Ian Craig Smith
Lawrence Livermore National Laboratory
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Featured researches published by Ian Craig Smith.
Applied Optics | 1997
Bruno M. Van Wonterghem; J. R. Murray; John H. Campbell; D. Ralph Speck; Charles E. Barker; Ian Craig Smith; Donald F. Browning; William C. Behrendt
The Beamlet is a single-beam prototype of future multibeam megajoule-class Nd:glass laser drivers for inertial confinement fusion. It uses a multipass main amplifier, adaptive optics, and efficient, high-fluence frequency conversion to the third harmonic. The Beamlet amplifier contains Brewster-angle glass slabs with a clear aperture of 39 cm x 39 cm and a full-aperture plasma-electrode Pockels cell switch. It has been successfully tested over a range of pulse lengths from 1-10 ns up to energies at 1.053 mum of 5.8 kJ at 1 ns and 17.3 kJ at 10 ns. A 39-actuator deformable mirror corrects the beam quality to a Strehl ratio of as much as 0.4. The 1.053-mum output has been converted to the third harmonic at efficiencies as high as 80% and fluences as high as 8.7 J/cm(2) for 3-ns pulses.
Physics of Plasmas | 2012
Kyle Peterson; Daniel Brian Sinars; Edmund P. Yu; Mark Herrmann; Michael Edward Cuneo; Stephen A. Slutz; Ian Craig Smith; Briggs W. Atherton; M. D. Knudson; Charles Nakhleh
This paper explores the role of electro-thermal instabilities on the dynamics of magnetically accelerated implosion systems. Electro-thermal instabilities result from non-uniform heating due to temperature dependence in the conductivity of a material. Comparatively little is known about these types of instabilities compared to the well known Magneto-Rayleigh-Taylor (MRT) instability. We present simulations that show electrothermal instabilities form immediately after the surface material of a conductor melts and can act as a significant seed to subsequent MRT instability growth. We also present the results of several experiments performed on Sandia National Laboratories Z accelerator to investigate signatures of electrothermal instability growth on well characterized initially solid aluminum and copper rods driven with a 20 MA, 100 ns risetime current pulse. These experiments show excellent agreement with electrothermal instability simulations and exhibit larger instability growth than can be explained by MRT theory alone.
Physics of Plasmas | 2015
P. F. Knapp; Paul Schmit; Stephanie B. Hansen; M. R. Gomez; Kelly Hahn; Daniel Brian Sinars; Kyle Peterson; Stephen A. Slutz; Adam B Sefkow; Thomas James Awe; Eric Harding; Christopher A. Jennings; Michael P. Desjarlais; Gordon Andrew Chandler; G. W. Cooper; Michael Edward Cuneo; Matthias Geissel; A. J. Harvey-Thompson; John L. Porter; Gregory A. Rochau; Dean C. Rovang; C. L. Ruiz; M. E. Savage; Ian Craig Smith; W. A. Stygar; Mark Herrmann
By magnetizing the fusion fuel in inertial confinement fusion (ICF) systems, the required stagnation pressure and density can be relaxed dramatically. This happens because the magnetic field insulates the hot fuel from the cold pusher and traps the charged fusion burn products. This trapping allows the burn products to deposit their energy in the fuel, facilitating plasma self-heating. Here, we report on a comprehensive theory of this trapping in a cylindrical DD plasma magnetized with a purely axial magnetic field. Using this theory, we are able to show that the secondary fusion reactions can be used to infer the magnetic field-radius product, BR, during fusion burn. This parameter, not ρR, is the primary confinement parameter in magnetized ICF. Using this method, we analyze data from recent Magnetized Liner Inertial Fusion experiments conducted on the Z machine at Sandia National Laboratories. We show that in these experiments BR ≈ 0.34(+0.14/−0.06) MG · cm, a ∼ 14× increase in BR from the initial value, and confirming that the DD-fusion tritons are magnetized at stagnation. This is the first experimental verification of charged burn product magnetization facilitated by compression of an initial seed magnetic flux.
conference on lasers and electro optics | 2002
Patrick K. Rambo; John L. Porter; Guy R. Bennett; Ian Craig Smith; Alvin C. Erlandson; James E. Murray; John A. Caird
Summary from only given. The Z-machine is a Z-pinch device, using pulsed power methods to implode wire arrays and create high density plasmas and consequent x-ray emission. Small cavities (holhraums) are used to symmetrically bathe capsules in this radiation, causing the capsules compress for ICF studies. Radiography performed during an accelerator shot shows implosion symmetry and a factor of 2 compression at 14 ns after peak accelerator radiation The new radiography ability provided by a Z-beamlet laser allows this implosion symmetry to be studied and improved.
conference on lasers and electro optics | 1995
J.H. Campbell; C.E. Barker; B.M. VanWonterghem; David Ralph Speck; William C. Behrendt; J. R. Murray; John A. Caird; D.E. Decker; Ian Craig Smith
The Beamlet laser is a large aperture, flashlamp pumped Nd: glass laser that is a scientific prototype of an advanced Inertial Fusion laser. Beamlet has achieved third harmonic, conversion efficiency of near 80% with its nominal 35cm {times} 35cm square beam at mean 3{omega} fluences in excess of 8 J/cm{sup 2}(3-ns). Beamlet uses an adaptive optics system to correct for aberrations and achieve less than 2 {times} diffraction limited far field spot size.
Archive | 2014
Patrick K. Rambo; Darrell Jewell Armstrong; Jens Schwarz; Ian Craig Smith; Jonathon Shores; Christopher Speas; John L. Porter
The Z-Beamlet laser has been operating at Sandia National Laboratories since 2001 to provide a source of laser-generated x-rays for radiography of events on the Z-Accelerator. Changes in desired operational scope have necessitated the increase in pulse duration and energy available from the laser system. This is enabled via the addition of a phase modulated seed laser as an alternative front-end. The practical aspects of deployment are discussed here.
Optical Interference Coatings (2010), paper FA8 | 2010
John Curtis Bellum; Damon E. Kletecka; Patrick K. Rambo; Ian Craig Smith; Jens Schwarz; Briggs Atherton
We report reflectivity, design and laser damage comparisons of our AR coatings for use at 1054 nm and/or 527 nm, and at angles of incidence between 0 and 45 degrees.
Archive | 2005
Carol S. Ashley; Patrick K. Rambo; Jens Schwarz; Darren R. Dunphy; Eric D. Branson; Ian Craig Smith; William Arthur Johnson; Scott T. Reed; Adam W. Cook
In order to develop the next generation of high peak intensity lasers, new grating technology providing higher damage thresholds and large apertures is required. The current assumption is that this technical innovation will be multilayer dielectric gratings, wherein the uppermost layer of a thin film mirror is etched to create the desired binary phase grating. A variant of this is explored with the upper grating layer being a lower density gelatin-based volume phase grating in either sol-gel or dichromated gelatin. One key benefit is the elimination of the etching step.
Frontiers in Optics | 2004
Jens Schwarz; Patrick K. Rambo; Ian Craig Smith; John L. Porter
The authors have used two Pockels cells in series to achieve simple temporal pulse shaping. This technique has been used in the optical parametric chirp pulse amplification (OPCPA) system to optimize the temporal shape of the pump pulse, providing a low cost alternative to arbitrary waveform generators.
Frontiers in Optics | 2003
Aaron Edens; T. Ditmire; Dustin Froula; Gianluca Gregori; J. F. Hansen; D. Price; John P. Edwards; Richard G. Adams; Robin Scott Broyles; Patrick K. Rambo; Larry Ruggles; Gennady Sergeevich Sarkisov; Ian Craig Smith; Benjamin D. Thurston; John L. Porter
We report experiments on high power laser driven radiative blast waves. By focusing 100J – 1 kJ laser pulses onto pin targets immersed in gases we attempted to produce the pressure-driven thin shell overstability thought to play a major role in supernova remnant hydrodynamics.