A. Callahan; J. A. Caggiano; Peter M. Celliers; D. S. Clark; S. M. Dixit; T. Döppner; Rebecca Dylla-Spears; E. G. Dzentitis; D. R. Farley; S. Glenn; S. H. Glenzer; S. W. Haan; B. J. Haid; C. A. Haynam; Damien G. Hicks; B. J. Kozioziemski; K. N. LaFortune; O. L. Landen; E. R. Mapoles; A. J. Mackinnon

A detailed simulation-based model of the June 2011 National Ignition Campaign cryogenic DT experiments is presented. The model is based on integrated hohlraum-capsule simulations that utilize the best available models for the hohlraum wall, ablator, and DT equations of state and opacities. The calculated radiation drive was adjusted by changing the input laser power to match the experimentally measured shock speeds, shock merger times, peak implosion velocity, and bangtime. The crossbeam energy transfer model was tuned to match the measured time-dependent symmetry. Mid-mode mix was included by directly modeling the ablator and ice surface perturbations up to mode 60. Simulated experimental values were extracted from the simulation and compared against the experiment. Although by design the model is able to reproduce the 1D in-flight implosion parameters and low-mode asymmetries, it is not able to accurately predict the measured and inferred stagnation properties and levels of mix. In particular, the measu...


Review of Scientific Instruments | 2010

Measuring symmetry of implosions in cryogenic Hohlraums at the NIF using gated x-ray detectors (invited)

George A. Kyrala; S. Dixit; S. H. Glenzer; D. H. Kalantar; David K. Bradley; N. Izumi; N. B. Meezan; O. L. Landen; D. A. Callahan; S. V. Weber; J. P. Holder; S. Glenn; M. J. Edwards; P. M. Bell; J. R. Kimbrough; J. A. Koch; R. Prasad; L. J. Suter; J. L. Kline; J. D. Kilkenny

Ignition of imploding inertial confinement capsules requires, among other things, controlling the symmetry with high accuracy and fidelity. We have used gated x-ray imaging, with 10 μm and 70 ps resolution, to detect the x-ray emission from the imploded core of symmetry capsules at the National Ignition Facility. The measurements are used to characterize the time dependent symmetry and the x-ray bang time of the implosion from two orthogonal directions. These measurements were one of the primary diagnostics used to tune the parameters of the laser and Hohlraum to vary the symmetry and x-ray bang time of the implosion of cryogenically cooled ignition scale deuterium/helium filled plastic capsules. Here, we will report on the successful measurements performed with up to 1.2 MJ of laser energy in a fully integrated cryogenics gas-filled ignition-scale Hohlraum and capsule illuminated with 192 smoothed laser beams. We will describe the technique, the accuracy of the technique, and the results of the variation in symmetry with tuning parameters, and explain how that set was used to predictably tune the implosion symmetry as the laser energy, the laser cone wavelength separation, and the Hohlraum size were increased to ignition scales. We will also describe how to apply that technique to cryogenically layered tritium-hydrogen-deuterium capsules.


Physics of Plasmas | 2011

Analysis of the National Ignition Facility Ignition Hohlraum Energetics Experiments

R. P. J. Town; M. D. Rosen; P. Michel; L. Divol; J. D. Moody; G. A. Kyrala; M. B. Schneider; J. L. Kline; C. A. Thomas; J. L. Milovich; D. A. Callahan; N. B. Meezan; D. E. Hinkel; E. A. Williams; R. L. Berger; M. J. Edwards; L. J. Suter; S. W. Haan; J. D. Lindl; E. L. Dewald; S. Dixit; S. H. Glenzer; O. L. Landen; E. I. Moses; Howard A. Scott; J. A. Harte; George B. Zimmerman

A series of 40 experiments on the National Ignition Facility (NIF) [E. I. Moses et al., Phys. Plasmas 16, 041006 (2009)] to study energy balance and implosion symmetry in reduced- and full-scale ignition hohlraums was shot at energies up to 1.3 MJ. This paper reports the findings of the analysis of the ensemble of experimental data obtained that has produced an improved model for simulating ignition hohlraums. Last year the first observation in a NIF hohlraum of energy transfer between cones of beams as a function of wavelength shift between those cones was reported [P. Michel et al., Phys. Plasmas 17, 056305 (2010)]. Detailed analysis of hohlraum wall emission as measured through the laser entrance hole (LEH) has allowed the amount of energy transferred versus wavelength shift to be quantified. The change in outer beam brightness is found to be quantitatively consistent with LASNEX [G. B. Zimmerman and W. L. Kruer, Comments Plasma Phys. Controlled Fusion 2, 51 (1975)] simulations using the predicted ener...


Physics of Plasmas | 2012

Hot-spot mix in ignition-scale implosions on the NIF

S. P. Regan; R. Epstein; B. A. Hammel; L. J. Suter; J. E. Ralph; Howard A. Scott; M. A. Barrios; D. K. Bradley; D. A. Callahan; C. Cerjan; G. W. Collins; S. Dixit; T. Doeppner; M. J. Edwards; D. R. Farley; S. Glenn; S. H. Glenzer; I. E. Golovkin; S. W. Haan; Alex V. Hamza; Damien G. Hicks; N. Izumi; J. D. Kilkenny; J. L. Kline; G. A. Kyrala; O. L. Landen; T. Ma; J. J. MacFarlane; R. C. Mancini; R. L. McCrory

Ignition of an inertial confinement fusion (ICF) target depends on the formation of a central hot spot with sufficient temperature and areal density. Radiative and conductive losses from the hot spot can be enhanced by hydrodynamic instabilities. The concentric spherical layers of current National Ignition Facility (NIF) ignition targets consist of a plastic ablator surrounding a thin shell of cryogenic thermonuclear fuel (i.e., hydrogen isotopes), with fuel vapor filling the interior volume [S. W. Haan et al., Phys. Plasmas 18, 051001 (2011)]. The Rev. 5 ablator is doped with Ge to minimize preheat of the ablator closest to the DT ice caused by Au M-band emission from the hohlraum x-ray drive [D. S. Clark et al., Phys. Plasmas 17, 052703 (2010)]. Richtmyer–Meshkov and Rayleigh–Taylor hydrodynamic instabilities seeded by high-mode (50<l<200) ablator-surface perturbations can cause Ge-doped ablator to mix into the interior of the shell at the end of the acceleration phase [B. A. Hammel et al., Phys. Plasma...

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L. Divol

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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O. L. Landen

Lawrence Livermore National Laboratory

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S. H. Glenzer

SLAC National Accelerator Laboratory

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L. J. Suter

Lawrence Livermore National Laboratory

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O. S. Jones

Lawrence Livermore National Laboratory

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A. J. Mackinnon

Lawrence Livermore National Laboratory

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E. L. Dewald

Lawrence Livermore National Laboratory

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J. L. Kline

Los Alamos National Laboratory

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D. E. Hinkel

Lawrence Livermore National Laboratory

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