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Dive into the research topics where Max Tabak is active.

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Featured researches published by Max Tabak.


Physics of Plasmas | 1994

Ignition and high gain with ultrapowerful lasers

Max Tabak; James H. Hammer; Michael E. Glinsky; W. L. Kruer; S. C. Wilks; John G. Woodworth; E. Michael Campbell; Michael D. Perry; R. J. Mason

Ultrahigh intensity lasers can potentially be used in conjunction with conventional fusion lasers to ignite inertial confinement fusion (ICF) capsules with a total energy of a few tens of kilojoules of laser light, and can possibly lead to high gain with as little as 100 kJ. A scheme is proposed with three phases. First, a capsule is imploded as in the conventional approach to inertial fusion to assemble a high‐density fuel configuration. Second, a hole is bored through the capsule corona composed of ablated material, as the critical density is pushed close to the high‐density core of the capsule by the ponderomotive force associated with high‐intensity laser light. Finally, the fuel is ignited by suprathermal electrons, produced in the high‐intensity laser–plasma interactions, which then propagate from critical density to this high‐density core. This new scheme also drastically reduces the difficulty of the implosion, and thereby allows lower quality fabrication and less stringent beam quality and symmet...


Physics of Plasmas | 1995

Design and modeling of ignition targets for the National Ignition Facility

S. W. Haan; Stephen M. Pollaine; J. D. Lindl; Laurance J. Suter; R. L. Berger; Linda V. Powers; W. Edward Alley; Peter A. Amendt; John A. H. Futterman; W. Kirk Levedahl; Mordecai D. Rosen; Dana P. Rowley; Richard A. Sacks; Aleksei I. Shestakov; George L. Strobel; Max Tabak; S. V. Weber; George B. Zimmerman; William J. Krauser; Douglas Wilson; Stephen V. Coggeshall; David B. Harris; Nelson M. Hoffman; Bernhard H. Wilde

Several targets are described that in simulations give yields of 1–30 MJ when indirectly driven by 0.9–2 MJ of 0.35 μm laser light. The article describes the targets, the modeling that was used to design them, and the modeling done to set specifications for the laser system in the proposed National Ignition Facility. Capsules with beryllium or polystyrene ablators are enclosed in gold hohlraums. All the designs utilize a cryogenic fuel layer; it is very difficult to achieve ignition at this scale with a noncryogenic capsule. It is necessary to use multiple bands of illumination in the hohlraum to achieve sufficiently uniform x‐ray irradiation, and to use a low‐Z gas fill in the hohlraum to reduce filling of the hohlraum with gold plasma. Critical issues are hohlraum design and optimization, Rayleigh–Taylor instability modeling, and laser–plasma interactions.


Physics of Plasmas | 1998

Hot electron production and heating by hot electrons in fast ignitor research

M.H. Key; M. D. Cable; Thomas E. Cowan; K. G. Estabrook; B. A. Hammel; S. P. Hatchett; E. A. Henry; D. E. Hinkel; J. D. Kilkenny; J. A. Koch; W. L. Kruer; A. B. Langdon; Barbara F. Lasinski; R.W. Lee; B. J. MacGowan; A. J. Mackinnon; J. D. Moody; M. J. Moran; A. A. Offenberger; Deanna M. Pennington; M. D. Perry; T. J. Phillips; Thomas C. Sangster; M. Singh; M. A. Stoyer; Max Tabak; G. L. Tietbohl; M. Tsukamoto; Kenneth Bradford Wharton; S. C. Wilks

In an experimental study of the physics of fast ignition the characteristics of the hot electron source at laser intensities up to 10(to the 20th power) Wcm{sup -2} and the heating produced at depth by hot electrons have been measured. Efficient generation of hot electrons but less than the anticipated heating have been observed.


Physics of Plasmas | 2006

High-energy Kα radiography using high-intensity, short-pulse lasersa)

H.-S. Park; D. M. Chambers; H.-K. Chung; R. J. Clarke; R. Eagleton; E. Giraldez; T. Goldsack; R. Heathcote; N. Izumi; M.H. Key; J. A. King; J. A. Koch; O. L. Landen; A. Nikroo; P. K. Patel; D. Price; B. A. Remington; H. F. Robey; Richard Adolph Snavely; D Steinman; R.B. Stephens; C. Stoeckl; M. Storm; Max Tabak; W. Theobald; R. P. J. Town; J. E. Wickersham; B. Zhang

The characteristics of 22–40keV Kα x-ray sources are measured. These high-energy sources are produced by 100TW and petawatt high-intensity lasers and will be used to develop and implement workable radiography solutions to probe high-Z and dense materials for the high-energy density experiments. The measurements show that the Kα source size from a simple foil target is larger than 60μm, too large for most radiography applications. The total Kα yield is independent of target thicknesses, verifying that refluxing plays a major role in photon generation. Smaller radiating volumes emit brighter Kα radiation. One-dimensional radiography experiments using small-edge-on foils resolved 10μm features with high contrast. Experiments were performed to test a variety of small volume two-dimensional point sources such as cones, wires, and embedded wires, measured photon yields, and compared the measurements with predictions from hybrid-particle-in-cell simulations. In addition to high-energy, high-resolution backlighte...


Physics of Plasmas | 1999

High yield inertial confinement fusion target design for a z-pinch-driven hohlraum

James H. Hammer; Max Tabak; S. C. Wilks; J. D. Lindl; David S. Bailey; Peter W. Rambo; Arthur Toor; George B. Zimmerman; John L. Porter

Calculations are presented for a high yield inertial fusion design, employing indirect drive with a double-ended z-pinch-driven hohlraum radiation source. A high current (∼60 MA) accelerator implodes z pinches within an enclosing hohlraum. Radial spoke arrays and shine shields isolate the capsule from the pinch plasma, magnetic field, and direct x-ray shine. Our approach places minimal requirements on z-pinch uniformity and stability, usually problematic due to magneto-Rayleigh–Taylor instability. Large inhomogeneities of the pinch and spoke array may be present, but the hohlraum adequately smooths the radiation field at the capsule. Simultaneity and reproducibility of the pinch x-ray output to better than 7% are required, however, for good symmetry. Recent experiments suggest a pulse shaping technique, through implosion of a multishell z pinch. X-ray bursts are calculated and observed to occur at each shell collision. A capsule absorbing 1 MJ of x rays at a peak drive temperature of 210 eV is found to ha...


Physics of Plasmas | 2005

Review of progress in Fast Ignition

Max Tabak; Daniel Clark; S. P. Hatchett; M.H. Key; Barbara F. Lasinski; Richard Adolph Snavely; S. C. Wilks; R. P. J. Town; R. Stephens; E. M. Campbell; R. Kodama; Kunioki Mima; K. A. Tanaka; S. Atzeni; R. R. Freeman

Marshall Rosenbluth’s extensive contributions included seminal analysis of the physics of the laser-plasma interaction and review and advocacy of the inertial fusion program. Over the last decade he avidly followed the efforts of many scientists around the world who have studied Fast Ignition, an alternate form of inertial fusion. In this scheme, the fuel is first compressed by a conventional inertial confinement fusion driver and then ignited by a short (∼10ps) pulse, high-power laser. Due to technological advances, such short-pulse lasers can focus power equivalent to that produced by the hydrodynamic stagnation of conventional inertial fusion capsules. This review will discuss the ignition requirements and gain curves starting from simple models and then describe how these are modified, as more detailed physics understanding is included. The critical design issues revolve around two questions: How can the compressed fuel be efficiently assembled? And how can power from the driver be delivered efficient...


Nuclear Fusion | 2001

A generalized scaling law for the ignition energy of inertial confinement fusion capsules

Mark Herrmann; Max Tabak; J. D. Lindl

The minimum energy needed to ignite an inertial confinement fusion capsule is of considerable interest in the optimization of an inertial fusion driver. Recent computational work investigating this minimum energy has found that it depends on the capsule implosion history, in particular, on the capsule drive pressure. This dependence is examined using a series of LASNEX simulations to find ignited capsules which have different values of the implosion velocity, fuel adiabat and drive pressure. It is found that the main effect of varying the drive pressure is to alter the stagnation of the capsule, changing its stagnation adiabat, which, in turn, affects the energy required for ignition. To account for this effect a generalized scaling law has been devised for the ignition energy, Eign ∝ αif1.88±0.05v-5.89±0.12P-0.77±0.03. This generalized scaling law agrees with the results of previous work in the appropriate limits.


Physics of Plasmas | 1996

Two‐dimensional radiation‐magnetohydrodynamic simulations of SATURN imploding Z pinches

James H. Hammer; James L. Eddleman; P. T. Springer; Max Tabak; Arthur Toor; K. L. Wong; George B. Zimmerman; Chris Deeney; Russ Humphreys; T. J. Nash; T. W. L. Sanford; Rick B. Spielman; John S. de Groot

Z‐pinch implosions driven by the SATURN device [D. D. Bloomquist et al., Proceedings of the 6th Institute of Electrical and Electronics Engineers (IEEE) Pulsed Power Conference, Arlington, VA, edited by P. J. Turchi and B. H. Bernstein (IEEE, New York, 1987), p. 310] at Sandia National Laboratory are modeled with a two‐dimensional radiation magnetohydrodynamic (MHD) code, showing strong growth of the magneto‐Rayleigh–Taylor (MRT) instability. Modeling of the linear and nonlinear development of MRT modes predicts growth of bubble‐spike structures that increase the time span of stagnation and the resulting x‐ray pulse width. Radiation is important in the pinch dynamics, keeping the sheath relatively cool during the run‐in and releasing most of the stagnation energy. The calculations give x‐ray pulse widths and magnitudes in reasonable agreement with experiments, but predict a radiating region that is too dense and radially localized at stagnation. We also consider peaked initial density profiles with consta...


Physics of Plasmas | 2012

Fast-ignition transport studies: Realistic electron source, integrated particle-in-cell and hydrodynamic modeling, imposed magnetic fields

D. J. Strozzi; Max Tabak; David J. Larson; L. Divol; Andreas Kemp; C. Bellei; M. M. Marinak; M.H. Key

Transport modeling of idealized, cone-guided fast ignition targets indicates the severe challenge posed by fast-electron source divergence. The hybrid particle-in-cell (PIC) code Zuma is run in tandem with the radiation-hydrodynamics code Hydra to model fast-electron propagation, fuel heating, and thermonuclear burn. The fast electron source is based on a 3D explicit-PIC laser-plasma simulation with the PSC code. This shows a quasi two-temperature energy spectrum and a divergent angle spectrum (average velocity-space polar angle of 52°). Transport simulations with the PIC-based divergence do not ignite for >1 MJ of fast-electron energy, for a modest (70 μm) standoff distance from fast-electron injection to the dense fuel. However, artificially collimating the source gives an ignition energy of 132 kJ. To mitigate the divergence, we consider imposed axial magnetic fields. Uniform fields ∼50 MG are sufficient to recover the artificially collimated ignition energy. Experiments at the Omega laser facility hav...


Nuclear Fusion | 1999

Z pinch driven inertial confinement fusion target physics research at Sandia National Laboratories

R. J. Leeper; T.E. Alberts; J.R. Asay; P.M. Baca; K.L. Baker; S.P. Breeze; G.A. Chandler; D.L. Cook; G.W. Cooper; C. Deeney; Mark S. Derzon; M.R. Douglas; D.L. Fehl; T. Gilliland; D.E. Hebron; M.J. Hurst; D.O. Jobe; J.W. Kellogg; J.S. Lash; S.E. Lazier; M.K. Matzen; D.H. McDaniel; J.S. McGurn; T.A. Mehlhorn; A.R. Moats; R.C. Mock; D.J. Muron; T.J. Nash; R. E. Olson; J.L. Porter

Three hohlraum concepts are being pursued at Sandia National Laboratories (SNL) to investigate the possibility of using pulsed power driven magnetic implosions (Z pinches) to drive targets capable of fusion yields in the range 200-1000 MJ. This research is being conducted on SNLs Z facility, which is capable of driving peak currents of 20 MA in various Z pinch load configurations that produce implosion velocities as high as 7.5 × 107cm/s, X ray energies of 1-2 MJ and X ray powers of 100-250 TW. The first concept, denoted dynamic hohlraum, has achieved a temperature of 180 ± 14 eV in a configuration suitable for driving capsules. In addition, this concept has also achieved a temperature of 230 ± 18 eV in an arrangement suitable for driving an external hohlraum. The second concept, denoted static walled hohlraum, has achieved temperatures of ~80-100 eV. Experimental investigation of the third concept, denoted Z pinch driven hohlraum, has recently begun. The article discusses each of these hohlraum concepts and provides an overview of the experiments that have been conducted on these systems to date.

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R. P. J. Town

Lawrence Livermore National Laboratory

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S. C. Wilks

Lawrence Livermore National Laboratory

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M.H. Key

Lawrence Livermore National Laboratory

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P. K. Patel

Lawrence Livermore National Laboratory

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Barbara F. Lasinski

Lawrence Livermore National Laboratory

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Andreas Kemp

Lawrence Livermore National Laboratory

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A. J. Mackinnon

Lawrence Livermore National Laboratory

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S. P. Hatchett

Lawrence Livermore National Laboratory

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D. A. Callahan

Lawrence Livermore National Laboratory

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Peter A. Amendt

Lawrence Livermore National Laboratory

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