Kenneth Bradford Wharton
Lawrence Livermore National Laboratory
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Featured researches published by Kenneth Bradford Wharton.
Physics of Plasmas | 1998
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 | 2002
J. Zweiback; Thomas E. Cowan; J. H. Hartley; R. H. Howell; Kenneth Bradford Wharton; John K. Crane; V. Yanovsky; G. Hays; R. A. Smith; T. Ditmire
Recent experiments on the interaction of intense, ultrafast pulses with large van der Waals bonded clusters have shown that these clusters can explode with sufficient kinetic energy to drive nuclear fusion. Irradiating deuterium clusters with a 35 fs laser pulse, it is found that the fusion neutron yield is strongly dependent on such factors as cluster size, laser focal geometry, and deuterium gas jet parameters. Neutron yield is shown to be limited by laser propagation effects as the pulse traverses the gas plume. From the experiments it is possible to get a detailed understanding of how the laser deposits its energy and heats the deuterium cluster plasma. The experiments are compared with simulations.
Review of Scientific Instruments | 2001
Kazuhito Yasuike; M.H. Key; S. P. Hatchett; Richard Adolph Snavely; Kenneth Bradford Wharton
Characterization of hot electron production from an ultraintense laser–solid target plasma interaction by using a buried molybdenum K-shell fluor layer technique has been reported. Laser energy was typically 400 J and its intensity was from 2×1018 up to 3×1020 W cm−2 at 20 TW to 1 PW laser power by changing pulse duration from 20 ps down to 0.5 ps. X-ray background noise level was significantly greater, i.e., gamma flash, in the shorter pulse experiments. Data analysis procedures for the experiments were developed. The conversion efficiency from the laser energy into the energy, carried by hot electrons, has been estimated to be ∼50% at 3×1020 W cm−2 laser intensity, higher than ∼18% at 1019 W cm−2 and ∼12% at 2×1018 W cm−2 intensity.
Physics of Plasmas | 2000
T. Ditmire; J. Zweiback; V. Yanovsky; Thomas E. Cowan; G. Hays; Kenneth Bradford Wharton
Recent experiments on the interaction of intense, ultrafast pulses with large van der Waals bonded clusters have shown that these clusters can explode with substantial kinetic energy. Producing explosions in deuterium clusters with a 35 fs laser pulse, deuterium ions were accelerated to sufficient kinetic energy to drive deuterium–deuterium (DD) nuclear fusion. By diagnosing the fusion yield through measurements of 2.45 MeV fusion neutrons, over 104 neutrons per laser shot were measured when 100 mJ of laser energy is used.
Optics Letters | 1997
Brent C. Stuart; M. D. Perry; John L. Miller; G. Tietbohl; S. Herman; J.A. Britten; C. Brown; Deanna M. Pennington; V. Yanovsky; Kenneth Bradford Wharton
We have demonstrated a Ti:sapphire/Nd:glass laser system that produces up to 51 J of energy in 395-fs pulses (125TW). Focusing at f/3 to a 2.5-times diffraction-limited spot results in a peak irradiance greater than 10(20) W/cm(2) . Our 40-cm-diameter gold diffraction gratings have a damage threshold of 0.42 J/cm(2) for 320-fs pulses.
Physics of Plasmas | 1998
Bruce I. Cohen; Barbara F. Lasinski; A. B. Langdon; E. A. Williams; Kenneth Bradford Wharton; R. K. Kirkwood; K. G. Estabrook
Particle simulations and solutions of coupled mode equations are used to analyze the energy transfer between two equal-frequency, opposed laser beams resonantly interacting with ion acoustic waves in a plasma drifting at the sound speed. The simulations and analysis illustrate the dependence of the energy transfer and the ion wave dynamics on laser intensities and detuning, and the time dependence of the phenomena. The simulation results are in qualitative agreement with experimental observations in the NOVA laser facility [E. M. Campbell et al., Rev. Sci. Instrum. 57, 2101 (1986)] at the Lawrence Livermore National Laboratory. This work is part of a continuing examination of possible resonant crossed-beam interactions in flowing plasmas and their potential effects on the fusion performance of current and future laser-fusion experiments with multiple crossing beams, e.g., proposed experiments in the National Ignition Facility [National Tech. Info. Service Document Nos. DE95017671-DE95017673 and DE95017676...
1999 Symposium on Cost-Effective Steps to Fusion Power, Washington, DC (US), 03/25/2000 | 2000
M.H. Key; E. M. Campbell; Thomas E. Cowan; S. P. Hatchett; E. A. Henry; J. A. Koch; A. B. Langdon; Barbara F. Lasinski; A. J. Mackinnon; A. A. Offenberger; Deanna M. Pennington; M. D. Perry; T. J. Phillips; Thomas C. Sangster; Singh; Richard Adolph Snavely; Stoyer; M. Tsukamoto; Kenneth Bradford Wharton; S. C. Wilks
A model of energy gain induced by fast ignition of thermonuclear burn in compressed deuterium-tritium fuel, is used to show the potential for 300× gain with a driver energy of 1 MJ, if the National Ignition Facility (NIF) were to be adapted for fast ignition. The physics of fast ignition has been studied using a petawatt laser facility at the Lawrence Livermore National Laboratory. Laser plasma interaction in a preformed plasma on a solid target leads to relativistic self-focusing evidenced by x-ray images. Absorption of the laser radiation transfers energy to an intense source of relativistic electrons. Good conversion efficiency into a wide angular distribution is reported. Heating by the electrons in solid density CD2 produces 0.5 to 1 keV temperature, inferred from the D-D thermo-nuclear neutron yield.
Laser and Particle Beams | 1998
J. A. Koch; C. A. Back; C. Brown; K. G. Estabrook; B. A. Hammel; S. P. Hatchett; M.H. Key; J. D. Kilkenny; O. L. Landen; R.W. Lee; J. D. Moody; A. A. Offenberger; Deanna M. Pennington; M. D. Perry; Max Tabak; V. Yanovsky; R. J. Wallace; Kenneth Bradford Wharton; S. C. Wilks
The fast ignitor concept for inertial confinement fusion relies on the generation of hot electrons, produced by a short-pulse ultrahigh intensity laser, which propagate through high-density plasma to deposit their energy in the compressed fuel core and heat it to ignition. In preliminary experiments designed to investigate deep heating of high-density matter, we used a 20 joule, 0.5-30 ps laser to heat solid targets, and used emission spectroscopy to measure plasma temperatures and densities achieved at large depths (2-20 microns) away from the initial target surface. The targets consisted of an Al tracer layer buried within a massive CH slab; H-like and He-like line emission was then used to diagnose plasma conditions. We observe spectra from tracer layers buried up to 20 microns deep, measure emission durations of up to 200 ps, measure plasma temperatures up to T e = 650 eV, and measure electron densities above 10 23 cm -3 . Analysis is in progress, but the data are in reasonable agreement with heating simulations when space-charge induced inhibition is included in hot-electron transport, and this supports the conclusion that the deep heating is initiated by hot electrons.
MULTIPHOTON PROCESSES: ICOMP VIII: 8th International Conference | 2001
J. Zweiback; R. A. Smith; V. P. Yanovsky; Thomas E. Cowan; G. Hays; Kenneth Bradford Wharton; T. Ditmire
Recent experiments on the interaction of intense, ultrafast pulses with large van der Waals bonded clusters have shown that these clusters can explode with substantial kinetic energy. Producing Coulomb explosions in deuterium clusters with a 35 fs laser pulse, we have accelerated ions to sufficient kinetic energy to drive DD nuclear fusion. By diagnosing the fusion yield through measurements of 2.45 MeV fusion neutrons, we have measured the production of over 104 neutrons per laser shot when 100 mJ of laser energy is used.
Physical Review E | 2001
Kenneth Bradford Wharton; C. D. Boley; Aleksey M. Komashko; Alexander M. Rubenchik; J. Zweiback; John K. Crane; G. Hays; Thomas E. Cowan; T. Ditmire