Thaddeus J. Orzechowski
Lawrence Livermore National Laboratory
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Featured researches published by Thaddeus J. Orzechowski.
Journal of Applied Physics | 1996
R. C. Spitzer; Thaddeus J. Orzechowski; D. W. Phillion; R. L. Kauffman; C. Cerjan
The conversion efficiency of spectral emission from laser‐irradiated solid targets was investigated for short wavelength source development. The plasma brightness was quantified using absolutely calibrated detectors for 20 materials and spectra were obtained between 50 and 200 A. Laser parameters such as wavelength, pulse length, intensity, and spot size were systematically varied to establish a comprehensive database for source optimization. Qualitative differences in the underlying dominant emission features as a function of atomic number and laser wavelength were observed that accounted for the relatively high spectral conversion efficiencies produced. In the specific case of Sn, a conversion efficiency greater than 0.8%/eV has been observed in the technologically important region of λ=134.0 A using a laser intensity of 1–2×1011 W/cm2.
Physics of Plasmas | 1996
L. J. Suter; R. L. Kauffman; C. B. Darrow; A. A. Hauer; H. N. Kornblum; O. L. Landen; Thaddeus J. Orzechowski; D. W. Phillion; J. L. Porter; L. V. Powers; A. Richard; M. D. Rosen; A. R. Thiessen; R. J. Wallace
Nearly 10 years of Nova [E. M. Campbell, Laser Part. Beams 9, 209 (1991)] experiments and analysis have lead to a relatively detailed quantitative and qualitative understanding of radiation drive in laser‐heated hohlraums. Our most successful quantitative modeling tool is two‐dimensional (2‐D) LASNEX numerical simulations [G. B. Zimmerman and W. L. Kruer, Comments Plasma Phys. Controlled Fusion 2, 51 (1975)]. Analysis of the simulations provides us with insight into the physics of hohlraum drive. In particular we find hohlraum radiation conversion efficiency becomes quite high with longer pulses as the accumulated, high‐Z blow‐off plasma begins to radiate. Extensive Nova experiments corroborate our quantitative and qualitative understanding.
Physics of Plasmas | 1998
R. L. Kauffman; L. V. Powers; S. Dixit; S. G. Glendinning; S. H. Glenzer; R. K. Kirkwood; O. L. Landen; B. J. MacGowan; John Moody; Thaddeus J. Orzechowski; Deanna M. Pennington; G. F. Stone; L. J. Suter; R. E. Turner; T. L. Weiland; A.L. Richard; M. A. Blain
Gas-filled hohlraums are presently the base line ignition target design for the National Ignition Facility. Initial Nova [E. M. Campbell et al. Rev. Sci. Instrum. 57, 2101 (1986).] experiments on gas-filled hohlraums showed that radiation temperature was reduced due to stimulated Brillouin and stimulated Raman scattering losses and that implosion symmetry had shifted compared with vacuum hohlraums and calculations. Subsequent single beam experiments imaging thermal x-ray emission showed the shift is due to laser–plasma heating dynamics and filamentation in a flowing plasma. Experiments using a single beam have shown that scattering losses and effects of filamentation are reduced when the beam is spatially smoothed with a random phase plate or kinoform phase plate. Scattering is further reduced to less than 5% of the incident laser energy when temporal smoothing is added.
Physics of Plasmas | 1997
R. E. Olson; John L. Porter; Gordon Andrew Chandler; D. L. Fehl; D. O. Jobe; R. J. Leeper; M. K. Matzen; J. McGurn; D. D. Noack; Laurence E. Ruggles; P. Sawyer; J. Torres; M. Vargas; D. M. Zagar; H. N. Kornblum; Thaddeus J. Orzechowski; D. W. Phillion; L. J. Suter; A. R. Thiessen; R. J. Wallace
The Saturn pulsed power accelerator [R. B. Spielman et al., in Proceedings of the 2nd International Conference on Dense Z-pinches, Laguna Beach, CA, 1989, edited by N. R. Pereira, J. Davis, and N. Rostoker (American Institute of Physics, New York, 1989), p. 3] at Sandia National Laboratories (SNL) and the Nova laser [J. T. Hunt and D. R. Speck, Opt. Eng. 28, 461 (1989)] at Lawrence Livermore National Laboratory (LLNL) have been used to explore techniques for studying the behavior of ablator material in x-ray radiation environments comparable in magnitude, spectrum, and duration to those that would be experienced in National Ignition Facility (NIF) hohlraums [J. D. Lindl, Phys. Plasmas 2, 3933 (1995)]. The large x-ray outputs available from the Saturn pulsed-power-driven z pinch have enabled us to drive hohlraums of full NIF ignition scale size at radiation temperatures and time scales comparable to those required for the low-power foot pulse of an ignition capsule. The high-intensity drives available in t...
Plasma Physics and Controlled Fusion | 1999
W. L. Kruer; E M Campbell; C D Decker; S. C. Wilks; J. D. Moody; Thaddeus J. Orzechowski; L. V. Powers; L. J. Suter; B B Afeyan; N Dague
An improved understanding of strongly driven laser-plasma coupling is important for optimal use of the National Ignition Facility (NIF) for both inertial fusion and for a variety of advanced applications. Such applications range from high-energy x-ray sources and high-temperature hohlraums to fast ignition and laser radiography. We discuss a novel model for the scaling of strongly driven stimulated Brillouin and Raman scattering. This model postulates an intensity-dependent correlation length associated with spatial incoherence due to filamentation and stimulated forward scattering. We first describe the model and then relate it to a variety of experiments. Particular attention is paid to high-temperature hohlraum experiments, which exhibit low to modest stimulated Brillouin scattering even though this instability is strongly driven. We also briefly discuss the strongly nonlinear interaction physics for efficient generation of high-energy electrons either by irradiating a large plasma with near quarter-critical density or by irradiating overdense targets with ultra-intense laser light.
22nd International Congress on High-Speed Photography and Photonics | 1997
D. H. Kalantar; P. M. Bell; R. Costa; B. A. Hammel; O. L. Landen; Thaddeus J. Orzechowski; Jonathan D. Hares; Anthony K. L. Dymoke-Bradshaw
There are many different types of measurements that require a continuous time history of x-ray emission that can be provided with an x-ray streak camera. In order to properly analyze the images that are recorded with the x-ray streak cameras operated on Nova, it is important to account for the streak characterization of each camera. We have performed a number of calibrations of the streak camera both on the bench as well as with Nova disk target shots where we use a time modulated laser intensity profile (self-beating of the laser) on the target to generate an x-ray comb. We have measured the streak camera sweep direction and spatial offset, curvature of the electron optics, sweep rate, and magnification and resolution of the electron optics.
The tenth American Physical Society topical conference on atomic processes in plasmas | 2008
Thaddeus J. Orzechowski; M. D. Rosen; H. N. Kornblum; J. L. Porter; L. J. Suter; A. R. Thiessen; R. J. Wallace
The Rosseland mean opacity can be used to describe radiation transport through high‐opacity materials. This mean opacity is dominated by the minima in the frequency‐dependent opacity. By mixing appropriate materials, we can fill in the low opacity regions of one material with the high opacity regions of another material, resulting in a material with a Rosseland mean opacity higher than either of the constituents. This composite material can be used to improve the energy balance in indirect‐drive inertial confinement fusion. For a given laser energy, this can raise the temperature of the laser heated hohlraum, or for a given desired temperature, require less laser energy.
Laser interaction and related plasma phenomena: 12th international conference | 2008
Thaddeus J. Orzechowski; R. L. Kauffman; R. K. Kirkwood; H. N. Kornblum; W. K. Levedahl; D. S. Montgomery; L. V. Powers; T. D. Shepard; G. F. Stone; L. J. Suter; R. J. Wallace; J. M. Foster; P. Rosen
In order to prevent high‐Z plasma from filling in the hohlraum in indirect drive experiments, a low‐Z material, or tamper is introduced into the hohlraum. This material, when fully ionized is typically less than one‐tenth of the critical density for the laser light used to illuminate the hohlraum. This tamper absorbs little of the laser light, thus allowing most of the laser energy to be absorbed in the high‐Z material. However, the pressure associated with this tamper is sufficient to keep the hohlraum wall material from moving a significant distance into the interior of the hohlraum. In this paper we discuss measurements of the motion of the interface between the tamper and the high‐Z hohlraum material. We also present measurements of the effect the tamper has on the hohlraum temperature.
Quantitative Nondestructive Evaluation | 2002
Maurice B. Aufderheide; Thaddeus J. Orzechowski; John D. Molitoris; Anne J. Sunwoo; Charles F. Cook; Ernie Urquidez; Gurcharn S. Dhillon; Jeffrey B. Chandler; Martin R. de Haven; Gary E. Steinhour; Dale M. Slone; Alexis E. Schach von Wittenau; Jessie Jackson; Harry E. Martz; Dennis M. Goodman
The failure of a steel pipe subjected to shock loading was observed using x ray imaging. We describe and analyze the x ray images in detail. We see radiographic evidence that most of the fractures were due to shear rather than brittle failure. We also make quantitative comparisons between static radiographs and simulations but do not see perfect agreement. The sources of the current lack of agreement are discussed, as well as future work planned.
Physical Review Letters | 1996
Thaddeus J. Orzechowski; Rosen; H. N. Kornblum; J. L. Porter; L. J. Suter; A. R. Thiessen; R. J. Wallace