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Dive into the research topics where Thomas Lehecka is active.

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Featured researches published by Thomas Lehecka.


Physics of Plasmas | 1996

The Nike KrF laser facility: Performance and initial target experiments

S. P. Obenschain; Stephen E. Bodner; Denis G. Colombant; K. A. Gerber; R. H. Lehmberg; E. A. McLean; A. N. Mostovych; Mark S. Pronko; Carl J. Pawley; Andrew J. Schmitt; J. D. Sethian; V. Serlin; J. A. Stamper; C. A. Sullivan; Jill P. Dahlburg; John H. Gardner; Y.-L. Chan; A. V. Deniz; J. Hardgrove; Thomas Lehecka; M. Klapisch

Krypton‐fluoride (KrF) lasers are of interest to laser fusion because they have both the large bandwidth capability (≳THz) desired for rapid beam smoothing and the short laser wavelength (1/4 μm) needed for good laser–target coupling. Nike is a recently completed 56‐beam KrF laser and target facility at the Naval Research Laboratory. Because of its bandwidth of 1 THz FWHM (full width at half‐maximum), Nike produces more uniform focal distributions than any other high‐energy ultraviolet laser. Nike was designed to study the hydrodynamic instability of ablatively accelerated planar targets. First results show that Nike has spatially uniform ablation pressures (Δp/p<2%). Targets have been accelerated for distances sufficient to study hydrodynamic instability while maintaining good planarity. In this review we present the performance of the Nike laser in producing uniform illumination, and its performance in correspondingly uniform acceleration of targets.


Applied Optics | 1998

High-resolution monochromatic x-ray imaging system based on spherically bent crystals.

Y. Aglitskiy; Thomas Lehecka; Stephen Obenschain; Stephen E. Bodner; Carl Pawley; Kent Gerber; John Sethian; Charles M. Brown; John F. Seely; Uri Feldman; Glenn E. Holland

We have developed an improved x-ray imaging system based on spherically curved crystals. It is designed and used for diagnostics of targets ablatively accelerated by the Nike KrF laser. A spherically curved quartz crystal (d = .?, R = mm) has been used to produce monochromatic backlit images with the He-like Si resonance line (1865 eV) as the source of radiation. The spatial resolution of the x-ray optical system is 1.7 mum in selected places and 2-3 mum over a larger area. Time-resolved backlit monochromatic images of polystyrene planar targets driven by the Nike facility have been obtained with a spatial resolution of 2.5 mum in selected places and 5 mum over the focal spot of the Nike laser.


Physics of Plasmas | 1999

Observation of Rayleigh-Taylor Growth to Short Wavelengths on Nike

Carl J. Pawley; Stephen E. Bodner; Jill P. Dahlburg; S. P. Obenschain; Andrew J. Schmitt; J. D. Sethian; C. A. Sullivan; John H. Gardner; Y. Aglitskiy; Y.-L. Chan; Thomas Lehecka

The uniform and smooth focal profile of the Nike KrF laser [S. Obenschain et al., Phys. Plasmas 3, 2098 (1996)] was used to ablatively accelerate 40 μm thick polystyrene planar targets with pulse shaping to minimize shock heating of the compressed material. The foils had imposed small-amplitude sinusoidal wave perturbations of 60, 30, 20, and 12.5 μm wavelength. The shortest wavelength is near the ablative stabilization cutoff for Rayleigh–Taylor growth. Modification of the saturated wave structure due to random laser imprint was observed. Excellent agreement was found between the two-dimensional simulations and experimental data for most cases where the laser imprint was not dominant.


Physics of Plasmas | 1997

Measurements of laser-imprinted perturbations and Rayleigh–Taylor growth with the Nike KrF laser

Carl J. Pawley; K. A. Gerber; R. H. Lehmberg; E. A. McLean; A. N. Mostovych; S. P. Obenschain; J. D. Sethian; V. Serlin; J. A. Stamper; C. A. Sullivan; Stephen E. Bodner; Denis G. Colombant; Jill P. Dahlburg; Andrew J. Schmitt; John H. Gardner; C. M. Brown; John F. Seely; Thomas Lehecka; Y. Aglitskiy; A. V. Deniz; Y.-L. Chan; Nathan Metzler; M. Klapisch

Nike is a 56 beam Krypton Fluoride (KrF) laser system using Induced Spatial Incoherence (ISI) beam smoothing with a measured focal nonuniformity 〈ΔI/I〉 of 1% rms in a single beam [S. Obenschain et al., Phys. Plasmas 3, 1996 (2098)]. When 37 of these beams are overlapped on the target, we estimate that the beam nonuniformity is reduced by 37, to (ΔI/I)≅0.15% (excluding short-wavelength beam-to-beam interference). The extraordinary uniformity of the laser drive, along with a newly developed x-ray framing diagnostic, has provided a unique facility for the accurate measurements of Rayleigh–Taylor amplified laser-imprinted mass perturbations under conditions relevant to direct-drive laser fusion. Data from targets with smooth surfaces as well as those with impressed sine wave perturbations agree with our two-dimensional (2-D) radiation hydrodynamics code that includes the time-dependent ISI beam modulations. A 2-D simulation of a target with a 100 A rms randomly rough surface finish driven by a completely unif...


Review of Scientific Instruments | 1997

Large area electron beam pumped krypton fluoride laser amplifier

J. D. Sethian; S. P. Obenschain; K. A. Gerber; Carl J. Pawley; V. Serlin; C. A. Sullivan; W. Webster; A. V. Deniz; Thomas Lehecka; M. W. McGeoch; R. A. Altes; P. A. Corcoran; I. D. Smith; O. C. Barr

Nike is a recently completed multi-kilojoule krypton fluoride (KrF) laser that has been built to study the physics of direct drive inertial confinement fusion. This paper describes in detail both the pulsed power and optical performance of the largest amplifier in the Nike laser, the 60 cm amplifier. This is a double pass, double sided, electron beam-pumped system that amplifies the laser beam from an input of 50 J to an output of up to 5 kJ. It has an optical aperture of 60 cm × 60 cm and a gain length of 200 cm. The two electron beams are 60 cm high × 200 cm wide, have a voltage of 640 kV, a current of 540 kA, and a flat top power pulse duration of 250 ns. A 2 kG magnetic field is used to guide the beams and prevent self-pinching. Each electron beam is produced by its own Marx/pulse forming line system. The amplifier has been fully integrated into the Nike system and is used on a daily basis for laser-target experiments.


Optics Communications | 1995

Production of high energy, uniform focal profiles with the Nike laser

Thomas Lehecka; R. H. Lehmberg; A. V. Deniz; K. A. Gerber; Stephen P. Obenschain; Carl J. Pawley; Mark S. Pronko; C. A. Sullivan

Abstract Nike, a KrF laser facility at the Naval Research Laboratory, is designed to produce high intensity, ultra-uniform focal profiles for experiments relating to direct drive inertial confinement fusion. We present measurements of focal profiles through the next-to-last amplifier, a 20 × 20 cm 2 aperture electron beam pumped amplifier capable of producing more than 120 J of output in a 120 ns pulse. Using echelon free induced spatial incoherence beam smoothing this system has produced focal profiles with less than 2% tilt and curvature and less than 2% rms variation from a flat top distribution.


Review of Scientific Instruments | 1999

X-RAY CRYSTAL IMAGERS FOR INERTIAL CONFINEMENT FUSION EXPERIMENTS (INVITED)

Y. Aglitskiy; Thomas Lehecka; S. P. Obenschain; Carl J. Pawley; C. M. Brown; John F. Seely

We report on our continued development of high resolution monochromatic x-ray imaging system based on spherically curved crystals. This system can be extensively used in the relevant experiments of the inertial confinement fusion (ICF) program. The system is currently used, but not limited to diagnostics of the targets ablatively accelerated by the Nike KrF laser. A spherically curved quartz crystal (2d=6.687 03 A, R=200 mm) has been used to produce monochromatic backlit images with the He-like Si resonance line (1865 eV) as the source of radiation. Another quartz crystal (2d=8.5099 A, R=200 mm) with the H-like Mg resonance line (1473 eV) has been used for backlit imaging with higher contrast. The spatial resolution of the x-ray optical system is 1.7 μm in selected places and 2–3 μm over a larger area. A second crystal with a separate backlighter was added to the imaging system. This makes it possible to make use of all four strips of the framing camera. Time resolved, 20× magnified, backlit monochromatic...


Optics Communications | 1998

Comparison between measured and calculated nonuniformities of Nike laser beams smoothed by induced spatial incoherence

A. V. Deniz; Thomas Lehecka; R. H. Lehmberg; S. P. Obenschain

We have studied the spatial fluence nonuniformities in single beams from the Nike KrF laser smoothed by the Induced Spatial Incoherence (ISI) technique. This study compares time-integrated CCD camera measurements with a numerical model of ISI speckle used in the NRL FAST2D hydrocode, and with analytic calculations that examine the ensemble-average behavior of that model. The results verify the model and calculations, showing good agreement of both the spatial mode spectra and the total nonuniformity versus pulsewidth and bandwidth.


Physics of Plasmas | 1996

X‐ray emission from plasmas created by smoothed KrF laser irradiation

Y. Aglitskiy; Thomas Lehecka; A. V. Deniz; J. Hardgrove; John F. Seely; C. M. Brown; U. Feldman; Carl J. Pawley; K. A. Gerber; Stephen E. Bodner; S. P. Obenschain; R. H. Lehmberg; E. A. McLean; Mark S. Pronko; J. D. Sethian; J. A. Stamper; Andrew J. Schmitt; C. A. Sullivan; Glenn E. Holland; M. Laming

The x‐ray emission from plasmas created by the Naval Research Laboratory Nike KrF laser [Phys. Plasmas 3, 2098 (1996) ] was characterized using imaging and spectroscopic instruments. The laser wavelength was 1/4 μm, and the beams were smoothed by induced spatial incoherence (ISI). The targets were thin foils of CH, aluminum, titanium, and cobalt and were irradiated by laser energies in the range 100–1500 J. A multilayer mirror microscope operating at an energy of 95 eV recorded images of the plasma with a spatial resolution of 2 μm. The variation of the 95 eV emission across the 800 μm focal spot was 1.3% rms. Using a curved crystal imager operating in the 1–2 keV x‐ray region, the density, temperature, and opacity of aluminum plasmas were determined with a spatial resolution of 10 μm perpendicular to the target surface. The spectral line ratios indicated that the aluminum plasmas were relatively dense, cool, and optically thick near the target surface. The absolute radiation flux was determined at 95 eV ...


Review of Scientific Instruments | 1997

X-ray imaging of targets irradiated by the Nike KrF laser

C. M. Brown; John F. Seely; U. Feldman; S. P. Obenschain; Stephen E. Bodner; Carl J. Pawley; K. A. Gerber; V. Serlin; J. D. Sethian; Y. Aglitskiy; Thomas Lehecka; G. Holland

Foil targets irradiated by the Naval Research Laboratory Nike KrF laser were imaged in the x-ray region with two-dimensional spatial resolution in the 2–10 μm range. The images revealed the smoothness of the emission from target and backlighter foils, the acceleration of the target foils, and the growth of Rayleigh–Taylor instabilities that were seeded by patterns on the irradiated sides of CH foils.

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Carl J. Pawley

United States Naval Research Laboratory

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J. D. Sethian

United States Naval Research Laboratory

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K. A. Gerber

United States Naval Research Laboratory

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Stephen E. Bodner

Lawrence Livermore National Laboratory

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S. P. Obenschain

United States Naval Research Laboratory

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Stephen P. Obenschain

United States Naval Research Laboratory

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V. Serlin

United States Naval Research Laboratory

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John F. Seely

Science Applications International Corporation

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Y. Aglitskiy

Science Applications International Corporation

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John H. Gardner

United States Naval Research Laboratory

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