C. Clay Widmayer
Lawrence Livermore National Laboratory
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Featured researches published by C. Clay Widmayer.
Applied Optics | 2007
C. A. Haynam; Paul J. Wegner; Jerome M. Auerbach; M. W. Bowers; S. Dixit; G. V. Erbert; G. M. Heestand; Mark A. Henesian; Mark Hermann; Kenneth S. Jancaitis; Kenneth R. Manes; Christopher D. Marshall; N. C. Mehta; Joseph A. Menapace; E. I. Moses; J. R. Murray; M. Nostrand; Charles D. Orth; R. Patterson; Richard A. Sacks; M. J. Shaw; M. Spaeth; S. Sutton; Wade H. Williams; C. Clay Widmayer; R. K. White; Steven T. Yang; B. Van Wonterghem
The National Ignition Facility (NIF) is the worlds largest laser system. It contains a 192 beam neodymium glass laser that is designed to deliver 1.8 MJ at 500 TW at 351 nm in order to achieve energy gain (ignition) in a deuterium-tritium nuclear fusion target. To meet this goal, laser design criteria include the ability to generate pulses of up to 1.8 MJ total energy, with peak power of 500 TW and temporal pulse shapes spanning 2 orders of magnitude at the third harmonic (351 nm or 3omega) of the laser wavelength. The focal-spot fluence distribution of these pulses is carefully controlled, through a combination of special optics in the 1omega (1053 nm) portion of the laser (continuous phase plates), smoothing by spectral dispersion, and the overlapping of multiple beams with orthogonal polarization (polarization smoothing). We report performance qualification tests of the first eight beams of the NIF laser. Measurements are reported at both 1omega and 3omega, both with and without focal-spot conditioning. When scaled to full 192 beam operation, these results demonstrate, to the best of our knowledge for the first time, that the NIF will meet its laser performance design criteria, and that the NIF can simultaneously meet the temporal pulse shaping, focal-spot conditioning, and peak power requirements for two candidate indirect drive ignition designs.
Applied Optics | 1997
C. Clay Widmayer; David Milam; Simon P. deSzoeke
Computer models are used to simulate the nonlinear formation of images of obscurations in laser beams. The predictions of the model are found to be in good agreement with measurements conducted in the nonlinear regime corresponding to a typical solid-state laser operation. In this regime, peak-to-mean fluence ratios large enough to induce damage in optical components are observed. The amplitude of the images and their location along the propagation axis are accurately predicted by the simulations. This indicates that the model is a reliable design tool for specifying component staging and optical specifications to avoid optical damage by this mechanism.
Applied Optics | 1998
C. Clay Widmayer; Melinda R. Nickels; David Milam
Experimental measurements and computer simulations of nonlinear holographic imaging of phase errors in laser beams are presented. The computer models are found to accurately predict the results of the experiments. Comparison with similar results by use of amplitude scatterers reveals that the image location (along the propagation path) is the same for phase and amplitude scatterers. However, the intensity and fluence of the image of a phase scatterer are significantly larger, indicating that phase objects pose a larger damage threat to optical components.
Journal of Physics: Conference Series | 2008
C. A. Haynam; Richard A. Sacks; Paul J. Wegner; M. W. Bowers; S. Dixit; G. Erbert; G. M. Heestand; Mark A. Henesian; Mark Hermann; Kenneth S. Jancaitis; Kenneth R. Manes; Christopher D. Marshall; N. C. Mehta; Joseph A. Menapace; Mike C. Nostrand; Charles D. Orth; M. J. Shaw; S. Sutton; Wade H. Williams; C. Clay Widmayer; R. K. White; Steven T. Yang; B. Van Wonterghem
The National Ignition Facility (NIF) at Lawrence Livermore National Laboratory contains a 192-beam 3.6 MJ neodymium glass laser that is frequency converted to 351nm light. It has been designed to support high energy density science (HEDS), including the demonstration of fusion ignition through Inertial Confinement. To meet this goal, laser design criteria include the ability to generate pulses of up to 1.8-MJ total energy at 351nm, with peak power of 500 TW and precisely-controlled temporal pulse shapes spanning two orders of magnitude. The focal spot fluence distribution of these pulses is conditioned, through a combination of special optics in the 1ω (1053 nm) portion of the laser (continuous phase plates), smoothing by spectral dispersion (SSD), and the overlapping of multiple beams with orthogonal polarization (polarization smoothing). In 2006 and 2007, a series of measurements were performed on the NIF laser, at both 1ω and 3ω (351 nm). When scaled to full 192-beam operation, these results lend confidence to the claim that NIF will meet its laser performance design criteria and that it will be able to simultaneously deliver the temporal pulse shaping, focal spot conditioning, peak power, shot-to-shot reproducibility, and power balance requirements of indirect-drive fusion ignition campaigns. We discuss the plans and status of NIFs commissioning, and the nature and results of these measurement campaigns.
Applied Optics | 2008
Seung-Whan Bahk; Jonathan D. Zuegel; James R. Fienup; C. Clay Widmayer; John E. Heebner
A spot-shadowing technique to mitigate damage growth in a high-energy laser is studied. Its goal is to minimize the energy loss and undesirable hot spots in intermediate planes of the laser. A nonlinear optimization algorithm solves for the complex fields required to mitigate damage growth in the National Ignition Facility amplifier chain. The method is generally applicable to any large fusion laser.
Boulder Damage Symposium XXXVII: Annual Symposium on Optical Materials for High Power Lasers | 2005
Mike Runkel; Ruth A. Hawley-Fedder; C. Clay Widmayer; Wade H. Williams; Carolyn L. Weinzapfel; Dave Roberts
A multi-wavelength laser based system has been constructed to measure defect induced beam modulation (diffraction) from ICF class laser optics. The Nd:YLF-based modulation measurement system (MMS) uses simple beam collimation and imaging to capture diffraction patterns from optical defects onto an 8-bit digital camera at 1053, 527 and 351 nm. The imaging system has a field of view of 4.5 x 2.8 mm2 and is capable of imaging any plane from 0 to 30 cm downstream from the defect. The system is calibrated using a 477 micron chromium dot on glass for which the downstream diffraction patterns were calculated numerically. Under nominal conditions the system can measure maximum peak modulations of approximately 7:1. An image division algorithm is used to calculate the peak modulation from the diffracted and empty field images after the baseline residual light background is subtracted from both. The peak modulation can then be plotted versus downstream position. The system includes a stage capable of holding optics up to 50 pounds with x and y translation of 40 cm and has been used to measure beam modulation due to solgel coating defects, surface digs on KDP crystals, lenslets in bulk fused silica and laser damage sites mitigated with CO2 lasers.
Optical Science and Technology, SPIE's 48th Annual Meeting | 2004
M. J. Shaw; Wade H. Williams; Kenneth S. Jancaitis; C. Clay Widmayer; Ronald K. House
The National Ignition Facility (NIF), currently under construction at the University of California s Lawrence Livermore National Laboratory (LLNL) is a stadium-sized facility containing a 192-beam, 1.8 Megajoule, 500-Terrawatt, 351-nm laser system together with a 10-meter diameter target chamber with room for nearly 100 experimental diagnostics. NIF is being built by the National Nuclear Security Administration and when completed will be the world s largest laser experimental system, providing a national center to study inertial confinement fusion and the physics of matter at extreme energy densities and pressures. NIF s 192 energetic laser beams will compress fusion targets to conditions where they will ignite and burn, liberating more energy than required to initiate the fusion reaction. The first four beamlines (a quad) are currently being commissioned, with increasingly energetic laser pulses being propagated throughout the laser system. Success on many of the NIF laser s missions depends on obtaining precisely specified energy waveforms from each of the 192 beams over a wide variety of pulse lengths and temporal shapes. A computational system, the Laser Performance Operations Model (LPOM) has been developed and deployed during NIF commissioning to automate the laser setup process, and accurately predict laser energtics. For each shot on NIF, the LPOM determines the characteristics of the injection laser system required to achieve the desired main laser output, provides parameter checking for equipment protection, determines the required diagnostic setup, and supplies post-shot data analysis and reporting.
Applied Optics | 2008
G. M. Heestand; C. A. Haynam; Paul J. Wegner; M. W. Bowers; S. Dixit; G. V. Erbert; Mark A. Henesian; Mark Hermann; Kenneth S. Jancaitis; K. Knittel; Thomas R. Kohut; J. D. Lindl; Kenneth R. Manes; Christopher D. Marshall; N. C. Mehta; Joseph A. Menapace; E. I. Moses; J. R. Murray; M. Nostrand; Charles D. Orth; R. Patterson; Richard A. Sacks; R. Saunders; M. J. Shaw; M. Spaeth; S. Sutton; Wade H. Williams; C. Clay Widmayer; R. K. White; Pamela K. Whitman
A single beamline of the National Ignition Facility (NIF) has been operated at a wavelength of 526.5 nm (2 omega) by frequency converting the fundamental 1053 nm (1 omega) wavelength with an 18.2 mm thick type-I potassium dihydrogen phosphate (KDP) second-harmonic generator (SHG) crystal. Second-harmonic energies of up to 17.9 kJ were measured at the final optics focal plane with a conversion efficiency of 82%. For a similarly configured 192-beam NIF, this scales to a total 2 omega energy of 3.4 MJ full NIF equivalent (FNE).
Journal of Nonlinear Optical Physics & Materials | 1998
C. Clay Widmayer; Laurel R. Jones; David Milam
We report a measurement of the nonlinear refractive index coefficient, γ, of Carbon Disulfide (CS2), taken at a wavelength of 1.053 μm. The measurement uses a new technique based on the generation of high fluence holographic images of obscurations by self-focusing in the CS2. Near-field beam distortion measurements are used in conjunction with detailed wave propagation analysis. The approach is attractive because it utilizes a sensitive near-field fluence measurement, it is tolerant of intensity modulation in the measurement beam, and it is straightforward to model with the computer. A value of γ = (3.1 ± 0.3)×10-14cm2/W is obtained.
Journal of Physics: Conference Series | 2016
E L Dewald; R Tommasini; A Mackinnon; A MacPhee; N Meezan; R Olson; D Hicks; S LePape; N Izumi; K. B. Fournier; M A Barrios; S. Ross; A Pak; T Döppner; D. H. Kalantar; K Opachich; R Rygg; D Bradley; P Bell; A Hamza; B. Dzenitis; O. L. Landen; B. J. MacGowan; K. LaFortune; C. Clay Widmayer; B. Van Wonterghem; J Kilkenny; M J Edwards; J Atherton; E. I. Moses
Streaked 1-dimensional (slit imaging) radiography of 1.1 mm radius capsules in ignition hohlraums was recently introduced on the National Ignition Facility (NIF) and gives an inflight continuous record of capsule ablator implosion velocities, shell thickness and remaining mass in the last 3-5 ns before peak implosion time. The high quality data delivers good accuracy in implosion metrics that meets our requirements for ignition and agrees with recently introduced 2-dimensional pinhole radiography. Calculations match measured trajectory across various capsule designs and laser drives when the peak laser power is reduced by 20%. Furthermore, calculations matching measured trajectories give also good agreement in ablator shell thickness and remaining mass.